List of Variables
The table below contains a list of variables that are used in the code and that are available for plotting / analysis.
Name : Name of the variable as it appears in the code. Pass a string with this name to any of the plotting functions to plot, or to the relevant
.compute()method to return the calculated quantity.Label : TeX label for the variable.
Units : Physical units for the variable.
Description : Description of the variable.
Aliases : Alternative names of the variable that are equivalent to the primary name.
kwargs : Optional keyword arguments that can be supplied when computing the variable. See the bottom of this page for detailed descriptions and default values of each argument. The only keyword argument that is valid for all variables is ‘basis’ (see explanation below).
All vector quantities are computed in toroidal coordinates \((R,\phi,Z)\) by default.
The keyword argument basis='xyz' can be used to convert the variables into Cartesian
coordinates \((X,Y,Z)\). basis must be one of {'rpz', 'xyz'}.
Our convention to denote partial derivatives is an underscore followed by the first
letter of the coordinate that the partial derivative is taken with respect to. Unless
otherwise specified or implied by the variable name, these partial derivatives are
those of the DESC \(\rho, \theta, \zeta\) coordinate system. For example, |B|_z
is \((\partial \vert B \vert / \partial\zeta)|_{\rho, \theta}\).
Many quantities require special grids to compute accurately.
To not burden users with such bookkeeping,
when an object method such as eq.compute(...,override_grid=True) is called,
DESC will automatically use a set of best grids for the computation.
However, when writing objectives developers must perform the bookkeeping
and ensure everything can be computed accurately on the chosen grid.
desc.equilibrium.equilibrium.Equilibrium
Name |
Label |
Units |
Description |
Aliases |
kwargs |
|---|---|---|---|---|---|
|
\(((\mathbf{B} \cdot \nabla) \mathbf{B})_{\rho}\) |
Tesla squared |
Covariant radial component of magnetic tension |
||
|
\(((\mathbf{B} \cdot \nabla) \mathbf{B})_{\theta}\) |
Tesla squared |
Covariant poloidal component of magnetic tension |
||
|
\(((\mathbf{B} \cdot \nabla) \mathbf{B})_{\zeta}\) |
Tesla squared |
Covariant toroidal component of magnetic tension |
||
|
\(\partial_{\theta} (\mathbf{B} \cdot \nabla B)\) |
Tesla squared / meters |
|||
|
\(\partial_{\theta} (\mathbf{B} \cdot \nabla B)\) |
Tesla squared / meters |
|||
|
\(\partial_{\zeta} (\mathbf{B} \cdot \nabla B)\) |
Tesla squared / meters |
|||
|
\(\nabla(\nabla(\rho))\) |
Tesla over square meters |
Gradient of contravariant radial basis vector(grad rho)along the magnetic field scaled by the magnetic field strength |
||
|
\((\mathbf{B} \cdot \nabla) \mathbf{B}\) |
Tesla squared / meters |
Magnetic tension |
||
|
\(\partial_{\rho} (\mathbf{J} \sqrt{g})\) |
Ampere meters |
Plasma current density weighted by 3-D volume Jacobian, radial derivative |
||
|
\(\partial_{\phi}|_{\rho, \vartheta} J^{\vartheta}\) |
Amperes / cubic meter |
Contravariant PEST poloidal component of plasma current density derivative w.r.t toroidal coordinate |
|
|
|
\(\partial_{\vartheta}|_{\rho, \phi} J^{\vartheta}\) |
Amperes / cubic meter |
Contravariant PEST poloidal component of plasma current density derivative w.r.t poloidal PEST coordinate |
|
|
|
\(\partial_{\phi}|_{\rho, \phi} J^{\zeta}\) |
Amperes / cubic meter |
Contravariant PEST toroidal component of plasma current density derivative w.r.t toroidal cylindrical coordinate |
||
|
\(\partial_{\vartheta}|_{\rho, \phi} J^{\zeta}\) |
Amperes / cubic meter |
Contravariant PEST toroidal component of plasma current density derivative w.r.t poloidal PEST coordinate |
||
|
\(((\nabla \times \mathbf{B}) \times \mathbf{B})_{\rho}\) |
Tesla squared |
Covariant radial component of Lorentz force |
||
|
\(((\nabla \times \mathbf{B}) \times \mathbf{B})_{\theta}\) |
Tesla squared |
Covariant poloidal component of Lorentz force |
||
|
\(((\nabla \times \mathbf{B}) \times \mathbf{B})_{\zeta}\) |
Tesla squared |
Covariant toroidal component of Lorentz force |
||
|
\(\partial_{\phi}|_{\vartheta, \rho} \mathbf{e}^{\rho}\) |
inverse meters |
Contravariant radial basis vector derivative w.r.t the cylindrical toroidal angle. |
||
|
\(\partial_{\vartheta}|_{\rho, \phi} \mathbf{e}^{\rho}\) |
inverse meters |
Contravariant radial basis vector derivative w.r.t the poloidal PEST coordinate. |
||
|
\(\partial_{\phi}\lvert_{\rho, \vartheta}(\mathbf{e}^{\vartheta})\) |
inverse meters |
Contravariant poloidal PEST basis vector, derivative wrt cylindrical toroidal coordinate ϕ. |
|
|
|
\(\partial_{\vartheta}|_{\rho, \phi} \mathbf{e}^{\vartheta}\) |
inverse meters |
Contravariant poloidal PEST basis vector derivative wrt theta poloidal PEST coordinate ϑ. |
|
|
|
\(\partial_{\phi}|_{\rho,\vartheta} \mathbf{e}^{\zeta}\) |
inverse meters |
Contravariant toroidal basis vector, derivative wrt cylindrical toroidal coordinate phi at constant rho and vartheta |
||
|
\(\partial_{\vartheta}_{\rho,\phi} \mathbf{e}^{\zeta}\) |
inverse meters |
Contravariant toroidal basis vector, derivative wrt theta poloidal PEST coordinate |
||
|
\((\partial_{\phi} |_{\rho, \vartheta} \mathbf{e}_{\phi}) |_{\rho, \vartheta}\) |
meters |
Derivative of the covariant toroidal basis vector instraight field line PEST coordinates (ρ,ϑ,ϕ) w.r.t the cylindricaltoroidal angle. |
||
|
\(\partial_{\rho} |_{\phi, \vartheta} (\mathbf{e}_{\phi} |_{\rho, \vartheta})\) |
meters |
Derivative of the covariant toroidal basis vector instraight field line PEST coordinates (ρ,ϑ,ϕ) w.r.t rho.ϕ increases counterclockwise when viewed from above(cylindrical R,ϕ plane with Z out of page). |
|
|
|
\(\partial_{\rho} |_{\phi, \vartheta} (\mathbf{e}_{\rho} |_{\phi, \vartheta})\) |
meters |
Derivative of the covariant radial basis vector instraight field line PEST coordinates (ρ,ϑ,ϕ) w.r.t rho.ϕ increases counterclockwise when viewed from above(cylindrical R,ϕ plane with Z out of page). |
||
|
\((\partial_{\phi} |_{\rho, \vartheta} (\mathbf{e}_{\vartheta}|_{\rho, \phi}))\) |
meters |
Derivative of the covariant poloidal basis vector instraight field line PEST coordinates (ρ,ϑ,ϕ) w.r.t the cylindricaltoroidal angle. ϕ increases counterclockwise when viewed from above(cylindrical R,ϕ plane with Z out of page). |
|
|
|
\((\partial_{\rho} |_{\phi, \vartheta} \mathbf{e}_{\vartheta}) |_{\rho, \phi}\) |
meters |
Derivative of the covariant poloidal PEST basis vector instraight field line PEST coordinates (ρ,ϑ,ϕ) w.r.t rho. |
|
|
|
\((\partial_{\vartheta}|_{\rho, \phi}(\mathbf{e}_{\vartheta})|_{\rho \phi})\) |
meters |
Derivative of the covariant poloidal basis vector instraight field line PEST coordinates (ρ,ϑ,ϕ) w.r.t straight fieldline PEST theta coordinate. ϕ increases counterclockwise when viewed above(cylindrical R,ϕ plane with Z out of page). |
|
|
|
\(\partial_{\alpha} (\mathbf{e}_{\zeta} |_{\rho, \alpha})\) |
meters |
Tangent vector along (collinear to) field line, derivative wrt field line poloidal label |
||
|
\(\partial_{\theta} (\mathbf{e}_{\zeta} |_{\rho, \alpha})\) |
meters |
Tangent vector along (collinear to) field line, derivative wrt DESC poloidal angle |
||
|
\(\partial_{\zeta} (\mathbf{e}_{\zeta} |_{\rho, \alpha})\) |
meters |
Tangent vector along (collinear to) field line, derivative wrt DESC toroidal angle at fixed ρ,θ. |
||
|
\(\partial_{\zeta} (\mathbf{e}_{\zeta} |_{\rho, \alpha}) |_{\rho, \alpha}\) |
meters |
Curvature vector along field line |
||
|
\(\partial_{\phi}|_{\rho, \vartheta} g^{\rho\rho}|PEST\) |
inverse square meters |
Radial-Radial element of contravariant metric tensor in PEST coordinates, derivative w.r.t toroidal cylindrical coordinate |
||
|
\(\partial_{\vartheta}|_{\rho, \phi} g^{\rho\rho}|PEST\) |
inverse square meters |
Radial-Radial element of contravariant metric tensor in PEST coordinates, derivative w.r.t poloidal PEST coordinate |
||
|
\(\partial_{\phi}|_{\rho, \vartheta} g^{\rho\vartheta}|PEST\) |
inverse square meters |
Radial-Poloidal element of contravariant metric tensor in PEST coordinates, derivative w.r.t toroidal cylidrical coordinate |
||
|
\(\partial_{\vartheta}|_{\rho, \phi} g^{\rho\vartheta}|PEST\) |
inverse square meters |
Radial-Poloidal element of contrvariant metric tensor in PEST coordinates, derivative w.r.t poloidal PEST coordinate |
||
|
\(\partial_{\phi}|_{\rho, \vartheta} g^{\rho\zeta}|PEST\) |
inverse square meters |
Radial-Toroidal element of contravariant metric tensor in PEST coordinates, derivative w.r.t toroidal cylindrical coordinate |
||
|
\(\partial_{\vartheta}|_{\rho, \phi} g^{\rho\zeta}|PEST\) |
inverse square meters |
Radial-Toroidal element of contrvariant metric tensor in PEST coordinates, derivative w.r.t polodal PEST coordinate |
||
|
\(\partial_{\theta_PEST}|_{\rho, \phi} g_{\phi\phi}|PEST\) |
square meters |
Toroidal-Toroidal element of covariant metric tensor in PEST coordinates, derivative w.r.t poloidal PEST coordinate |
||
|
\(\partial_{\phi}|_{\rho, \vartheta} g_{\rho\rho}|PEST\) |
square meters |
Radial-Radial element of covariant metric tensor in PEST coordinates, derivative w.r.t toroidal cylindrical coordinate |
||
|
\(\partial_{\theta_PEST}|_{\rho, \phi} g_{\rho\rho}|PEST\) |
square meters |
Radial-Radial element of covariant metric tensor in PEST coordinates, derivative w.r.t poloidal PEST coordinate |
||
|
\(a\partial_{\phi}|_{\rho, \vartheta} g_{\rho\vartheta}|PEST\) |
square meters |
Radial-Poloidal element of covariant metric tensor in PEST coordinates, derivative w.r.t toroidal cylindrical coordinate |
||
|
\(\partial_{\phi}|_{\rho, \vartheta} g_{\vartheta\vartheta}|PEST\) |
square meters |
Poloidal-Poloidal element of covariant metric tensor in PEST coordinates, derivative w.r.t toroidal cylindrical coordinate |
||
|
\(\partial_{\rho}|_{\phi, \vartheta} g_{\vartheta \vartheta}|PEST\) |
square meters |
Poloidal-Poloidal element of covariant metric tensor in PEST coordinates, derivative w.r.t radial coordinate |
||
|
\(\partial_{\rho} (\psi' / \sqrt{g})\) |
Tesla / meter |
|||
|
\(\partial_{\rho \rho} (\psi' / \sqrt{g})\) |
Tesla / meters |
|||
|
\(\partial_{\rho\theta} (\psi' / \sqrt{g})\) |
Tesla / meters |
|
||
|
\(\partial_{\rho\zeta} (\psi' / \sqrt{g})\) |
Tesla / meters |
|
||
|
\(\partial_{\theta} (\psi' / \sqrt{g})\) |
Tesla / meter |
|||
|
\(\partial_{\theta \theta} (\psi' / \sqrt{g})\) |
Tesla / meter |
|||
|
\(\partial_{\theta\zeta} (\psi' / \sqrt{g})\) |
Tesla / meter |
|
||
|
\(\partial_{\zeta} (\psi' / \sqrt{g})\) |
Tesla / meter |
|||
|
\(\partial_{\zeta \zeta} (\psi' / \sqrt{g})\) |
Tesla / meter |
|||
|
\(\partial_{\phi}|_{\rho, \vartheta} \sqrt{g}_PEST\) |
cubic meters |
Jacobian determinant of PEST coordinate system derivative w.r.t cylindrical toroidal angle |
||
|
\(\partial_{\rho}|_{\phi, \vartheta} \sqrt{g}_PEST\) |
cubic meters |
Jacobian determinant of PEST coordinate system derivative w.r.t radial coordinate rho |
||
|
\(\partial_{\vartheta}|_{\rho, \phi} \sqrt{g}_PEST\) |
cubic meters |
Jacobian determinant of PEST coordinate system derivative w.r.t PEST poloidal angle |
||
|
\(0\) |
None |
Zeros |
|
|
|
\(1\) |
None |
Ones |
|
|
|
\(\langle 1/|B| \rangle\) |
1 / Tesla |
Flux surface averaged inverse field strength |
||
|
\(\langle \mathbf{J} \cdot \mathbf{B} \rangle\) |
Newtons / cubic meter |
Flux surface average of current density dotted into magnetic field (note units are not Amperes) |
||
|
\(\langle\mathbf{J}\cdot\mathbf{B}\rangle_{Redl}\) |
Tesla Ampere / meter^2 |
Bootstrap current profile, Redl model for quasisymmetry |
|
|
|
\(\langle \beta \rangle_{vol}\) |
None |
Normalized plasma pressure |
||
|
\(\langle \beta_{pol} \rangle_{vol}\) |
None |
Normalized poloidal plasma pressure |
||
|
\(\langle \beta_{tor} \rangle_{vol}\) |
None |
Normalized toroidal plasma pressure |
||
|
\(\langle n_e \rangle_{vol}\) |
1 / cubic meters |
Volume average electron density |
||
|
\(\langle\sigma\nu\rangle\) |
cubic meters / second |
Thermal reactivity from Bosch-Hale parameterization |
|
|
|
\(\langle |(\mathbf{B} \cdot \nabla) \mathbf{B}| \rangle_{vol}\) |
Tesla squared / meters |
Volume average magnetic tension magnitude |
||
|
\(\langle |B| \rangle\) |
Tesla |
Flux surface average magnetic field |
||
|
\(\langle |\mathbf{B}| \rangle_{axis}\) |
Tesla |
Average magnitude of magnetic field on the innermost flux surface on the given grid |
||
|
\(\langle |B| \rangle_{rms}\) |
Tesla |
Volume average magnetic field, root mean square |
||
|
\(\langle |B| \rangle_{vol}\) |
Tesla |
Volume average magnetic field |
||
|
\(\langle |B|^2 \rangle\) |
Tesla squared |
Flux surface average magnetic field squared |
||
|
\(\partial_{\rho} \langle |B|^2 \rangle\) |
Tesla squared |
Flux surface average magnetic field squared, radial derivative |
||
|
\(\langle |\mathbf{J} \times \mathbf{B} - \nabla p| \rangle_{vol}\) |
Newtons / cubic meter |
Volume average of magnitude of force balance error |
||
|
\(\langle |\nabla p| \rangle_{vol}\) |
Newtons per cubic meter |
Volume average of magnitude of pressure gradient |
||
|
\(\langle \vert \nabla \rho \vert \rangle\) |
inverse meters |
Magnitude of contravariant radial basis vector, flux surface average |
||
|
\(\langle |\nabla |B|^{2}/(2\mu_0)| \rangle_{vol}\) |
Newtons per cubic meter |
Volume average of magnitude of magnetic pressure gradient |
||
|
\(A\) |
square meters |
Average enclosed cross-sectional (constant zeta surface) area, extrapolated to last closed flux surface |
||
|
\(A(\rho)\) |
square meters |
Average area of enclosed cross-section (enclosed constant zeta surface), as function of rho |
||
|
\(A(\zeta)\) |
square meters |
Area of enclosed cross-section (enclosed constant zeta surface), extrapolated to last closed flux surface |
||
|
\(\mathbf{B}\) |
Tesla |
Magnetic field |
||
|
\(\mathrm{Boozer~modes}\) |
None |
Boozer harmonics |
|
|
|
\(\mathbf{B} \cdot \nabla B\) |
Tesla squared / meters |
|||
|
\(B^{\phi}\) |
Tesla / meter |
Contravariant cylindrical toroidal angle component of magnetic field |
||
|
\(\partial_{\phi} B^{\phi} |_{\rho, \vartheta}\) |
Tesla / meter |
Contravariant cylindrical toroidal angle component of magnetic field, partial derivative wrt ϕ in (ρ, ϑ, ϕ) coordinates. |
||
|
\(\partial_{\rho} B^{\phi} |_{\theta, \zeta}\) |
Tesla / meter |
Contravariant cylindrical toroidal angle component of magnetic field, partial derivative wrt ρ in (ρ, θ, ζ) coordinates. |
||
|
\(\partial_{\rho}|_{\vartheta, \phi} B^{\phi}\) |
Tesla / meter |
Contravariant cylindrical toroidal angle component of magnetic field, partial derivative wrt ρ in (ρ, ϑ, ϕ) coordinates. |
||
|
\(\partial_{\theta} B^{\phi} |_{\rho, \zeta}\) |
Tesla / meter |
Contravariant cylindrical toroidal angle component of magnetic field, partial derivative wrt θ in (ρ, θ, ζ) coordinates. |
||
|
\(\partial_{\vartheta} B^{\phi} |_{\rho, \phi}\) |
Tesla / meter |
Contravariant cylindrical toroidal angle component of magnetic field, partial derivative wrt ϑ in (ρ, ϑ, ϕ) coordinates. |
||
|
\(\partial_{\zeta} B^{\phi} |_{\rho, \theta}\) |
Tesla / meter |
Contravariant cylindrical toroidal angle component of magnetic field, partial derivative wrt ζ in (ρ, θ, ζ) coordinates. |
||
|
\(B^{\rho}\) |
Tesla / meter |
Contravariant radial component of magnetic field |
||
|
\(B^{\theta}\) |
Tesla / meter |
Contravariant poloidal component of magnetic field |
||
|
\(\partial_{\rho} B^{\theta}\) |
Tesla / meter |
Contravariant poloidal component of magnetic field, derivative wrt radial coordinate |
||
|
\(\partial_{\rho\rho} B^{\theta}\) |
Tesla / meter |
Contravariant poloidal component of magnetic field, second derivative wrt radial and radial coordinates |
||
|
\(\partial_{\rho\theta} B^{\theta}\) |
Tesla / meter |
Contravariant poloidal component of magnetic field, second derivative wrt radial and poloidal coordinates |
|
|
|
\(\partial_{\rho\zeta} B^{\theta}\) |
Tesla / meter |
Contravariant poloidal component of magnetic field, second derivative wrt radial and toroidal coordinates |
|
|
|
\(\partial_{\theta} B^{\theta}\) |
Tesla / meter |
Contravariant poloidal component of magnetic field, derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta\theta} B^{\theta}\) |
Tesla / meter |
Contravariant poloidal component of magnetic field, second derivative wrt poloidal and poloidal coordinates |
||
|
\(\partial_{\theta\zeta} B^{\theta}\) |
Tesla / meter |
Contravariant poloidal component of magnetic field, second derivative wrt poloidal and toroidal coordinates |
|
|
|
\(\partial_{\zeta} B^{\theta}\) |
Tesla / meter |
Contravariant poloidal component of magnetic field, derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta\zeta} B^{\theta}\) |
Tesla / meter |
Contravariant poloidal component of magnetic field, second derivative wrt toroidal and toroidal coordinates |
||
|
\(B^{\zeta}\) |
Tesla / meter |
Contravariant toroidal component of magnetic field |
||
|
\(\partial_{\alpha} B^{\zeta}\) |
Tesla / meter |
Contravariant toroidal component of magnetic field, derivative wrt field line poloidal label |
||
|
\(\partial_{\rho} B^{\zeta}\) |
Tesla / meter |
Contravariant toroidal component of magnetic field, derivative wrt radial coordinate |
||
|
\(\partial_{\rho\rho} B^{\zeta}\) |
Tesla / meter |
Contravariant toroidal component of magnetic field, second derivative wrt radial and radial coordinates |
||
|
\(\partial_{\rho\theta} B^{\zeta}\) |
Tesla / meter |
Contravariant toroidal component of magnetic field, second derivative wrt radial and poloidal coordinates |
|
|
|
\(\partial_{\rho\zeta} B^{\zeta}\) |
Tesla / meter |
Contravariant toroidal component of magnetic field, second derivative wrt radial and toroidal coordinates |
|
|
|
\(\partial_{\theta} B^{\zeta}\) |
Tesla / meter |
Contravariant toroidal component of magnetic field, derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta\theta} B^{\zeta}\) |
Tesla / meter |
Contravariant toroidal component of magnetic field, second derivative wrt poloidal and poloidal coordinates |
||
|
\(\partial_{\theta\zeta} B^{\zeta}\) |
Tesla / meter |
Contravariant toroidal component of magnetic field, second derivative wrt poloidal and toroidal coordinates |
|
|
|
\(\partial_{\zeta} B^{\zeta}\) |
Tesla / meter |
Contravariant toroidal component of magnetic field, derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta\zeta} B^{\zeta}\) |
Tesla / meter |
Contravariant toroidal component of magnetic field, second derivative wrt toroidal and toroidal coordinates |
||
|
\(\partial_{\zeta} B^{\zeta} |_{\rho, \alpha}\) |
Tesla / meter |
Contravariant toroidal component of magnetic field, derivative along field line |
||
|
\(B_{R} = \mathbf{B} \cdot \hat{R}\) |
Tesla |
Radial component of magnetic field in lab frame |
||
|
\(B_{Z} = \mathbf{B} \cdot \hat{Z}\) |
Tesla |
Vertical component of magnetic field in lab frame |
||
|
\(B_{\phi} = \mathbf{B} \cdot \hat{\phi} = \mathbf{B} \cdot R^{-1} \mathbf{e}_{\phi} |_{R, Z}\) |
Tesla |
Toroidal component of magnetic field in lab frame |
||
|
\(B_{\phi, m, n}\) |
Tesla * meters |
Fourier coefficients for covariant toroidal component of magnetic field in (ρ,θ,ϕ) coordinates. |
|
|
|
\(B_{\phi} = B \cdot \mathbf{e}_{\phi} |_{\rho, \theta}\) |
Tesla * meters |
Covariant toroidal component of magnetic field in (ρ,θ,ϕ) coordinates. |
||
|
\(\partial_{\rho} \mathbf{B}\) |
Tesla |
Magnetic field, derivative wrt radial coordinate |
||
|
\(B_{\rho}\) |
Tesla * meters |
Covariant radial component of magnetic field |
||
|
\(\partial_{\rho} B_{\rho}\) |
Tesla * meters |
Covariant radial component of magnetic field, derivative wrt radial coordinate |
||
|
\(\partial_{\rho\rho} B_{\rho}\) |
Tesla * meters |
Covariant radial component of magnetic field, second derivative wrt radial coordinate |
||
|
\(\partial_{\rho\theta} B_{\rho}\) |
Tesla * meters |
Covariant radial component of magnetic field, second derivative wrt radial coordinate and poloidal angle |
|
|
|
\(\partial_{\rho\zeta} B_{\rho}\) |
Tesla * meters |
Covariant radial component of magnetic field, second derivative wrt radial coordinate and toroidal angle |
|
|
|
\(\partial_{\theta} B_{\rho}\) |
Tesla * meters |
Covariant radial component of magnetic field, derivative wrt poloidal angle |
||
|
\(\partial_{\theta\theta} B_{\rho}\) |
Tesla * meters |
Covariant radial component of magnetic field, second derivative wrt poloidal angle |
||
|
\(\partial_{\theta\zeta} B_{\rho}\) |
Tesla * meters |
Covariant radial component of magnetic field, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\zeta} B_{\rho}\) |
Tesla * meters |
Covariant radial component of magnetic field, derivative wrt toroidal angle |
||
|
\(\partial_{\zeta\zeta} B_{\rho}\) |
Tesla * meters |
Covariant radial component of magnetic field, second derivative wrt toroidal angle |
||
|
\(\partial_{\rho\rho} \mathbf{B}\) |
Tesla |
Magnetic field, second derivative wrt radial coordinate |
||
|
\(\partial_{\rho\theta} \mathbf{B}\) |
Tesla |
Magnetic field, second derivative wrt radial coordinate and poloidal angle |
|
|
|
\(\partial_{\rho\zeta} \mathbf{B}\) |
Tesla |
Magnetic field, second derivative wrt radial coordinate and toroidal angle |
|
|
|
\(\partial_{\theta} \mathbf{B}\) |
Tesla |
Magnetic field, derivative wrt poloidal angle |
||
|
\(B_{\theta}\) |
Tesla * meters |
Covariant poloidal component of magnetic field |
||
|
\(B_{\theta, m, n}\) |
Tesla * meters |
Fourier coefficients for covariant poloidal component of magnetic field. |
|
|
|
\(\partial_{\rho} B_{\theta}\) |
Tesla * meters |
Covariant poloidal component of magnetic field, derivative wrt radial coordinate |
||
|
\(\partial_{\rho\rho} B_{\theta}\) |
Tesla * meters |
Covariant poloidal component of magnetic field, second derivative wrt radial coordinate |
||
|
\(\partial_{\rho\theta} B_{\theta}\) |
Tesla * meters |
Covariant poloidal component of magnetic field, second derivative wrt radial coordinate and poloidal angle |
|
|
|
\(\partial_{\rho\zeta} B_{\theta}\) |
Tesla * meters |
Covariant poloidal component of magnetic field, second derivative wrt radial coordinate and toroidal angle |
|
|
|
\(\partial_{\theta} B_{\theta}\) |
Tesla * meters |
Covariant poloidal component of magnetic field, derivative wrt poloidal angle |
||
|
\(\partial_{\theta\theta} B_{\theta}\) |
Tesla * meters |
Covariant poloidal component of magnetic field, second derivative wrt poloidal angle |
||
|
\(\partial_{\theta\zeta} B_{\theta}\) |
Tesla * meters |
Covariant poloidal component of magnetic field, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\zeta} B_{\theta}\) |
Tesla * meters |
Covariant poloidal component of magnetic field, derivative wrt toroidal angle |
||
|
\(\partial_{\zeta\zeta} B_{\theta}\) |
Tesla * meters |
Covariant poloidal component of magnetic field, second derivative wrt toroidal angle |
||
|
\(\partial_{\theta\theta} \mathbf{B}\) |
Tesla |
Magnetic field, second derivative wrt poloidal angle |
||
|
\(\partial_{\theta\zeta} \mathbf{B}\) |
Tesla |
Magnetic field, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\zeta} \mathbf{B}\) |
Tesla |
Magnetic field, derivative wrt toroidal angle |
||
|
\(B_{\zeta}\) |
Tesla * meters |
Covariant toroidal component of magnetic field |
||
|
\(\partial_{\rho} B_{\zeta}\) |
Tesla * meters |
Covariant toroidal component of magnetic field, derivative wrt radial coordinate |
||
|
\(\partial_{\rho\rho} B_{\zeta}\) |
Tesla * meters |
Covariant toroidal component of magnetic field, second derivative wrt radial coordinate |
||
|
\(\partial_{\rho\theta} B_{\zeta}\) |
Tesla * meters |
Covariant toroidal component of magnetic field, second derivative wrt radial coordinate and poloidal angle |
|
|
|
\(\partial_{\rho\zeta} B_{\zeta}\) |
Tesla * meters |
Covariant toroidal component of magnetic field, second derivative wrt radial coordinate and toroidal angle |
|
|
|
\(\partial_{\theta} B_{\zeta}\) |
Tesla * meters |
Covariant toroidal component of magnetic field, derivative wrt poloidal angle |
||
|
\(\partial_{\theta\theta} B_{\zeta}\) |
Tesla * meters |
Covariant toroidal component of magnetic field, second derivative wrt poloidal angle |
||
|
\(\partial_{\theta\zeta} B_{\zeta}\) |
Tesla * meters |
Covariant toroidal component of magnetic field, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\zeta} B_{\zeta}\) |
Tesla * meters |
Covariant toroidal component of magnetic field, derivative wrt toroidal angle |
||
|
\(\partial_{\zeta\zeta} B_{\zeta}\) |
Tesla * meters |
Covariant toroidal component of magnetic field, second derivative wrt toroidal angle |
||
|
\(\partial_{\zeta\zeta} \mathbf{B}\) |
Tesla |
Magnetic field, second derivative wrt toroidal angle |
||
|
:math:`` |
None |
Inner product norm for boozer modes basis. This norm is used as aweight when performing the integral of the Boozer transform to get the correct Boozer Fourier amplitudes. |
||
|
\(D_{\mathrm{Mercier}}\) |
Inverse Webers squared |
Mercier stability criterion (positive/negative value denotes stability/instability) |
||
|
\(D_{\mathrm{current}}\) |
Inverse Webers squared |
Mercier stability criterion toroidal current term |
||
|
\(D_{\mathrm{geodesic}}\) |
Inverse Webers squared |
Mercier stability criterion geodesic curvature term |
||
|
\(D_{\mathrm{shear}}\) |
Inverse Webers squared |
Mercier stability criterion magnetic shear term |
||
|
\(D_{\mathrm{well}}\) |
Inverse Webers squared |
Mercier stability criterion magnetic well term |
||
|
\(\mathbf{J} \times \mathbf{B} - \nabla p\) |
Newtons / cubic meter |
Force balance error |
||
|
\(F_{\mathrm{anisotropic}}\) |
Newtons / cubic meter |
Anisotropic force balance error |
||
|
\(F_{\mathrm{helical}}\) |
Amperes |
Covariant helical component of force balance error |
||
|
\(F_{\rho}\) |
Newtons / square meter |
Covariant radial component of force balance error |
||
|
\(F_{\theta}\) |
Newtons / square meter |
Covariant poloidal component of force balance error |
||
|
\(F_{\zeta}\) |
Newtons / square meter |
Covariant toroidal component of force balance error |
||
|
\(G\) |
Tesla * meters |
Covariant toroidal component of magnetic field in Boozer coordinates (proportional to poloidal current) |
||
|
\(\partial_{\rho} G\) |
Tesla * meters |
Covariant toroidal component of magnetic field in Boozer coordinates (proportional to poloidal current), derivative wrt radial coordinate |
||
|
\(\partial_{\rho\rho} G\) |
Tesla * meters |
Boozer poloidal current enclosed by flux surfaces, second derivative wrt radial coordinate |
||
|
\(\Gamma_c = \frac{\pi}{8 \sqrt{2}} \int d\lambda \langle \sum_j (v \tau \gamma_c^2)_j \rangle\) |
None |
Fast ion confinement proxy (scalar) |
|
|
|
\(\Gamma_c = \frac{\pi}{8 \sqrt{2}} \int d\lambda \langle \sum_j (v \tau \gamma_c^2)_j \rangle\) |
None |
Fast ion confinement proxy (scalar) as defined by Velasco et al. (doi:10.1088/1741-4326/ac2994) |
|
|
|
\(I\) |
Tesla * meters |
Covariant poloidal component of magnetic field in Boozer coordinates (proportional to toroidal current) |
||
|
\(\partial_{\rho} I\) |
Tesla * meters |
Covariant poloidal component of magnetic field in Boozer coordinates (proportional to toroidal current), derivative wrt radial coordinate |
||
|
\(\partial_{\rho\rho} I\) |
Tesla * meters |
Boozer toroidal current enclosed by flux surfaces, second derivative wrt radial coordinate |
||
|
\(\mathbf{J}\) |
Amperes / square meter |
Plasma current density |
||
|
\(\mathbf{J} \times (\nabla \rho)\) |
Amperes / cubed meter |
Plasma current density cross with grad(rho) |
||
|
\(\mathbf{J} \cdot \mathbf{B}\) |
Newtons / cubic meter |
Current density parallel to magnetic field, times field strength (note units are not Amperes) |
||
|
\(\mathbf{J} \sqrt{g}\) |
Ampere meters |
Plasma current density weighted by 3-D volume Jacobian |
||
|
\(J^{\rho}\) |
Amperes / cubic meter |
Contravariant radial component of plasma current density |
||
|
\(J^{\theta}\) |
Amperes / cubic meter |
Contravariant poloidal component of plasma current density |
||
|
\(J^{\theta} \sqrt{g}\) |
Amperes |
Contravariant poloidal component of plasma current density, weighted by 3-D volume Jacobian |
||
|
\(J^{\theta_{PEST}}\) |
Amperes / cubic meter |
Contravariant PEST poloidal component of plasma current density |
|
|
|
\(\partial_{\theta} J^{\theta}\) |
Amperes / cubic meter |
Derivative of contravariant poloidal component of plasma currentdensity w.r.t the poloidal coordinate |
||
|
\(\partial_{\theta} J^{\theta}\) |
Amperes / cubic meter |
Derivative of Contravariant poloidal component of plasma currentdensity w.r.t the toroidal coordinate |
||
|
\(J^{\zeta}\) |
Amperes / cubic meter |
Contravariant toroidal component of plasma current density |
||
|
\(\partial_{\theta} J^{\zeta}\) |
Amperes / cubic meter |
Derivative of the contravariant toroidal component of plasmacurrent density w.r.t the poloidal coordinate |
||
|
\(\partial_{\zeta} J^{\zeta}\) |
Amperes / cubic meter |
Derivative of the contravariant toroidal component of plasmacurrent density w.r.t the toroidal coordinate |
||
|
\(J_{R}\) |
Amperes / square meter |
Radial component of plasma current density in lab frame |
||
|
\(J_{Z}\) |
Amperes / square meter |
Vertical component of plasma current density in lab frame |
||
|
\(\mathbf{J} \cdot \hat{\mathbf{b}}\) |
Amperes / square meter |
Plasma current density parallel to magnetic field |
||
|
\(J_{\phi}\) |
Amperes / square meter |
Toroidal component of plasma current density in lab frame |
||
|
\(J_{\rho}\) |
Amperes / meter |
Covariant radial component of plasma current density |
||
|
\(J_{\theta}\) |
Amperes / meter |
Covariant poloidal component of plasma current density |
||
|
\(J_{\zeta}\) |
Amperes / meter |
Covariant toroidal component of plasma current density |
||
|
\(\mathbf{K}_{VC} = \frac{1}{\mu_0}\mathbf{n} \times \mathbf{B}\) |
Amps / meter |
Virtual casing sheet current |
||
|
\(L_{\nabla \mathbf{B}} = \frac{\sqrt{2}|B|}{|\nabla \mathbf{B}|}\) |
meters |
Magnetic field length scale based on Frobenius norm of gradient of magnetic field vector |
||
|
\(L_{\mathrm{SFF},\rho}\) |
meters |
L coefficient of second fundamental form of constant rho surface |
||
|
\(L_{\mathrm{SFF},\theta}\) |
meters |
L coefficient of second fundamental form of constant theta surface |
||
|
\(L_{\mathrm{SFF},\zeta}\) |
meters |
L coefficient of second fundamental form of constant zeta surface |
||
|
\(M_{\mathrm{SFF},\rho}\) |
meters |
M coefficient of second fundamental form of constant rho surface |
||
|
\(M_{\mathrm{SFF},\theta}\) |
meters |
M coefficient of second fundamental form of constant theta surface |
||
|
\(M_{\mathrm{SFF},\zeta}\) |
meters |
M coefficient of second fundamental form of constant zeta surface |
||
|
\(N_{\mathrm{SFF},\rho}\) |
meters |
N coefficient of second fundamental form of constant rho surface |
||
|
\(N_{\mathrm{SFF},\theta}\) |
meters |
N coefficient of second fundamental form of constant theta surface |
||
|
\(N_{\mathrm{SFF},\zeta}\) |
meters |
N coefficient of second fundamental form of constant zeta surface |
||
|
\(\mathrm{Newcomb-ballooning-metric}\) |
None |
A measure of Newcomb’s distance from marginal ballooning stability |
||
|
\(P_{ISS04}\) |
Watts |
Heating power required by the ISS04 energy confinement time scaling |
|
|
|
\(P_{fusion}\) |
Watts |
Fusion power |
|
|
|
\(\Psi\) |
Webers |
Toroidal flux |
||
|
\(R\) |
meters |
Major radius in lab frame |
||
|
\(R_{0} = V / (2\pi A) = \int R(\rho=0) d\zeta / (2\pi)\) |
meters |
Average major radius |
||
|
\(R_{0} / a\) |
None |
Aspect ratio |
||
|
\(R_{mn}^{\mathrm{Boozer}}\) |
meters |
Boozer harmonics of radial toroidal coordinate of a flux surface |
|
|
|
\(\partial_{\rho} R\) |
meters |
Major radius in lab frame, first radial derivative |
||
|
\(\partial_{\rho \rho} R\) |
meters |
Major radius in lab frame, second radial derivative |
||
|
\(\partial_{\rho \rho \rho} R\) |
meters |
Major radius in lab frame, third radial derivative |
||
|
\(\partial_{\rho \rho \rho \rho} R\) |
meters |
Major radius in lab frame, fourth radial derivative |
||
|
\(\partial_{\rho \rho \rho \theta} R\) |
meters |
Major radius in lab frame, fourth derivative wrt radial coordinate thrice and poloidal once |
|
|
|
\(\partial_{\rho \rho \rho \zeta} R\) |
meters |
Major radius in lab frame, fourth derivative wrt radial coordinate thrice and toroidal once |
|
|
|
\(\partial_{\rho \rho \theta} R\) |
meters |
Major radius in lab frame, third derivative, wrt radius twice and poloidal angle |
|
|
|
\(\partial_{\rho \rho \theta \theta} R\) |
meters |
Major radius in lab frame, fourth derivative, wrt radius twice and poloidal angle twice |
|
|
|
\(\partial_{\rho \rho \theta \zeta} R\) |
meters |
Major radius in lab frame, fourth derivative wrt radius twice, poloidal angle, and toroidal angle |
|
|
|
\(\partial_{\rho \rho \zeta} R\) |
meters |
Major radius in lab frame, third derivative, wrt radius twice and toroidal angle |
|
|
|
\(\partial_{\rho \rho \zeta \zeta} R\) |
meters |
Major radius in lab frame, fourth derivative, wrt radius twice and toroidal angle twice |
|
|
|
\(\partial_{\rho \theta} R\) |
meters |
Major radius in lab frame, second derivative wrt radius and poloidal angle |
|
|
|
\(\partial_{\rho \theta \theta} R\) |
meters |
Major radius in lab frame, third derivative wrt radius and poloidal angle twice |
|
|
|
\(\partial_{\rho \theta \theta \theta} R\) |
meters |
Major radius in lab frame, fourth derivative wrt radius and poloidal angle thrice |
|
|
|
\(\partial_{\rho \theta \theta \zeta} R\) |
meters |
Major radius in lab frame, fourth derivative wrt radius once, poloidal angle twice, and toroidal angle once |
|
|
|
\(\partial_{\rho \theta \zeta} R\) |
meters |
Major radius in lab frame, third derivative wrt radius, poloidal angle, and toroidal angle |
|
|
|
\(\partial_{\rho \theta \zeta \zeta} R\) |
meters |
Major radius in lab frame, fourth derivative wrt radius, poloidal angle, and toroidal angle twice |
|
|
|
\(\partial_{\rho \zeta} R\) |
meters |
Major radius in lab frame, second derivative wrt radius and toroidal angle |
|
|
|
\(\partial_{\rho \zeta \zeta} R\) |
meters |
Major radius in lab frame, third derivative wrt radius and toroidal angle twice |
|
|
|
\(\partial_{\rho \zeta \zeta \zeta} R\) |
meters |
Major radius in lab frame, fourth derivative wrt radius and toroidal angle thrice |
|
|
|
\(\partial_{\theta} R\) |
meters |
Major radius in lab frame, first poloidal derivative |
||
|
\(\partial_{\theta \theta} R\) |
meters |
Major radius in lab frame, second poloidal derivative |
||
|
\(\partial_{\theta \theta \theta} R\) |
meters |
Major radius in lab frame, third poloidal derivative |
||
|
\(\partial_{\theta \theta \zeta} R\) |
meters |
Major radius in lab frame, third derivative wrt poloidal angle twice and toroidal angle |
|
|
|
\(\partial_{\theta \zeta} R\) |
meters |
Major radius in lab frame, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\theta \zeta \zeta} R\) |
meters |
Major radius in lab frame, third derivative wrt poloidal angle and toroidal angle twice |
|
|
|
\(\partial_{\zeta} R\) |
meters |
Major radius in lab frame, first toroidal derivative |
||
|
\(\partial_{\zeta \zeta} R\) |
meters |
Major radius in lab frame, second toroidal derivative |
||
|
\(\partial_{\zeta \zeta \zeta} R\) |
meters |
Major radius in lab frame, third toroidal derivative |
||
|
\(S\) |
square meters |
Surface area of outermost flux surface, extrapolated to last closed flux surface |
||
|
\(S(\rho)\) |
square meters |
Surface area of flux surfaces |
||
|
\(\partial_{\rho} S(\rho)\) |
square meters |
Surface area of flux surfaces, derivative wrt radial coordinate |
||
|
\(\partial_{\rho\rho} S(\rho)\) |
square meters |
Surface area of flux surfaces, second derivative wrt radial coordinate |
||
|
\(T_e\) |
electron-Volts |
Electron temperature |
||
|
\(\partial_{\rho} T_e\) |
electron-Volts |
Electron temperature, first radial derivative |
||
|
\(\partial_{\rho \rho} T_e\) |
electron-Volts |
Electron temperature, second radial derivative |
||
|
\(T_i\) |
electron-Volts |
Ion temperature |
||
|
\(\partial_{\rho} T_i\) |
electron-Volts |
Ion temperature, first radial derivative |
||
|
\(\partial_{\rho \rho} T_i\) |
electron-Volts |
Ion temperature, second radial derivative |
||
|
\(V\) |
cubic meters |
Volume extrapolated to last closed flux surface |
||
|
\(V(\rho)\) |
cubic meters |
Volume enclosed by flux surfaces |
||
|
\(\int \vert B^{\zeta} \vert^{-1} \mathrm{d}\alpha \mathrm{d}\zeta\) |
cubic meters per Weber |
Surface integrated volume Jacobian determinant of Clebsch field line coordinate system (ψ,α,ζ) where ζ is the DESC toroidal coordinate. |
||
|
\(\partial_{\rho} V(\rho)\) |
cubic meters |
Volume enclosed by flux surfaces, derivative wrt radial coordinate |
||
|
\(\partial_{\rho\rho} V(\rho)\) |
cubic meters |
Volume enclosed by flux surfaces, second derivative wrt radial coordinate |
||
|
\(\partial_{\rho\rho\rho} V(\rho)\) |
cubic meters |
Volume enclosed by flux surfaces, third derivative wrt radial coordinate |
||
|
\(W\) |
Joules |
Plasma total energy |
||
|
\(W_B\) |
Joules |
Plasma magnetic energy |
||
|
\(W_{B,pol}\) |
Joules |
Plasma magnetic energy in poloidal field |
||
|
\(W_{B,tor}\) |
Joules |
Plasma magnetic energy in toroidal field |
||
|
\(W_p\) |
Joules |
Plasma thermodynamic energy |
|
|
|
\(X = R \cos{\phi}\) |
meters |
Cartesian X coordinate |
||
|
\(\partial_{\rho} X\) |
meters |
Cartesian X coordinate, derivative wrt radial coordinate |
||
|
\(\partial_{\theta} X\) |
meters |
Cartesian X coordinate, derivative wrt poloidal coordinate |
||
|
\(\partial_{\zeta} X\) |
meters |
Cartesian X coordinate, derivative wrt toroidal coordinate |
||
|
\(Y = R \sin{\phi}\) |
meters |
Cartesian Y coordinate |
||
|
\(\partial_{\rho} Y\) |
meters |
Cartesian Y coordinate, derivative wrt radial coordinate |
||
|
\(\partial_{\theta} Y\) |
meters |
Cartesian Y coordinate, derivative wrt poloidal coordinate |
||
|
\(\partial_{\zeta} Y\) |
meters |
Cartesian Y coordinate, derivative wrt toroidal coordinate |
||
|
\(Z\) |
meters |
Vertical coordinate in lab frame |
||
|
\(Z_{mn}^{\mathrm{Boozer}}\) |
meters |
Boozer harmonics of vertical coordinate of a flux surface |
|
|
|
\(\partial_{\rho} Z\) |
meters |
Vertical coordinate in lab frame, first radial derivative |
||
|
\(\partial_{\rho \rho} Z\) |
meters |
Vertical coordinate in lab frame, second radial derivative |
||
|
\(\partial_{\rho \rho \rho} Z\) |
meters |
Vertical coordinate in lab frame, third radial derivative |
||
|
\(\partial_{\rho \rho \rho \rho} Z\) |
meters |
Vertical coordinate in lab frame, fourth radial derivative |
||
|
\(\partial_{\rho \rho \rho \theta} Z\) |
meters |
Vertical coordinate in lab frame, fourth derivative wrt radial coordinate thrice and poloidal once |
|
|
|
\(\partial_{\rho \rho \rho \zeta} Z\) |
meters |
Vertical coordinate in lab frame, fourth derivative wrt radial coordinate thrice and toroidal once |
|
|
|
\(\partial_{\rho \rho \theta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative, wrt radius twice and poloidal angle |
|
|
|
\(\partial_{\rho \rho \theta} Z\) |
meters |
Vertical coordinate in lab frame, fourth derivative, wrt radius twice and poloidal angle twice |
|
|
|
\(\partial_{\rho \rho \theta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, fourth derivative wrt radiustwice, poloidal angle, and toroidal angle |
|
|
|
\(\partial_{\rho \rho \zeta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative, wrt radius twice and toroidal angle |
|
|
|
\(\partial_{\rho \rho \zeta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, fourth derivative, wrt radius twice and toroidal angle twice |
|
|
|
\(\partial_{\rho \theta} Z\) |
meters |
Vertical coordinate in lab frame, second derivative wrt radius and poloidal angle |
|
|
|
\(\partial_{\rho \theta \theta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative wrt radius and poloidal angle twice |
|
|
|
\(\partial_{\rho \theta \theta \theta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative wrt radius and poloidal angle thrice |
|
|
|
\(\partial_{\rho \theta \theta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, fourth derivative wrt radius once, poloidal angle twice, and toroidal angle once |
|
|
|
\(\partial_{\rho \theta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative wrt radius, poloidal angle, and toroidal angle |
|
|
|
\(\partial_{\rho \theta \zeta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, fourth derivative wrt radius, poloidal angle, and toroidal angle twice |
|
|
|
\(\partial_{\rho \zeta} Z\) |
meters |
Vertical coordinate in lab frame, second derivative wrt radius and toroidal angle |
|
|
|
\(\partial_{\rho \zeta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative wrt radius and toroidal angle twice |
|
|
|
\(\partial_{\rho \zeta \zeta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative wrt radius and toroidal angle thrice |
|
|
|
\(\partial_{\theta} Z\) |
meters |
Vertical coordinate in lab frame, first poloidal derivative |
||
|
\(\partial_{\theta \theta} Z\) |
meters |
Vertical coordinate in lab frame, second poloidal derivative |
||
|
\(\partial_{\theta \theta \theta} Z\) |
meters |
Vertical coordinate in lab frame, third poloidal derivative |
||
|
\(\partial_{\theta \theta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative wrt poloidal angle twice and toroidal angle |
|
|
|
\(\partial_{\theta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\theta \zeta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative wrt poloidal angle and toroidal angle twice |
|
|
|
\(\partial_{\zeta} Z\) |
meters |
Vertical coordinate in lab frame, first toroidal derivative |
||
|
\(\partial_{\zeta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, second toroidal derivative |
||
|
\(\partial_{\zeta \zeta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, third toroidal derivative |
||
|
\(Z_{eff}\) |
None |
Effective atomic number |
||
|
\(\partial_{\rho} Z_{eff}\) |
None |
Effective atomic number, first radial derivative |
||
|
\(a\) |
meters |
Average minor radius |
||
|
\(a_{\mathrm{major}} / a_{\mathrm{minor}}\) |
None |
Elongation at a toroidal cross-section (constant zeta surface), extrapolated to last closed flux surface. |
||
|
\(\alpha\) |
None |
Field line label |
||
|
\(\partial_\rho \alpha\) |
None |
Field line label, derivative wrt radial coordinate |
||
|
\(\mathrm{periodic}(\partial_\rho \alpha)\) |
None |
Field line label, derivative wrt radial coordinate, periodic component |
||
|
\(\mathrm{secular}(\partial_\rho \alpha)\) |
None |
Field line label, derivative wrt radial coordinate, secular component |
||
|
\(\partial_\theta \alpha\) |
None |
Field line label, derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta} \alpha\) |
None |
Field line label, second-order derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \zeta} \alpha\) |
None |
Field line label, derivative wrt poloidal and toroidal coordinates |
|
|
|
\(\partial_\zeta \alpha\) |
None |
Field line label, derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta \zeta} \alpha\) |
None |
Field line label, second-order derivative wrt toroidal coordinate |
||
|
\(\hat{b}\) |
None |
Unit vector along magnetic field |
||
|
\(\beta_a = \mu_0 (p_{||} - p_{\perp})/B^2\) |
None |
Pressure anisotropy |
||
|
\(\partial_{\rho} \beta_a = \mu_0 (p_{||} - p_{\perp})/B^2\) |
None |
Pressure anisotropy, first radial derivative |
||
|
\(\partial_{\theta} \beta_a = \mu_0 (p_{||} - p_{\perp})/B^2\) |
None |
Pressure anisotropy, first poloidal derivative |
||
|
\(\partial_{\zeta} \beta_a = \mu_0 (p_{||} - p_{\perp})/B^2\) |
None |
Pressure anisotropy, first toroidal derivative |
||
|
\(2 a^3 B_n \mu_0 \mathrm{sign}(\psi) (\partial_{\psi} p) / (\vert B \vert^2 b \cdot \nabla ζ) (b \times \kappa) \cdot \nabla (\alpha + \iota \zeta_0) \rho^2\) |
None |
Parameter in ideal ballooning equation |
|
|
|
\(\chi\) |
Webers |
Poloidal flux (normalized by 2pi) |
||
|
\(\partial_{\rho} \chi\) |
Webers |
Poloidal flux (normalized by 2pi), first radial derivative |
||
|
\((\nabla \times \mathbf{B}) \times \mathbf{B}\) |
Tesla squared / meters |
Lorentz force |
||
|
\(\frac{2\pi}{\mu_0} I\) |
Amperes |
Net toroidal current enclosed by flux surfaces |
||
|
\(\frac{2\pi}{\mu_0} I_{Redl}\) |
Amperes |
Net toroidal current enclosed by flux surfaces, consistent with bootstrap current from Redl formula |
|
|
|
\(\frac{2\pi}{\mu_0} \partial_{\rho} I\) |
Amperes |
Net toroidal current enclosed by flux surfaces, derivative wrt radial coordinate |
||
|
\(\frac{2\pi}{\mu_0} \partial_{\rho\rho} I\) |
Amperes |
Net toroidal current enclosed by flux surfaces, second derivative wrt radial coordinate |
||
|
\(H_{\rho}\) |
inverse meters |
Mean curvature of constant rho surfaces |
||
|
\(H_{\theta}\) |
inverse meters |
Mean curvature of constant theta surfaces |
||
|
\(H_{\zeta}\) |
inverse meters |
Mean curvature of constant zeta surfaces |
||
|
\(K_{\rho}\) |
inverse meters squared |
Gaussian curvature of constant rho surfaces |
||
|
\(K_{\theta}\) |
inverse meters squared |
Gaussian curvature of constant theta surfaces |
||
|
\(K_{\zeta}\) |
inverse meters squared |
Gaussian curvature of constant zeta surfaces |
||
|
\(k_{1,\rho}\) |
inverse meters |
First principle curvature of constant rho surfaces |
||
|
\(k_{1,\theta}\) |
inverse meters |
First principle curvature of constant theta surfaces |
||
|
\(k_{1,\zeta}\) |
inverse meters |
First principle curvature of constant zeta surfaces |
||
|
\(k_{2,\rho}\) |
inverse meters |
Second principle curvature of constant rho surfaces |
||
|
\(k_{2,\theta}\) |
inverse meters |
Second principle curvature of constant theta surfaces |
||
|
\(k_{2,\zeta}\) |
inverse meters |
Second principle curvature of constant zeta surfaces |
||
|
\(\mathrm{cvdrift} = 1/B^{3} (\mathbf{b}\times\nabla( \mu_0 p + B^2/2))\cdot \nabla \alpha\) |
Inverse webers |
Binormal, geometric part of the curvature drift. Used for local stability analyses and gyrokinetics. |
||
|
\(\mathrm{cvdrift (periodic)}\) |
Inverse webers |
Periodic, binormal, geometric part of the curvature drift. |
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|
\(\mathrm{cvdrift0} = 1/B^{2} (\mathbf{b}\times\nabla \vert B \vert)\cdot (2 \rho \nabla \rho)\) |
Inverse webers |
Radial, geometric part of the curvature drift. Used for local stability analyses, gyrokinetics, and Gamma_c. |
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|
\(B^{\theta} \nabla \zeta - B^{\zeta} \nabla \theta\) |
Tesla / square meter |
Helical basis vector |
||
|
\(\sqrt{g}(B^{\theta} \nabla \zeta - B^{\zeta} \nabla \theta)\) |
Tesla * square meter |
Helical basis vector weighted by 3-D volume Jacobian |
||
|
\(\mathbf{e}^{\rho}\) |
inverse meters |
Contravariant radial basis vector |
|
|
|
\(\partial_{\rho} \mathbf{e}^{\rho}\) |
inverse meters |
Contravariant radial basis vector, derivative wrt radial coordinate |
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|
\(\partial_{\rho\rho} \mathbf{e}^{\rho}\) |
inverse square meters |
Contravariant Radial basis vector, 2nd derivative wrt radial coordinate |
||
|
\(\partial_{\rho\theta} \mathbf{e}^{\rho}\) |
inverse square meters |
Contravariant Radial basis vector, derivative wrt radial and poloidal coordinate |
|
|
|
\(\partial_{\rho\zeta} \mathbf{e}^{\rho}\) |
inverse square meters |
Contravariant Radial basis vector, derivative wrt radial and toroidal coordinate |
|
|
|
\(\partial_{\theta} \mathbf{e}^{\rho}\) |
inverse meters |
Contravariant radial basis vector, derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta\theta} \mathbf{e}^{\rho}\) |
inverse square meters |
Contravariant Radial basis vector, 2nd derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta\zeta} \mathbf{e}^{\rho}\) |
inverse square meters |
Contravariant Radial basis vector, derivative wrt poloidal and toroidal coordinate |
|
|
|
\(\partial_{\zeta} \mathbf{e}^{\rho}\) |
inverse meters |
Contravariant radial basis vector, derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta\zeta} \mathbf{e}^{\rho}\) |
inverse square meters |
Contravariant Radial basis vector, 2nd derivative wrt toroidal coordinate |
||
|
\(\mathbf{e}^{\theta}\) |
inverse meters |
Contravariant poloidal basis vector |
||
|
\(\mathbf{e}^{\theta} \sqrt{g}\) |
square meters |
Contravariant poloidal basis vector weighted by 3-D volume Jacobian |
||
|
\(\partial_{\rho} \mathbf{e}^{\theta}\) |
inverse meters |
Contravariant poloidal basis vector, derivative wrt radial coordinate |
||
|
\(\partial_{\rho\rho} \mathbf{e}^{\theta}\) |
inverse square meters |
Contravariant Poloidal basis vector, 2nd derivative wrt radial coordinate |
||
|
\(\partial_{\rho\theta} \mathbf{e}^{\theta}\) |
inverse square meters |
Contravariant Poloidal basis vector, derivative wrt radial and poloidal coordinate |
|
|
|
\(\partial_{\rho\zeta} \mathbf{e}^{\theta}\) |
inverse square meters |
Contravariant Poloidal basis vector, derivative wrt radial and toroidal coordinate |
|
|
|
\(\partial_{\theta} \mathbf{e}^{\theta}\) |
inverse meters |
Contravariant poloidal basis vector, derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta\theta} \mathbf{e}^{\theta}\) |
inverse square meters |
Contravariant Poloidal basis vector, 2nd derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta\zeta} \mathbf{e}^{\theta}\) |
inverse square meters |
Contravariant Poloidal basis vector, derivative wrt poloidal and toroidal coordinate |
|
|
|
\(\partial_{\zeta} \mathbf{e}^{\theta}\) |
inverse meters |
Contravariant poloidal basis vector, derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta\zeta} \mathbf{e}^{\theta}\) |
inverse square meters |
Contravariant Poloidal basis vector, 2nd derivative wrt toroidal coordinate |
||
|
\(\mathbf{e}^{\vartheta}\) |
inverse meters |
Contravariant PEST poloidal basis vector |
|
|
|
\(\mathbf{e}^{\zeta}\) |
inverse meters |
Contravariant toroidal basis vector |
||
|
\(\partial_{\rho} \mathbf{e}^{\zeta}\) |
inverse meters |
Contravariant toroidal basis vector, derivative wrt radial coordinate |
||
|
\(\partial_{\rho\rho} \mathbf{e}^{\zeta}\) |
inverse square meters |
Contravariant Toroidal basis vector, 2nd derivative wrt radial coordinate |
||
|
\(\partial_{\rho\theta} \mathbf{e}^{\zeta}\) |
inverse square meters |
Contravariant Toroidal basis vector, derivative wrt radial and poloidal coordinate |
|
|
|
\(\partial_{\rho\zeta} \mathbf{e}^{\zeta}\) |
inverse square meters |
Contravariant Toroidal basis vector, derivative wrt radial and toroidal coordinate |
|
|
|
\(\partial_{\theta} \mathbf{e}^{\zeta}\) |
inverse meters |
Contravariant toroidal basis vector, derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta\theta} \mathbf{e}^{\zeta}\) |
inverse square meters |
Contravariant Toroidal basis vector, 2nd derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta\zeta} \mathbf{e}^{\zeta}\) |
inverse square meters |
Contravariant Toroidal basis vector, derivative wrt poloidal and toroidal coordinate |
|
|
|
\(\partial_{\zeta} \mathbf{e}^{\zeta}\) |
inverse meters |
Contravariant toroidal basis vector, derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta\zeta} \mathbf{e}^{\zeta}\) |
inverse square meters |
Contravariant Toroidal basis vector, 2nd derivative wrt toroidal coordinate |
||
|
\(\mathbf{e}_{\alpha}\) |
meters |
Covariant poloidal basis vector in (ρ, α, ζ) Clebsch coordinates. |
||
|
\(\partial_{\theta} \mathbf{e}_{\alpha}\) |
meters |
Covariant poloidal basis vector in (ρ, α, ζ) Clebsch coordinates, derivative wrt DESC poloidal angle |
||
|
\(\partial_{\zeta} \mathbf{e}_{\alpha}\) |
meters |
Covariant poloidal basis vector in (ρ, α, ζ) Clebsch coordinates, derivative wrt DESC toroidal angle at fixed ρ,θ. |
||
|
\(\mathbf{e}_{\alpha} |_{\rho, \phi}\) |
meters |
Covariant poloidal basis vector in (ρ, α, ϕ) Clebsch coordinates. |
||
|
\(\mathbf{e}_{\phi} |_{\rho, \theta}\) |
meters |
Covariant toroidal basis vector in (ρ,θ,ϕ) coordinates |
|
|
|
\(\mathbf{e}_{\phi} |_{\rho, \vartheta}\) |
meters |
Covariant toroidal basis vector in (ρ,ϑ,ϕ) coordinates or straight field line PEST coordinates. ϕ increases counterclockwise when viewed from above (cylindrical R,ϕ plane with Z out of page). |
|
|
|
\(\mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector |
||
|
\(\partial_{\rho} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, derivative wrt radial coordinate |
||
|
\(\partial_{\rho \rho} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, second derivative wrt radial and radial coordinates |
||
|
\(\partial_{\rho \rho \rho} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, third derivative wrt radial coordinate |
||
|
\(\partial_{\rho \rho \theta} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, third derivative wrt radial coordinate twice and poloidal once |
|
|
|
\(\partial_{\rho \rho \zeta} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, third derivative wrt radial coordinate twice and toroidal once |
|
|
|
\(\partial_{\rho \theta} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, second derivative wrt radial and poloidal coordinates |
|
|
|
\(\partial_{\rho \theta \theta} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, third derivative wrt radial coordinateonce and poloidal twice |
|
|
|
\(\partial_{\rho \theta \zeta} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, third derivative wrt radial, poloidal, and toroidal coordinates |
|
|
|
\(\partial_{\rho \zeta} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, second derivative wrt radial and toroidal coordinates |
|
|
|
\(\partial_{\rho \zeta \zeta} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, third derivative wrt radial coordinate once and toroidal twice |
|
|
|
\(\partial_{\theta} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, derivative wrt poloidal coordinate |
|
|
|
\(\partial_{\theta \theta} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, second derivative wrt poloidal and poloidal coordinates |
|
|
|
\(\partial_{\theta \zeta} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, second derivative wrt poloidal and toroidal coordinates |
|
|
|
\(\partial_{\zeta} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, derivative wrt toroidal coordinate |
|
|
|
\(\partial_{\zeta \zeta} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, second derivative wrt toroidal and toroidal coordinates |
|
|
|
\(\mathbf{e}_{\rho} |_{\alpha, \zeta}\) |
meters |
Covariant radial basis vector in (ρ, α, ζ) Clebsch coordinates. |
||
|
\(\mathbf{e}_{\rho} |_{\vartheta, \phi}\) |
meters |
Covariant radial basis vector in (ρ,ϑ,ϕ) coordinates or straight field line PEST coordinates. ϕ increases counterclockwise when viewed from above (cylindrical R,ϕ plane with Z out of page). |
|
|
|
\(\mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector |
||
|
\(\mathbf{e}_{\theta} / \sqrt{g}\) |
meters |
Covariant Poloidal basis vector divided by 3-D volume Jacobian |
||
|
\(\mathbf{e}_{\vartheta} |_{\rho, \phi} = \mathbf{e}_{\theta_{PEST}}\) |
meters |
Covariant poloidal basis vector in (ρ,ϑ,ϕ) coordinates or straight field line PEST coordinates. ϕ increases counterclockwise when viewed from above (cylindrical R,ϕ plane with Z out of page). |
|
|
|
\(\partial_{\rho \theta \theta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, third derivative wrt radial coordinate once and poloidal twice |
|
|
|
\(\partial_{\rho \theta \zeta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, third derivative wrt radial, poloidal, and toroidal coordinates |
|
|
|
\(\partial_{\rho \zeta \zeta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, third derivative wrt radial coordinate once and toroidal twice |
|
|
|
\(\partial_{\theta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, second derivative wrt poloidal and poloidal coordinates |
||
|
\(\partial_{\theta \zeta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, second derivative wrt poloidal and toroidal coordinates |
|
|
|
\(\partial_{\zeta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, derivative wrt toroidal coordinate |
|
|
|
\(\partial_{\zeta \zeta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, second derivative wrt toroidal and toroidal coordinates |
|
|
|
\(\mathbf{e}_{\theta} |_{\rho, \phi}\) |
meters |
Covariant poloidal basis vector in (ρ,θ,ϕ) coordinates. ϕ increases counterclockwise when viewed from above (cylindrical R,ϕ plane with Z out of page). |
||
|
\(\mathbf{e}_{\zeta}\) |
meters |
Covariant Toroidal basis vector |
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|
\(\partial_{\rho \zeta \zeta} \mathbf{e}_{\zeta}\) |
meters |
Covariant Toroidal basis vector, third derivative wrt radial coordinate once and toroidal twice |
|
|
|
\(\partial_{\zeta} \mathbf{e}_{\zeta}\) |
meters |
Covariant Toroidal basis vector, derivative wrt toroidal coordinate |
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|
\(\partial_{\zeta \zeta} \mathbf{e}_{\zeta}\) |
meters |
Covariant Toroidal basis vector, second derivative wrt toroidal and toroidal coordinates |
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|
\(\mathbf{e}_{\zeta} |_{\rho, \alpha} = \frac{\mathbf{B}}{\mathbf{B} \cdot \nabla \zeta}\) |
meters |
Tangent vector along (collinear to) field line |
||
|
\((r / R_0)_{\mathrm{effective}}\) |
None |
Effective local inverse aspect ratio, based on max and min |B| |
||
|
\(\epsilon_{\mathrm{eff}}\) |
None |
Neoclassical transport in the banana regime |
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|
\(\epsilon_{\mathrm{eff}}^{3/2} = \frac{\pi}{8 \sqrt{2}} R_0^2 \langle \vert\nabla \psi\vert \rangle^{-2} B_0^{-1} \int d\lambda \lambda^{-2} \langle \sum_j H_j^2 / I_j \rangle\) |
None |
Effective ripple modulation amplitude to 3/2 power |
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|
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\(a B_n^3 \vert B \vert^{-2} / (B \cdot \nabla ζ) \vert \nabla (\alpha + \iota \zeta_0 \mathrm{sign} \iota) \vert^2 \rho^2\) |
None |
Parameter in ideal ballooning equation |
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|
\([(M \iota - N) (\mathbf{B} \times \nabla \psi) - (M G + N I) \mathbf{B}] \cdot \nabla B\) |
Tesla cubed |
Two-term quasisymmetry metric |
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|
|
\(\nabla \psi \times \nabla B \cdot \nabla (\mathbf{B} \cdot \nabla B)\) |
Tesla quarted / square meters |
Triple product quasisymmetry metric |
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\(\int_{\zeta_{\mathrm{min}}}^{\zeta_{\mathrm{max}}} \frac{d\zeta}{|B^{\zeta}|}\) |
Meter / tesla |
(Mean) proper length of field line(s) |
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\(\int_{\zeta_{\mathrm{min}}}^{\zeta_{\mathrm{max}}} \frac{d\zeta}{|B^{\zeta} \sqrt g|}\) |
inverse webers |
(Mean) proper length over volume of field line(s) |
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\((\mathbf{J} \times (\nabla \rho))/{(g^{\rho \rho})}^2 \mathbf{B} \cdot \mathbf{\nabla} (\mathbf{\nabla} \rho)\) |
Tesla Amperes / meter |
finite-n instability drive term |
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\(a^3 B_n \vert B \vert^{-2} (B \cdot \nabla ζ) \vert \nabla (\alpha + \iota \zeta_0 \mathrm{sign} \iota) \vert^2 \rho^2\) |
None |
Parameter in ideal ballooning equation |
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\(g^{\alpha \alpha}\) |
inverse square meters |
Contravariant metric tensor grad alpha dot grad alpha |
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\(g^{\rho \alpha}\) |
inverse square meters |
Contravariant metric tensor grad rho dot grad alpha |
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|
\(g^{\rho\rho}\) |
inverse square meters |
Radial/Radial element of contravariant metric tensor |
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\(\partial_{\rho} g^{\rho \rho}\) |
inverse square meters |
Radial/Radial element of contravariant metric tensor, first radial derivative |
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|
\(\partial_{\theta} g^{\rho \rho}\) |
inverse square meters |
Radial/Radial element of contravariant metric tensor, first poloidal derivative |
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|
\(\partial_{\zeta} g^{\rho \rho}\) |
inverse square meters |
Radial/Radial element of contravariant metric tensor, first toroidal derivative |
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|
\(g^{\rho\theta}\) |
inverse square meters |
Radial/Poloidal (ρ, θ) element of contravariant metric tensor |
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|
\(\partial_{\rho} g^{\rho \theta}\) |
inverse square meters |
Radial/Poloidal element of contravariant metric tensor, first radial derivative |
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|
\(\partial_{\theta} g^{\rho \theta}\) |
inverse square meters |
Radial/Poloidal element of contravariant metric tensor, first poloidal derivative |
||
|
\(\partial_{\zeta} g^{\rho \theta}\) |
inverse square meters |
Radial/Poloidal element of contravariant metric tensor, first toroidal derivative |
||
|
\(g^{\rho \vartheta}\) |
inverse square meters |
Radial-Poloidal element of covariant metric tensor PEST_coordinates |
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|
\(g^{\rho\zeta}\) |
inverse square meters |
Radial/Toroidal element of contravariant metric tensor |
||
|
\(\partial_{\rho} g^{\rho \zeta}\) |
inverse square meters |
Radial/Toroidal element of contravariant metric tensor, first radial derivative |
||
|
\(\partial_{\theta} g^{\rho \zeta}\) |
inverse square meters |
Radial/Toroidal element of contravariant metric tensor, first poloidal derivative |
||
|
\(\partial_{\zeta} g^{\rho \zeta}\) |
inverse square meters |
Radial/Toroidal element of contravariant metric tensor, first toroidal derivative |
||
|
\(g^{\theta\theta}\) |
inverse square meters |
Poloidal/Poloidal element of contravariant metric tensor |
||
|
\(\partial_{\rho} g^{\theta \theta}\) |
inverse square meters |
Poloidal/Poloidal element of contravariant metric tensor, first radial derivative |
||
|
\(\partial_{\theta} g^{\theta \theta}\) |
inverse square meters |
Poloidal/Poloidal element of contravariant metric tensor, first poloidal derivative |
||
|
\(\partial_{\zeta} g^{\theta \theta}\) |
inverse square meters |
Poloidal/Poloidal element of contravariant metric tensor, first toroidal derivative |
||
|
\(g^{\theta\zeta}\) |
inverse square meters |
Poloidal/Toroidal element of contravariant metric tensor |
|
|
|
\(\partial_{\rho} g^{\theta \zeta}\) |
inverse square meters |
Poloidal/Toroidal element of contravariant metric tensor, first radial derivative |
||
|
\(\partial_{\theta} g^{\theta \zeta}\) |
inverse square meters |
Poloidal/Toroidal element of contravariant metric tensor, first poloidal derivative |
||
|
\(\partial_{\zeta} g^{\theta \zeta}\) |
inverse square meters |
Poloidal/Toroidal element of contravariant metric tensor, first toroidal derivative |
||
|
\(g^{\zeta\zeta}\) |
inverse square meters |
Toroidal/Toroidal element of contravariant metric tensor |
||
|
\(\partial_{\rho} g^{\zeta \zeta}\) |
inverse square meters |
Toroidal/Toroidal element of contravariant metric tensor, first radial derivative |
||
|
\(\partial_{\theta} g^{\zeta \zeta}\) |
inverse square meters |
Toroidal/Toroidal element of contravariant metric tensor, first poloidal derivative |
||
|
\(\partial_{\zeta} g^{\zeta \zeta}\) |
inverse square meters |
Toroidal/Toroidal element of contravariant metric tensor, first toroidal derivative |
||
|
\(g_{\phi \phi}|PEST\) |
square meters |
Toroidal-Toroidal element of covariant metric tensor PEST_coordinates |
||
|
\(g_{\rho\phi}|PEST\) |
square meters |
Radial-Toroidal element of covariant metric tensor PEST_coordinates |
|
|
|
\(g_{\rho\rho}\) |
square meters |
Radial/Radial element of covariant metric tensor |
||
|
\(g_{\rho\rho}|PEST\) |
square meters |
Radial-Radial element of covariant metric tensor PEST_coordinates |
||
|
\(g_{\rho\theta}\) |
square meters |
Radial/Poloidal element of covariant metric tensor |
|
|
|
\(g_{\rho\vartheta}|PEST\) |
square meters |
Radial-Poloidal element of covariant metric tensor PEST_coordinates |
|
|
|
\(g_{\rho\zeta}\) |
square meters |
Radial/Toroidal element of covariant metric tensor |
|
|
|
\(g_{\theta\theta}\) |
square meters |
Poloidal/Poloidal element of covariant metric tensor |
||
|
\(\partial_{\rho} g_{\theta\theta}\) |
square meters |
Poloidal/Poloidal element of covariant metric tensor, derivative wrt rho |
||
|
\(\partial_{\rho\rho} g_{\theta\theta}\) |
square meters |
Poloidal/Poloidal element of covariant metric tensor, second derivative wrt rho |
||
|
\(\partial_{\rho\rho\rho} g_{\theta\theta}\) |
square meters |
Poloidal/Poloidal element of covariant metric tensor, third derivative wrt rho |
||
|
\(g_{\theta\zeta}\) |
square meters |
Poloidal/Toroidal element of covariant metric tensor |
|
|
|
\(\partial_{\rho} g_{\theta\zeta}\) |
square meters |
Poloidal/Toroidal element of covariant metric tensor, derivative wrt rho |
||
|
\(\partial_{\rho\rho} g_{\theta\zeta}\) |
square meters |
Poloidal/Toroidal element of covariant metric tensor, second derivative wrt rho |
||
|
\(\partial_{\rho\rho\rho} g_{\theta\zeta}\) |
square meters |
Poloidal/Toroidal element of covariant metric tensor, third derivative wrt rho |
||
|
\(g_{\vartheta \phi}|PEST\) |
square meters |
Poloidal-Toroidal element of covariant metric tensor PEST_coordinates |
|
|
|
\(g_{\vartheta \vartheta}|PEST\) |
square meters |
Poloidal-Poloidal element of covariant metric tensor PEST_coordinates |
||
|
\(g_{\zeta\zeta}\) |
square meters |
Toroidal/Toroidal element of covariant metric tensor |
||
|
\(\sum_{w} \gamma_c(\rho, \alpha, \lambda, w)\) |
None |
Fast ion confinement proxy |
|
|
|
\((\nabla \vert B \vert)_{\mathrm{drift}} = (\mathbf{b} \times \nabla B) \cdot \nabla \alpha / \vert B \vert^{2}\) |
Inverse webers |
Binormal, geometric part of the gradB drift. Used for local stability analyses, gyrokinetics, and Gamma_c. |
||
|
\(\mathrm{periodic}(\nabla \vert B \vert)_{\mathrm{drift}}\) |
Inverse webers |
Periodic, binormal, geometric part of the gradB drift. |
||
|
\(\mathrm{secular}(\nabla \vert B \vert)_{\mathrm{drift}}\) |
Inverse webers |
Secular, binormal, geometric part of the gradB drift. |
||
|
\(\mathrm{secular}(\nabla \vert B \vert)_{\mathrm{drift}} / \phi\) |
Inverse webers |
Secular, binormal, geometric part of the gradB drift divided by the toroidal angle. This quantity is periodic. |
||
|
\(\nabla \mathbf{B}\) |
Tesla / meter |
Gradient of magnetic field vector |
||
|
\(\nabla \alpha\) |
Inverse meters |
Gradient of field line label, which is perpendicular to the field line |
||
|
\(\mathrm{periodic}(\nabla \alpha)\) |
Inverse meters |
Gradient of field line label, which is perpendicular to the field line, periodic component |
||
|
\(\mathrm{secular}(\nabla \alpha)\) |
Inverse meters |
Gradient of field line label, which is perpendicular to the field line, secular component |
||
|
\(\nabla \beta_a = \nabla \mu_0 (p_{||} - p_{\perp})/B^2\) |
Inverse meters |
Pressure anisotropy gradient |
||
|
\(\nabla p\) |
Newtons / cubic meter |
Pressure gradient |
||
|
\(\nabla \phi\) |
Inverse meters |
Gradient of cylindrical toroidal angle ϕ. |
||
|
\(\nabla\psi\) |
Webers per meter |
Toroidal flux gradient (normalized by 2pi) |
||
|
\(\nabla |\mathbf{B}|\) |
Tesla / meters |
Gradient of magnetic field magnitude |
||
|
\(\nabla |B|^{2}\) |
Tesla squared / meters |
Magnetic pressure gradient |
||
|
\((\nabla |B|^{2})_{\rho}\) |
Tesla squared |
Covariant radial component of magnetic pressure gradient |
||
|
\((\nabla |B|^{2})_{\theta}\) |
Tesla squared |
Covariant poloidal component of magnetic pressure gradient |
||
|
\((\nabla |B|^{2})_{\zeta}\) |
Tesla squared |
Covariant toroidal component of magnetic pressure gradient |
||
|
\(X_{\mathrm{ballooning}}\) |
None |
Ideal ballooning eigenfunction |
||
|
\(\lambda_{\mathrm{ballooning}}=\gamma^2\) |
None |
Normalized squared ideal ballooning growth rate |
|
|
|
\(\iota\) |
None |
Rotational transform (normalized by 2pi) |
||
|
\(\iota~\mathrm{from~current}\) |
None |
Rotational transform (normalized by 2pi), current contribution |
||
|
\(\iota~\mathrm{in~vacuum}\) |
None |
Rotational transform (normalized by 2pi), vacuum contribution |
||
|
\(\iota_{\mathrm{denominator}}\) |
inverse meters |
Denominator of rotational transform formula |
||
|
\(\partial_{\rho} \iota_{\mathrm{denominator}}\) |
inverse meters |
Denominator of rotational transform formula, first radial derivative |
||
|
\(\partial_{\rho\rho} \iota_{\mathrm{denominator}}\) |
inverse meters |
Denominator of rotational transform formula, second radial derivative |
||
|
\(\partial_{\rho\rho\rho} \iota_{\mathrm{denominator}}\) |
inverse meters |
Denominator of rotational transform formula, third radial derivative |
||
|
\(\iota_{\mathrm{numerator}}\) |
inverse meters |
Numerator of rotational transform formula |
||
|
\(\iota_{\mathrm{numerator}}~\mathrm{from~current}\) |
inverse meters |
Numerator of rotational transform formula, current contribution |
||
|
\(\iota_{\mathrm{numerator}}~\mathrm{in~vacuum}\) |
inverse meters |
Numerator of rotational transform formula, vacuum contribution |
||
|
\(\partial_{\rho} \iota_{\mathrm{numerator}}\) |
inverse meters |
Numerator of rotational transform formula, first radial derivative |
||
|
\(\partial_{\rho} \iota_{\mathrm{numerator}}~\mathrm{from~current}\) |
inverse meters |
Numerator of rotational transform formula, current contribution, first radial derivative |
||
|
\(\partial_{\rho} \iota_{\mathrm{numerator}}~\mathrm{in~vacuum}\) |
inverse meters |
Numerator of rotational transform formula, vacuum contribution, first radial derivative |
||
|
\(\partial_{\rho\rho} \iota_{\mathrm{numerator}}\) |
inverse meters |
Numerator of rotational transform formula, second radial derivative |
||
|
\(\partial_{\rho\rho\rho} \iota_{\mathrm{numerator}}\) |
inverse meters |
Numerator of rotational transform formula, third radial derivative |
||
|
\(\partial_{\psi} \iota\) |
Inverse Webers |
Rotational transform, radial derivative wrt toroidal flux |
||
|
\(\partial_{\rho} \iota\) |
None |
Rotational transform (normalized by 2pi), first radial derivative |
||
|
\(\partial_{\rho\rho} \iota\) |
None |
Rotational transform (normalized by 2pi), second radial derivative |
||
|
\(1/|B|^2 (\mathbf{b} \times \nabla B) \cdot \nabla \psi\) |
None |
Measure of cross field drift at each point, unweighted by particle energy |
||
|
\(\kappa\) |
Inverse meters |
Curvature vector of magnetic field lines |
||
|
\(\kappa_g\) |
Inverse meters |
Geodesic curvature of magnetic field lines |
||
|
\(\kappa_n\) |
Inverse meters |
Normal curvature of magnetic field lines |
||
|
\(\lambda\) |
radians |
Poloidal stream function |
||
|
\(\partial_{\rho} \lambda\) |
radians |
Poloidal stream function, first radial derivative |
||
|
\(\partial_{\rho \rho} \lambda\) |
radians |
Poloidal stream function, second radial derivative |
||
|
\(\partial_{\rho \rho \rho} \lambda\) |
radians |
Poloidal stream function, third radial derivative |
||
|
\(\partial_{\rho \rho \rho \theta} \lambda\) |
radians |
Poloidal stream function, third radial derivative and first poloidal derivative |
|
|
|
\(\partial_{\rho \rho \rho \zeta} \lambda\) |
radians |
Poloidal stream function, third radial derivative and first toroidal derivative |
|
|
|
\(\partial_{\rho \rho \theta} \lambda\) |
radians |
Poloidal stream function, third derivative, wrt radius twice and poloidal angle |
|
|
|
\(\partial_{\rho \rho \zeta} \lambda\) |
radians |
Poloidal stream function, third derivative, wrt radius twice and toroidal angle |
|
|
|
\(\partial_{\rho \theta} \lambda\) |
radians |
Poloidal stream function, second derivative wrt radius and poloidal angle |
|
|
|
\(\partial_{\rho \theta \theta} \lambda\) |
radians |
Poloidal stream function, third derivative wrt radius and poloidal angle twice |
|
|
|
\(\partial_{\rho \theta \zeta} \lambda\) |
radians |
Poloidal stream function, third derivative wrt radius, poloidal angle, and toroidal angle |
|
|
|
\(\partial_{\rho \zeta} \lambda\) |
radians |
Poloidal stream function, second derivative wrt radius and toroidal angle |
|
|
|
\(\partial_{\rho \zeta \zeta} \lambda\) |
radians |
Poloidal stream function, third derivative wrt radius and toroidal angle twice |
|
|
|
\(\partial_{\theta} \lambda\) |
radians |
Poloidal stream function, first poloidal derivative |
||
|
\(\partial_{\theta \theta} \lambda\) |
radians |
Poloidal stream function, second poloidal derivative |
||
|
\(\partial_{\theta \theta \theta} \lambda\) |
radians |
Poloidal stream function, third poloidal derivative |
||
|
\(\partial_{\theta \theta \zeta} \lambda\) |
radians |
Poloidal stream function, third derivative wrt poloidal angle twice and toroidal angle |
|
|
|
\(\partial_{\theta \zeta} \lambda\) |
radians |
Poloidal stream function, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\theta \zeta \zeta} \lambda\) |
radians |
Poloidal stream function, third derivative wrt poloidal angle and toroidal angle twice |
|
|
|
\(\partial_{\zeta} \lambda\) |
radians |
Poloidal stream function, first toroidal derivative |
||
|
\(\partial_{\zeta \zeta} \lambda\) |
radians |
Poloidal stream function, second toroidal derivative |
||
|
\(\partial_{\zeta \zeta \zeta} \lambda\) |
radians |
Poloidal stream function, third toroidal derivative |
||
|
\(\mathrm{Magnetic~Well}\) |
None |
Magnetic well proxy for MHD stability (positive/negative value denotes stability/instability) |
||
|
\(\max_{\theta \zeta} |\mathbf{B}|\) |
Tesla |
Maximum field strength on each flux surface |
||
|
\(\min_{\theta \zeta} |\mathbf{B}|\) |
Tesla |
Minimum field strength on each flux surface |
||
|
\((B_{max} - B_{min}) / (B_{min} + B_{max})\) |
None |
Mirror ratio on each flux surface |
||
|
\(\hat{\mathbf{n}}_{\rho}\) |
None |
Unit vector normal to constant rho surface (direction of e^rho) |
||
|
\(\partial_{\zeta}\hat{\mathbf{n}}_{\rho}\) |
None |
Unit vector normal to constant rho surface (direction of e^rho), derivative wrt toroidal angle |
||
|
\(\hat{\mathbf{n}}_{\theta}\) |
None |
Unit vector normal to constant theta surface (direction of e^theta) |
||
|
\(\hat{\mathbf{n}}_{\zeta}\) |
None |
Unit vector normal to constant zeta surface (direction of e^zeta) |
||
|
\(n_e\) |
1 / cubic meters |
Electron density |
||
|
\(\partial_{\rho} n_e\) |
1 / cubic meters |
Electron density, first radial derivative |
||
|
\(\partial_{\rho \rho} n_e\) |
1 / cubic meters |
Electron density, second radial derivative |
||
|
\(n_i\) |
1 / cubic meters |
Ion density |
||
|
\(\partial_{\rho} n_i\) |
1 / cubic meters |
Ion density, first radial derivative |
||
|
\(\nu = \zeta_{B} - \zeta\) |
radians |
Boozer toroidal stream function |
||
|
\(\nu_{mn} = (\zeta_{B} - \zeta)_{mn}\) |
radians |
Boozer harmonics of Boozer toroidal stream function |
|
|
|
\(\partial_{\theta} \nu\) |
radians |
Boozer toroidal stream function, derivative wrt poloidal angle |
||
|
\(\partial_{\zeta} \nu\) |
radians |
Boozer toroidal stream function, derivative wrt toroidal angle |
||
|
\(\omega\) |
radians |
Toroidal stream function |
||
|
\(\partial_{\rho} \omega\) |
radians |
Toroidal stream function, first radial derivative |
||
|
\(\partial_{\rho \rho} \omega\) |
radians |
Toroidal stream function, second radial derivative |
||
|
\(\partial_{\rho \rho \rho} \omega\) |
radians |
Toroidal stream function, third radial derivative |
||
|
\(\partial_{\rho \rho \rho \rho} \omega\) |
radians |
Toroidal stream function, fourth radial derivative |
||
|
\(\partial_{\rho \rho \rho \theta} \omega\) |
radians |
Toroidal stream function, fourth derivative wrt radial coordinate thrice and poloidal once |
|
|
|
\(\partial_{\rho \rho \rho \zeta} \omega\) |
radians |
Toroidal stream function, fourth derivative wrt radial coordinate thrice and toroidal once |
|
|
|
\(\partial_{\rho \rho \theta} \omega\) |
radians |
Toroidal stream function, third derivative, wrt radius twice and poloidal angle |
|
|
|
\(\partial_{\rho \rho \theta \theta} \omega\) |
radians |
Toroidal stream function, fourth derivative, wrt radius twice and poloidal angle twice |
|
|
|
\(\partial_{\rho \theta \zeta} \omega\) |
radians |
Toroidal stream function, fourth derivative wrt radius twice, poloidal angle, and toroidal angle |
|
|
|
\(\partial_{\rho \rho \zeta} \omega\) |
radians |
Toroidal stream function, third derivative, wrt radius twice and toroidal angle |
|
|
|
\(\partial_{\rho \rho \zeta \zeta} \omega\) |
radians |
Toroidal stream function, fourth derivative, wrt radius twice and toroidal angle twice |
|
|
|
\(\partial_{\rho \theta} \omega\) |
radians |
Toroidal stream function, second derivative wrt radius and poloidal angle |
|
|
|
\(\partial_{\rho \theta \theta} \omega\) |
radians |
Toroidal stream function, third derivative wrt radius and poloidal angle twice |
|
|
|
\(\partial_{\rho \theta \theta \theta} \omega\) |
radians |
Toroidal stream function, third derivative wrt radius and poloidal angle thrice |
|
|
|
\(\partial_{\rho \theta \theta \zeta} \omega\) |
radians |
Toroidal stream function, fourth derivative wrt radius once, poloidal angle twice, and toroidal angle once |
|
|
|
\(\partial_{\rho \theta \zeta} \omega\) |
radians |
Toroidal stream function, third derivative wrt radius, poloidal angle, and toroidal angle |
|
|
|
\(\partial_{\rho \theta \zeta \zeta} \omega\) |
radians |
Toroidal stream function, fourth derivative wrt radius, poloidal angle, and toroidal angle twice |
|
|
|
\(\partial_{\rho \zeta} \omega\) |
radians |
Toroidal stream function, second derivative wrt radius and toroidal angle |
|
|
|
\(\partial_{\rho \zeta \zeta} \omega\) |
radians |
Toroidal stream function, third derivative wrt radius and toroidal angle twice |
|
|
|
\(\partial_{\rho \zeta \zeta \zeta} \omega\) |
radians |
Toroidal stream function, third derivative wrt radius and toroidal angle thrice |
|
|
|
\(\partial_{\theta} \omega\) |
radians |
Toroidal stream function, first poloidal derivative |
||
|
\(\partial_{\theta \theta} \omega\) |
radians |
Toroidal stream function, second poloidal derivative |
||
|
\(\partial_{\theta \theta \theta} \omega\) |
radians |
Toroidal stream function, third poloidal derivative |
||
|
\(\partial_{\theta \theta \zeta} \omega\) |
radians |
Toroidal stream function, third derivative wrt poloidal angle twice and toroidal angle |
|
|
|
\(\partial_{\theta \zeta} \omega\) |
radians |
Toroidal stream function, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\theta \zeta \zeta} \omega\) |
radians |
Toroidal stream function, third derivative wrt poloidal angle and toroidal angle twice |
|
|
|
\(\partial_{\zeta} \omega\) |
radians |
Toroidal stream function, first toroidal derivative |
||
|
\(\partial_{\zeta \zeta} \omega\) |
radians |
Toroidal stream function, second toroidal derivative |
||
|
\(\partial_{\zeta \zeta \zeta} \omega\) |
radians |
Toroidal stream function, third toroidal derivative |
||
|
\(p\) |
Pascals |
Pressure |
|
|
|
\(\partial_{\rho} p\) |
Pascals |
Pressure, first radial derivative |
||
|
\(\partial_{\theta} p\) |
Pascals |
Pressure, first poloidal derivative |
||
|
\(\partial_{\zeta} p\) |
Pascals |
Pressure, first toroidal derivative |
||
|
\(P(\zeta)\) |
meters |
Perimeter of enclosed cross-section (enclosed constant zeta surface), extrapolated to last closed flux surface |
||
|
\(\phi\) |
radians |
Toroidal angle in lab frame |
||
|
\(\partial_{\rho} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt radial coordinate |
||
|
\(\partial_{\rho \rho} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt radial coordinate |
||
|
\(\partial_{\rho \rho \zeta} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt radial coordinate and first wrt DESC toroidal coordinate |
|
|
|
\(\partial_{\rho \theta} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt radial and poloidal coordinate |
|
|
|
\(\partial_{\rho \theta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, third derivative wrt radial, poloidal, and toroidal coordinates |
|
|
|
\(\partial_{\rho \zeta} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt radial and toroidal coordinate |
|
|
|
\(\partial_{\rho \zeta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, first derivative wrt radial and second derivative wrt DESC toroidal coordinate |
|
|
|
\(\partial_{\theta} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt poloidal coordinate and first derivative wrt toroidal coordinate |
|
|
|
\(\partial_{\theta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt poloidal and toroidal coordinate |
|
|
|
\(\partial_{\theta \zeta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt poloidal coordinate and second derivative wrt toroidal coordinate |
|
|
|
\(\partial_{\zeta} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta \zeta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, third derivative wrt toroidal coordinate |
||
|
\(\psi = \Psi / (2 \pi)\) |
Webers |
Toroidal flux (normalized by 2pi) |
||
|
\(\partial_{\rho} \psi = \partial_{\rho} \Psi / (2 \pi)\) |
Webers |
Toroidal flux (normalized by 2pi), first radial derivative |
||
|
\(\psi' / \sqrt{g}\) |
Tesla / meter |
|||
|
\(\partial_{\rho\rho} \psi = \partial_{\rho\rho} \Psi / (2 \pi)\) |
Webers |
Toroidal flux (normalized by 2pi), second radial derivative |
||
|
\(\partial_{\rho\rho\rho} \psi = \partial_{\rho\rho\rho} \Psi / (2 \pi)\) |
Webers |
Toroidal flux (normalized by 2pi), third radial derivative |
||
|
\(q = 1/\iota\) |
None |
Safety factor ‘q’, inverse of rotational transform. |
||
|
\(\rho\) |
None |
Radial coordinate, proportional to the square root of the toroidal flux |
||
|
\(-\rho \frac{\partial_{\rho}\iota}{\iota}\) |
None |
Global magnetic shear |
||
|
\(\sqrt{g}\) |
cubic meters |
Jacobian determinant of flux coordinate system |
||
|
\(\sqrt{g}_Boozer\) |
cubic meters |
Jacobian determinant from (rho, theta_B, zeta_B) Boozer coordinates to (R,phi,Z) lab frame. |
||
|
\(\frac{\partial(\theta_B,\zeta_B)}{\theta_{DESC},\zeta_{DESC}}\) |
None |
Jacobian determinant from Boozer coordinates (rho, theta_B, zeta_B) to DESC coordinates (rho,theta,zeta). |
|
|
|
\(\sqrt{g}_{B,mn}\) |
cubic meters |
Boozer harmonics of Jacobian determinant from (rho, theta_B, zeta_B) Boozer coordinates to (R,phi,Z) lab frame. |
|
|
|
\(\sqrt{g}_{\text{Clebsch}}\) |
cubic meters |
Jacobian determinant of Clebsch field line coordinate system (ρ,α,ζ) where ζ is the DESC toroidal coordinate. |
||
|
\(\sqrt{g}_{PEST}\) |
cubic meters |
Jacobian determinant of (ρ,ϑ,ϕ) coordinate system or straight field line PEST coordinates. ϕ increases counterclockwise when viewed from above (cylindrical R,ϕ plane with Z out of page). |
||
|
\(\partial_{\rho} \sqrt{g}\) |
cubic meters |
Jacobian determinant of flux coordinate system, derivative wrt radial coordinate |
||
|
\(\partial_{\rho\rho} \sqrt{g}\) |
cubic meters |
Jacobian determinant of flux coordinate system, second derivative wrt radial coordinate |
||
|
\(\partial_{\rho\rho\rho} \sqrt{g}\) |
cubic meters |
Jacobian determinant of flux coordinate system, third derivative wrt radial coordinate |
||
|
\(\partial_{\rho\rho\theta} \sqrt{g}\) |
cubic meters |
Jacobian determinant of flux coordinate system, third derivative wrt radial coordinate twice and poloidal angle once |
|
|
|
\(\partial_{\rho\rho\zeta} \sqrt{g}\) |
cubic meters |
Jacobian determinant of flux coordinate system, third derivative wrt radial coordinate twice and toroidal angle once |
|
|
|
\(\partial_{\rho\theta} \sqrt{g}\) |
cubic meters |
Jacobian determinant of flux coordinate system, second derivative wrt radial coordinate and poloidal angle |
|
|
|
\(\partial_{\rho\theta\theta} \sqrt{g}\) |
cubic meters |
Jacobian determinant of flux coordinate system, third derivative wrt radial coordinate once and poloidal angle twice. |
|
|
|
\(\partial_{\rho\theta\zeta} \sqrt{g}\) |
cubic meters |
Jacobian determinant of flux coordinate system, third derivative wrt radial, poloidal, and toroidal coordinate |
|
|
|
\(\partial_{\rho\zeta} \sqrt{g}\) |
cubic meters |
Jacobian determinant of flux coordinate system, second derivative wrt radial coordinate and toroidal angle |
|
|
|
\(\partial_{\rho\zeta\zeta} \sqrt{g}\) |
cubic meters |
Jacobian determinant of flux coordinate system, third derivative wrt radial coordinate once and toroidal angle twice |
|
|
|
\(\partial_{\theta} \sqrt{g}\) |
cubic meters |
Jacobian determinant of flux coordinate system, derivative wrt poloidal angle |
||
|
\(\partial_{\theta\theta} \sqrt{g}\) |
cubic meters |
Jacobian determinant of flux coordinate system, second derivative wrt poloidal angle |
||
|
\(\partial_{\theta\zeta} \sqrt{g}\) |
cubic meters |
Jacobian determinant of flux coordinate system, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\zeta} \sqrt{g}\) |
cubic meters |
Jacobian determinant of flux coordinate system, derivative wrt toroidal angle |
||
|
\(\partial_{\zeta\zeta} \sqrt{g}\) |
cubic meters |
Jacobian determinant of flux coordinate system, second derivative wrt toroidal angle |
||
|
\(\theta\) |
radians |
Poloidal angular coordinate (geometric, not magnetic) |
||
|
\(\theta_{B}\) |
radians |
Boozer poloidal angular coordinate |
||
|
\(\vartheta\) |
radians |
PEST straight field line poloidal angular coordinate |
||
|
\(\partial_{\rho} \vartheta\) |
radians |
PEST straight field line poloidal angular coordinate, derivative wrt radial coordinate |
||
|
\(\partial_{\rho \rho} \vartheta\) |
radians |
PEST straight field line poloidal angular coordinate, derivative wrt radial coordinate, second order |
||
|
\(\partial_{\rho \rho \theta} \vartheta\) |
radians |
PEST straight field line poloidal angular coordinate, second derivative wrt radial coordinate and first derivative wrt DESC poloidal coordinate |
|
|
|
\(\partial_{\rho \theta} \vartheta\) |
radians |
PEST straight field line poloidal angular coordinate,derivative wrt poloidal and radial coordinate |
|
|
|
\(\partial_{\rho \theta \theta} \vartheta\) |
radians |
PEST straight field line poloidal angular coordinate, derivative wrt radial coordinate once and DESC poloidal coordinate twice |
|
|
|
\(\partial_{\rho \theta \zeta} \vartheta\) |
radians |
PEST straight field line poloidal angular coordinate, derivative wrt radial and DESC poloidal and toroidal coordinates |
|
|
|
\(\partial_{\rho \zeta} \vartheta\) |
radians |
PEST straight field line poloidal angular coordinate, derivative wrt radial and DESC toroidal coordinate |
|
|
|
\(\partial_{\theta} \vartheta\) |
radians |
PEST straight field line poloidal angular coordinate, derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta} \vartheta\) |
radians |
PEST straight field line poloidal angular coordinate,second derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta \theta} \vartheta\) |
radians |
PEST straight field line poloidal angular coordinate, third derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta \zeta} \vartheta\) |
radians |
PEST straight field line poloidal angular coordinate, second derivative wrt poloidal coordinate and derivative wrt toroidal coordinate |
|
|
|
\(\partial_{\theta \zeta} \vartheta\) |
radians |
PEST straight field line poloidal angular coordinate, derivative wrt poloidal and toroidal coordinates |
|
|
|
\(\partial_{\theta \zeta \zeta} \vartheta\) |
radians |
PEST straight field line poloidal angular coordinate, derivative wrt poloidal coordinate once and toroidal coordinate twice |
|
|
|
\(\partial_{\zeta} \vartheta\) |
radians |
PEST straight field line poloidal angular coordinate, derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta \zeta} \vartheta\) |
radians |
PEST straight field line poloidal angular coordinate, second derivative wrt toroidal coordinate |
||
|
\(1 - \frac{3}{4} \langle |B|^2 \rangle \int_0^{1/Bmax} \frac{\lambda\; d\lambda}{\langle \sqrt{1 - \lambda B} \rangle}\) |
None |
Neoclassical effective trapped particle fraction |
|
|
|
\(w_{\mathrm{Boozer}}\) |
Tesla * meters |
Inverse Fourier transform of RHS of eq 10 in Hirshman 1995 ‘Transformation from VMEC to Boozer Coordinates’ |
|
|
|
\(w_{\mathrm{Boozer},m,n}\) |
Tesla * meters |
RHS of eq 10 in Hirshman 1995 ‘Transformation from VMEC to Boozer Coordinates’ |
|
|
|
\(\partial_{\theta} w_{\mathrm{Boozer}}\) |
Tesla * meters |
Inverse Fourier transform of RHS of eq 10 in Hirshman 1995 ‘Transformation from VMEC to Boozer Coordinates’, poloidal derivative |
|
|
|
\(\partial_{\zeta} w_{\mathrm{Boozer}}\) |
Tesla * meters |
Inverse Fourier transform of RHS of eq 10 in Hirshman 1995 ‘Transformation from VMEC to Boozer Coordinates’, toroidal derivative |
|
|
|
\(\mathbf{x}\) |
not applicable |
Coordinate triplet. This is not a position vector unless basis is cartesian. When basis is cartesian, the units are meters. |
||
|
\(\zeta\) |
radians |
Toroidal angular coordinate |
||
|
\(\zeta_{B}\) |
radians |
Boozer toroidal angular coordinate |
||
|
\(|(\mathbf{B} \cdot \nabla) \mathbf{B}|\) |
Tesla squared / meters |
Magnitude of magnetic tension |
||
|
\(|\mathbf{B}|\) |
Tesla |
Magnitude of magnetic field |
||
|
\(|\mathbf{B}|^{2}\) |
Tesla squared |
Magnitude of magnetic field, squared |
||
|
\(\partial_{\alpha} (|\mathbf{B}|) |_{\rho, \zeta}\) |
Tesla |
Magnitude of magnetic field, derivative wrt field line angle |
||
|
\(B_{mn}^{\mathrm{Boozer}}\) |
Tesla |
Boozer harmonics of magnetic field |
|
|
|
\(\partial_{\rho} |\mathbf{B}|\) |
Tesla |
Magnitude of magnetic field, derivative wrt radial coordinate |
||
|
\(\partial_{\rho\rho} |\mathbf{B}|\) |
Tesla |
Magnitude of magnetic field, second derivative wrt radial coordinate |
||
|
\(\partial_{\rho\theta} |\mathbf{B}|\) |
Tesla |
Magnitude of magnetic field, derivative wrt radial coordinate and poloidal angle |
|
|
|
\(\partial_{\rho\zeta} |\mathbf{B}|\) |
Tesla |
Magnitude of magnetic field, derivative wrt radial coordinate and toroidal angle |
|
|
|
\(\partial_{\rho}|_{\vartheta, \phi} |\mathbf{B}|\) |
Tesla |
Magnetic field norm, derivative wrt ρ in (ρ, ϑ, ϕ) coordinates. |
||
|
\(\partial_{\theta} |\mathbf{B}|\) |
Tesla |
Magnitude of magnetic field, derivative wrt poloidal angle |
||
|
\(\partial_{\theta\theta} |\mathbf{B}|\) |
Tesla |
Magnitude of magnetic field, second derivative wrt poloidal angle |
||
|
\(\partial_{\theta\zeta} |\mathbf{B}|\) |
Tesla |
Magnitude of magnetic field, derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\zeta} |\mathbf{B}|\) |
Tesla |
Magnitude of magnetic field, derivative wrt toroidal angle |
||
|
\(\partial_{\zeta\zeta} |\mathbf{B}|\) |
Tesla |
Magnitude of magnetic field, second derivative wrt toroidal angle |
||
|
\(\partial_{\zeta} (|\mathbf{B}|) |_{\rho, \alpha}\) |
Tesla |
Magnitude of magnetic field, derivative along field line |
||
|
\(|\mathbf{J} \times \mathbf{B} - \nabla p|\) |
Newtons / cubic meter |
Magnitude of force balance error |
||
|
\(|\mathbf{J} \times \mathbf{B} - \nabla p|/\langle |\nabla |B|^{2}/(2\mu_0)| \rangle_{vol}\) |
None |
Magnitude of force balance error normalized by volume averaged magnetic pressure gradient |
||
|
\(|\mathbf{J}|\) |
Amperes / square meter |
Magnitude of plasma current density |
||
|
\(|\sqrt{g}(B^{\theta} \nabla \zeta - B^{\zeta} \nabla \theta)|\) |
Tesla * square meter |
Magnitude of helical basis vector weighted by 3-D volume Jacobian |
||
|
\(|B^{\theta} \nabla \zeta - B^{\zeta} \nabla \theta|\) |
Tesla / square meter |
Magnitude of helical basis vector |
||
|
\(|\mathbf{e}_{\alpha} |_{\rho, \phi}|\) |
meters |
Norm of covariant poloidal basis vector in (ρ, α, ϕ) Clebsch coordinates. |
||
|
\(|\mathbf{e}_{\rho} \times \mathbf{e}_{\alpha}|\) |
square meters |
2D Jacobian determinant for constant zeta surface in Clebsch field line coordinates (ρ,α,ζ) where ζ is the DESC toroidal coordinate. |
||
|
\(|\mathbf{e}_{\rho} \times \mathbf{e}_{\theta}|\) |
square meters |
2D Jacobian determinant for constant zeta surface |
||
|
\(\partial_{\rho} |\mathbf{e}_{\rho} \times \mathbf{e}_{\theta}|\) |
square meters |
2D Jacobian determinant for constant zeta surface derivative wrt radial coordinate |
||
|
\(\partial_{\rho \rho} |\mathbf{e}_{\rho} \times \mathbf{e}_{\theta}|\) |
square meters |
2D Jacobian determinant for constant zeta surface second derivative wrt radial coordinate |
||
|
\(| \mathbf{e}_{\theta} \times \mathbf{e}_{\zeta} |\) |
square meters |
2D Jacobian determinant for constant rho surface |
||
|
\(\partial_{\rho} |\mathbf{e}_{\theta} \times \mathbf{e}_{\zeta}|\) |
square meters |
2D Jacobian determinant for constant rho surface derivative wrt radial coordinate |
||
|
\(\partial_{\rho\rho}|\mathbf{e}_{\theta}\times\mathbf{e}_{\zeta}|\) |
square meters |
2D Jacobian determinant for constant rho surface second derivative wrt radial coordinate |
||
|
\(\partial_{\zeta}|\mathbf{e}_{\theta} \times \mathbf{e}_{\zeta}|\) |
square meters |
2D Jacobian determinant for constant rho surface,derivative wrt toroidal angle |
||
|
\(|\mathbf{e}_{\zeta} \times \mathbf{e}_{\rho}|\) |
square meters |
2D Jacobian determinant for constant theta surface |
||
|
\(|\mathbf{e}_{\zeta} |_{\rho, \alpha}| = \frac{|\mathbf{B}|}{|\mathbf{B} \cdot \nabla \zeta|}\) |
meters |
Differential length along field line |
||
|
\(\partial_{\zeta} |\mathbf{e}_{\zeta} |_{\rho, \alpha}| |_{\rho, \alpha}\) |
meters |
Differential length along field line, derivative along field line |
||
|
\(|\nabla \mathbf{B}|\) |
Tesla / meter |
Frobenius norm of gradient of magnetic field vector |
||
|
\(|\nabla p|\) |
Newtons per cubic meter |
Magnitude of pressure gradient |
||
|
\(|\nabla p|^{2}\) |
Newtons per cubic meter squared |
Magnitude of pressure gradient squared |
||
|
\(|\nabla\psi|\) |
Webers per meter |
Toroidal flux gradient (normalized by 2pi) magnitude |
||
|
\(|\nabla\psi|^{2}\) |
Webers squared per square meter |
Toroidal flux gradient (normalized by 2pi) magnitude squared |
||
|
\(|\nabla \rho|\) |
inverse meters |
Magnitude of contravariant radial basis vector |
||
|
\(|\nabla \theta|\) |
inverse meters |
Magnitude of contravariant poloidal basis vector |
||
|
\(|\nabla \zeta|\) |
inverse meters |
Magnitude of contravariant toroidal basis vector |
||
|
\(|\nabla |B|^{2}|/(2\mu_0)\) |
Newton / cubic meter |
Magnitude of magnetic pressure gradient |
desc.geometry.curve.FourierRZCurve
Name |
Label |
Units |
Description |
Aliases |
kwargs |
|---|---|---|---|---|---|
|
\(0\) |
None |
Zeros |
|
|
|
\(1\) |
None |
Ones |
|
|
|
\(R\) |
meters |
Cylindrical radial position along curve |
||
|
\(X\) |
meters |
Cartesian X coordinate. |
||
|
\(Y\) |
meters |
Cartesian Y coordinate. |
||
|
\(Z\) |
meters |
Cylindrical vertical position along curve |
||
|
\(\langle\mathbf{x}\rangle\) |
meters |
Centroid of the curve |
||
|
\(\kappa\) |
Inverse meters |
Scalar curvature of the curve, with the sign denoting the convexity/concavity relative to the center of the curve (a circle has positive curvature) |
||
|
\(ds\) |
None |
Quadrature weights for integration along the curve, i.e. an alias for |
||
|
\(\mathbf{B}_{\mathrm{Frenet-Serret}}\) |
None |
Binormal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{N}_{\mathrm{Frenet-Serret}}\) |
None |
Normal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{T}_{\mathrm{Frenet-Serret}}\) |
None |
Tangent unit vector to curve in Frenet-Serret frame |
||
|
\(L\) |
meters |
Length of the curve |
||
|
\(\phi\) |
radians |
Toroidal phi position along curve |
||
|
\(s\) |
None |
Curve parameter, on [0, 2pi) |
||
|
\(\tau\) |
Inverse meters |
Scalar torsion of the curve |
||
|
\(\mathbf{x}\) |
not applicable |
Coordinate triplet. This is not a position vector unless basis is cartesian. When basis is cartesian, the units are meters. |
||
|
\(\partial_{s} \mathbf{x}\) |
meters |
Position vector along curve, first derivative |
||
|
\(\partial_{ss} \mathbf{x}\) |
meters |
Position vector along curve, second derivative |
||
|
\(\partial_{sss} \mathbf{x}\) |
meters |
Position vector along curve, third derivative |
desc.geometry.curve.FourierXYZCurve
Name |
Label |
Units |
Description |
Aliases |
kwargs |
|---|---|---|---|---|---|
|
\(0\) |
None |
Zeros |
|
|
|
\(1\) |
None |
Ones |
|
|
|
\(R\) |
meters |
Cylindrical radial position along curve |
||
|
\(X\) |
meters |
Cartesian X coordinate. |
||
|
\(Y\) |
meters |
Cartesian Y coordinate. |
||
|
\(Z\) |
meters |
Cylindrical vertical position along curve |
||
|
\(\langle\mathbf{x}\rangle\) |
meters |
Centroid of the curve |
||
|
\(\kappa\) |
Inverse meters |
Scalar curvature of the curve, with the sign denoting the convexity/concavity relative to the center of the curve (a circle has positive curvature) |
||
|
\(ds\) |
None |
Quadrature weights for integration along the curve, i.e. an alias for |
||
|
\(\mathbf{B}_{\mathrm{Frenet-Serret}}\) |
None |
Binormal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{N}_{\mathrm{Frenet-Serret}}\) |
None |
Normal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{T}_{\mathrm{Frenet-Serret}}\) |
None |
Tangent unit vector to curve in Frenet-Serret frame |
||
|
\(L\) |
meters |
Length of the curve |
||
|
\(\phi\) |
radians |
Toroidal phi position along curve |
||
|
\(s\) |
None |
Curve parameter, on [0, 2pi) |
||
|
\(\tau\) |
Inverse meters |
Scalar torsion of the curve |
||
|
\(\mathbf{x}\) |
not applicable |
Coordinate triplet. This is not a position vector unless basis is cartesian. When basis is cartesian, the units are meters. |
||
|
\(\partial_{s} \mathbf{x}\) |
meters |
Position vector along curve, first derivative |
||
|
\(\partial_{ss} \mathbf{x}\) |
meters |
Position vector along curve, second derivative |
||
|
\(\partial_{sss} \mathbf{x}\) |
meters |
Position vector along curve, third derivative |
desc.geometry.curve.FourierPlanarCurve
Name |
Label |
Units |
Description |
Aliases |
kwargs |
|---|---|---|---|---|---|
|
\(0\) |
None |
Zeros |
|
|
|
\(1\) |
None |
Ones |
|
|
|
\(R\) |
meters |
Cylindrical radial position along curve |
||
|
\(X\) |
meters |
Cartesian X coordinate. |
||
|
\(Y\) |
meters |
Cartesian Y coordinate. |
||
|
\(Z\) |
meters |
Cylindrical vertical position along curve |
||
|
\(\langle\mathbf{x}\rangle\) |
meters |
Centroid of the curve |
|
|
|
\(\kappa\) |
Inverse meters |
Scalar curvature of the curve, with the sign denoting the convexity/concavity relative to the center of the curve (a circle has positive curvature) |
||
|
\(ds\) |
None |
Quadrature weights for integration along the curve, i.e. an alias for |
||
|
\(\mathbf{B}_{\mathrm{Frenet-Serret}}\) |
None |
Binormal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{N}_{\mathrm{Frenet-Serret}}\) |
None |
Normal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{T}_{\mathrm{Frenet-Serret}}\) |
None |
Tangent unit vector to curve in Frenet-Serret frame |
||
|
\(L\) |
meters |
Length of the curve |
||
|
\(\phi\) |
radians |
Toroidal phi position along curve |
||
|
\(s\) |
None |
Curve parameter, on [0, 2pi) |
||
|
\(\tau\) |
Inverse meters |
Scalar torsion of the curve |
||
|
\(\mathbf{x}\) |
not applicable |
Coordinate triplet. This is not a position vector unless basis is cartesian. When basis is cartesian, the units are meters. |
|
|
|
\(\partial_{s} \mathbf{x}\) |
meters |
Position vector along curve, first derivative |
|
|
|
\(\partial_{ss} \mathbf{x}\) |
meters |
Position vector along curve, second derivative |
|
|
|
\(\partial_{sss} \mathbf{x}\) |
meters |
Position vector along curve, third derivative |
|
desc.geometry.curve.FourierXYCurve
Name |
Label |
Units |
Description |
Aliases |
kwargs |
|---|---|---|---|---|---|
|
\(0\) |
None |
Zeros |
|
|
|
\(1\) |
None |
Ones |
|
|
|
\(R\) |
meters |
Cylindrical radial position along curve |
||
|
\(X\) |
meters |
Cartesian X coordinate. |
||
|
\(Y\) |
meters |
Cartesian Y coordinate. |
||
|
\(Z\) |
meters |
Cylindrical vertical position along curve |
||
|
\(\langle\mathbf{x}\rangle\) |
meters |
Centroid of the curve |
|
|
|
\(\kappa\) |
Inverse meters |
Scalar curvature of the curve, with the sign denoting the convexity/concavity relative to the center of the curve (a circle has positive curvature) |
||
|
\(ds\) |
None |
Quadrature weights for integration along the curve, i.e. an alias for |
||
|
\(\mathbf{B}_{\mathrm{Frenet-Serret}}\) |
None |
Binormal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{N}_{\mathrm{Frenet-Serret}}\) |
None |
Normal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{T}_{\mathrm{Frenet-Serret}}\) |
None |
Tangent unit vector to curve in Frenet-Serret frame |
||
|
\(L\) |
meters |
Length of the curve |
||
|
\(\phi\) |
radians |
Toroidal phi position along curve |
||
|
\(s\) |
None |
Curve parameter, on [0, 2pi) |
||
|
\(\tau\) |
Inverse meters |
Scalar torsion of the curve |
||
|
\(\mathbf{x}\) |
not applicable |
Coordinate triplet. This is not a position vector unless basis is cartesian. When basis is cartesian, the units are meters. |
|
|
|
\(\partial_{s} \mathbf{x}\) |
meters |
Position vector along curve, first derivative |
|
|
|
\(\partial_{ss} \mathbf{x}\) |
meters |
Position vector along curve, second derivative |
|
|
|
\(\partial_{sss} \mathbf{x}\) |
meters |
Position vector along curve, third derivative |
|
desc.geometry.curve.SplineXYZCurve
Name |
Label |
Units |
Description |
Aliases |
kwargs |
|---|---|---|---|---|---|
|
\(0\) |
None |
Zeros |
|
|
|
\(1\) |
None |
Ones |
|
|
|
\(R\) |
meters |
Cylindrical radial position along curve |
||
|
\(X\) |
meters |
Cartesian X coordinate. |
||
|
\(Y\) |
meters |
Cartesian Y coordinate. |
||
|
\(Z\) |
meters |
Cylindrical vertical position along curve |
||
|
\(\langle\mathbf{x}\rangle\) |
meters |
Centroid of the curve |
||
|
\(\kappa\) |
Inverse meters |
Scalar curvature of the curve, with the sign denoting the convexity/concavity relative to the center of the curve (a circle has positive curvature) |
||
|
\(ds\) |
None |
Quadrature weights for integration along the curve, i.e. an alias for |
||
|
\(\mathbf{B}_{\mathrm{Frenet-Serret}}\) |
None |
Binormal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{N}_{\mathrm{Frenet-Serret}}\) |
None |
Normal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{T}_{\mathrm{Frenet-Serret}}\) |
None |
Tangent unit vector to curve in Frenet-Serret frame |
||
|
\(L\) |
meters |
Length of the curve |
|
|
|
\(\phi\) |
radians |
Toroidal phi position along curve |
||
|
\(s\) |
None |
Curve parameter, on [0, 2pi) |
||
|
\(\tau\) |
Inverse meters |
Scalar torsion of the curve |
||
|
\(\mathbf{x}\) |
not applicable |
Coordinate triplet. This is not a position vector unless basis is cartesian. When basis is cartesian, the units are meters. |
|
|
|
\(\partial_{s} \mathbf{x}\) |
meters |
Position vector along curve, first derivative |
|
|
|
\(\partial_{ss} \mathbf{x}\) |
meters |
Position vector along curve, second derivative |
|
|
|
\(\partial_{sss} \mathbf{x}\) |
meters |
Position vector along curve, third derivative |
|
desc.geometry.surface.FourierRZToroidalSurface
Name |
Label |
Units |
Description |
Aliases |
kwargs |
|---|---|---|---|---|---|
|
\(0\) |
None |
Zeros |
|
|
|
\(1\) |
None |
Ones |
|
|
|
\(A\) |
square meters |
Average enclosed cross-sectional (constant zeta surface) area |
||
|
\(A(\rho)\) |
square meters |
Average area of enclosed cross-section (enclosed constant zeta surface), as function of rho |
||
|
\(A(\zeta)\) |
square meters |
Area of enclosed cross-section (enclosed constant zeta surface) |
||
|
\(L_{\mathrm{SFF},\rho}\) |
meters |
L coefficient of second fundamental form of constant rho surface |
||
|
\(M_{\mathrm{SFF},\rho}\) |
meters |
M coefficient of second fundamental form of constant rho surface |
||
|
\(N_{\mathrm{SFF},\rho}\) |
meters |
N coefficient of second fundamental form of constant rho surface |
||
|
\(R\) |
meters |
Major radius in lab frame |
||
|
\(R_{0} = V / (2\pi A) = \int R(\rho=0) d\zeta / (2\pi)\) |
meters |
Average major radius |
||
|
\(R_{0} / a\) |
None |
Aspect ratio |
||
|
\(\partial_{\theta} R\) |
meters |
Major radius in lab frame, first poloidal derivative |
||
|
\(\partial_{\theta \theta} R\) |
meters |
Major radius in lab frame, second poloidal derivative |
||
|
\(\partial_{\theta \theta \theta} R\) |
meters |
Major radius in lab frame, third poloidal derivative |
||
|
\(\partial_{\theta \theta \zeta} R\) |
meters |
Major radius in lab frame, third derivative wrt poloidal angle twice and toroidal angle |
|
|
|
\(\partial_{\theta \zeta} R\) |
meters |
Major radius in lab frame, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\theta \zeta \zeta} R\) |
meters |
Major radius in lab frame, third derivative wrt poloidal angle and toroidal angle twice |
|
|
|
\(\partial_{\zeta} R\) |
meters |
Major radius in lab frame, first toroidal derivative |
||
|
\(\partial_{\zeta \zeta} R\) |
meters |
Major radius in lab frame, second toroidal derivative |
||
|
\(\partial_{\zeta \zeta \zeta} R\) |
meters |
Major radius in lab frame, third toroidal derivative |
||
|
\(S\) |
square meters |
Surface area |
||
|
\(S(\rho)\) |
square meters |
Surface area of flux surfaces |
||
|
\(V\) |
cubic meters |
Volume enclosed by surface |
||
|
\(V(\rho)\) |
cubic meters |
Volume enclosed by flux surfaces |
||
|
\(X = R \cos{\phi}\) |
meters |
Cartesian X coordinate |
||
|
\(Y = R \sin{\phi}\) |
meters |
Cartesian Y coordinate |
||
|
\(Z\) |
meters |
Vertical coordinate in lab frame |
||
|
\(\partial_{\theta} Z\) |
meters |
Vertical coordinate in lab frame, first poloidal derivative |
||
|
\(\partial_{\theta \theta} Z\) |
meters |
Vertical coordinate in lab frame, second poloidal derivative |
||
|
\(\partial_{\theta \theta \theta} Z\) |
meters |
Vertical coordinate in lab frame, third poloidal derivative |
||
|
\(\partial_{\theta \theta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative wrt poloidal angle twice and toroidal angle |
|
|
|
\(\partial_{\theta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\theta \zeta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative wrt poloidal angle and toroidal angle twice |
|
|
|
\(\partial_{\zeta} Z\) |
meters |
Vertical coordinate in lab frame, first toroidal derivative |
||
|
\(\partial_{\zeta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, second toroidal derivative |
||
|
\(\partial_{\zeta \zeta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, third toroidal derivative |
||
|
\(a\) |
meters |
Average minor radius |
||
|
\(a_{\mathrm{major}} / a_{\mathrm{minor}}\) |
None |
Elongation at a toroidal cross-section (constant zeta surface) |
||
|
\(H_{\rho}\) |
inverse meters |
Mean curvature of constant rho surfaces |
||
|
\(K_{\rho}\) |
inverse meters squared |
Gaussian curvature of constant rho surfaces |
||
|
\(k_{1,\rho}\) |
inverse meters |
First principle curvature of constant rho surfaces |
||
|
\(k_{2,\rho}\) |
inverse meters |
Second principle curvature of constant rho surfaces |
||
|
\(\mathbf{e}_{\phi} |_{\rho, \theta}\) |
meters |
Covariant toroidal basis vector in (ρ,θ,ϕ) coordinates |
|
|
|
\(\mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector |
||
|
\(\partial_{\theta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, second derivative wrt poloidal and poloidal coordinates |
||
|
\(\partial_{\theta \zeta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, second derivative wrt poloidal and toroidal coordinates |
|
|
|
\(\partial_{\zeta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, derivative wrt toroidal coordinate |
|
|
|
\(\partial_{\zeta \zeta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, second derivative wrt toroidal and toroidal coordinates |
|
|
|
\(\mathbf{e}_{\theta} |_{\rho, \phi}\) |
meters |
Covariant poloidal basis vector in (ρ,θ,ϕ) coordinates. ϕ increases counterclockwise when viewed from above (cylindrical R,ϕ plane with Z out of page). |
||
|
\(\mathbf{e}_{\zeta}\) |
meters |
Covariant Toroidal basis vector |
||
|
\(\partial_{\zeta} \mathbf{e}_{\zeta}\) |
meters |
Covariant Toroidal basis vector, derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta \zeta} \mathbf{e}_{\zeta}\) |
meters |
Covariant Toroidal basis vector, second derivative wrt toroidal and toroidal coordinates |
||
|
\(g_{\theta\theta}\) |
square meters |
Poloidal/Poloidal element of covariant metric tensor |
||
|
\(g_{\theta\zeta}\) |
square meters |
Poloidal/Toroidal element of covariant metric tensor |
|
|
|
\(g_{\zeta\zeta}\) |
square meters |
Toroidal/Toroidal element of covariant metric tensor |
||
|
\(\nabla \phi\) |
Inverse meters |
Gradient of cylindrical toroidal angle ϕ. |
||
|
\(\hat{\mathbf{n}}_{\rho}\) |
None |
Unit vector normal to constant rho surface (direction of e^rho) |
||
|
\(\partial_{\zeta}\hat{\mathbf{n}}_{\rho}\) |
None |
Unit vector normal to constant rho surface (direction of e^rho), derivative wrt toroidal angle |
||
|
\(\omega\) |
radians |
Toroidal stream function |
||
|
\(\partial_{\rho} \omega\) |
radians |
Toroidal stream function, first radial derivative |
||
|
\(\partial_{\theta} \omega\) |
radians |
Toroidal stream function, first poloidal derivative |
||
|
\(\partial_{\theta \theta} \omega\) |
radians |
Toroidal stream function, second poloidal derivative |
||
|
\(\partial_{\theta \theta \theta} \omega\) |
radians |
Toroidal stream function, third poloidal derivative |
||
|
\(\partial_{\theta \theta \zeta} \omega\) |
radians |
Toroidal stream function, third derivative wrt poloidal angle twice and toroidal angle |
|
|
|
\(\partial_{\theta \zeta} \omega\) |
radians |
Toroidal stream function, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\theta \zeta \zeta} \omega\) |
radians |
Toroidal stream function, third derivative wrt poloidal angle and toroidal angle twice |
|
|
|
\(\partial_{\zeta} \omega\) |
radians |
Toroidal stream function, first toroidal derivative |
||
|
\(\partial_{\zeta \zeta} \omega\) |
radians |
Toroidal stream function, second toroidal derivative |
||
|
\(\partial_{\zeta \zeta \zeta} \omega\) |
radians |
Toroidal stream function, third toroidal derivative |
||
|
\(P(\zeta)\) |
meters |
Perimeter of enclosed cross-section (enclosed constant zeta surface) |
||
|
\(\phi\) |
radians |
Toroidal angle in lab frame |
||
|
\(\partial_{\rho} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt radial coordinate |
||
|
\(\partial_{\theta} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt poloidal coordinate and first derivative wrt toroidal coordinate |
|
|
|
\(\partial_{\theta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt poloidal and toroidal coordinate |
|
|
|
\(\partial_{\theta \zeta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt poloidal coordinate and second derivative wrt toroidal coordinate |
|
|
|
\(\partial_{\zeta} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta \zeta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, third derivative wrt toroidal coordinate |
||
|
\(\rho\) |
None |
Radial coordinate, proportional to the square root of the toroidal flux |
||
|
\(\theta\) |
radians |
Poloidal angular coordinate (geometric, not magnetic) |
||
|
\(\mathbf{x}\) |
not applicable |
Coordinate triplet. This is not a position vector unless basis is cartesian. When basis is cartesian, the units are meters. |
||
|
\(\zeta\) |
radians |
Toroidal angular coordinate |
||
|
\(| \mathbf{e}_{\theta} \times \mathbf{e}_{\zeta} |\) |
square meters |
2D Jacobian determinant for constant rho surface |
||
|
\(\partial_{\zeta}|\mathbf{e}_{\theta} \times \mathbf{e}_{\zeta}|\) |
square meters |
2D Jacobian determinant for constant rho surface,derivative wrt toroidal angle |
desc.geometry.surface.ZernikeRZToroidalSection
Name |
Label |
Units |
Description |
Aliases |
kwargs |
|---|---|---|---|---|---|
|
\(0\) |
None |
Zeros |
|
|
|
\(1\) |
None |
Ones |
|
|
|
\(A\) |
square meters |
Average enclosed cross-sectional (constant zeta surface) area, extrapolated to last closed flux surface |
||
|
\(A(\zeta)\) |
square meters |
Area of enclosed cross-section (enclosed constant zeta surface), extrapolated to last closed flux surface |
||
|
\(L_{\mathrm{SFF},\zeta}\) |
meters |
L coefficient of second fundamental form of constant zeta surface |
||
|
\(M_{\mathrm{SFF},\zeta}\) |
meters |
M coefficient of second fundamental form of constant zeta surface |
||
|
\(N_{\mathrm{SFF},\zeta}\) |
meters |
N coefficient of second fundamental form of constant zeta surface |
||
|
\(R\) |
meters |
Major radius in lab frame |
||
|
\(\partial_{\rho} R\) |
meters |
Major radius in lab frame, first radial derivative |
||
|
\(\partial_{\rho \rho} R\) |
meters |
Major radius in lab frame, second radial derivative |
||
|
\(\partial_{\rho \rho \rho} R\) |
meters |
Major radius in lab frame, third radial derivative |
||
|
\(\partial_{\rho \rho \rho \rho} R\) |
meters |
Major radius in lab frame, fourth radial derivative |
||
|
\(\partial_{\rho \rho \rho \theta} R\) |
meters |
Major radius in lab frame, fourth derivative wrt radial coordinate thrice and poloidal once |
|
|
|
\(\partial_{\rho \rho \theta} R\) |
meters |
Major radius in lab frame, third derivative, wrt radius twice and poloidal angle |
|
|
|
\(\partial_{\rho \rho \theta \theta} R\) |
meters |
Major radius in lab frame, fourth derivative, wrt radius twice and poloidal angle twice |
|
|
|
\(\partial_{\rho \rho \theta \zeta} R\) |
meters |
Major radius in lab frame, fourth derivative wrt radius twice, poloidal angle, and toroidal angle |
|
|
|
\(\partial_{\rho \theta} R\) |
meters |
Major radius in lab frame, second derivative wrt radius and poloidal angle |
|
|
|
\(\partial_{\rho \theta \theta} R\) |
meters |
Major radius in lab frame, third derivative wrt radius and poloidal angle twice |
|
|
|
\(\partial_{\rho \theta \theta \theta} R\) |
meters |
Major radius in lab frame, fourth derivative wrt radius and poloidal angle thrice |
|
|
|
\(\partial_{\theta} R\) |
meters |
Major radius in lab frame, first poloidal derivative |
||
|
\(\partial_{\theta \theta} R\) |
meters |
Major radius in lab frame, second poloidal derivative |
||
|
\(\partial_{\theta \theta \theta} R\) |
meters |
Major radius in lab frame, third poloidal derivative |
||
|
\(X = R \cos{\phi}\) |
meters |
Cartesian X coordinate |
||
|
\(Y = R \sin{\phi}\) |
meters |
Cartesian Y coordinate |
||
|
\(Z\) |
meters |
Vertical coordinate in lab frame |
||
|
\(\partial_{\rho} Z\) |
meters |
Vertical coordinate in lab frame, first radial derivative |
||
|
\(\partial_{\rho \rho} Z\) |
meters |
Vertical coordinate in lab frame, second radial derivative |
||
|
\(\partial_{\rho \rho \rho} Z\) |
meters |
Vertical coordinate in lab frame, third radial derivative |
||
|
\(\partial_{\rho \rho \rho \rho} Z\) |
meters |
Vertical coordinate in lab frame, fourth radial derivative |
||
|
\(\partial_{\rho \rho \rho \theta} Z\) |
meters |
Vertical coordinate in lab frame, fourth derivative wrt radial coordinate thrice and poloidal once |
|
|
|
\(\partial_{\rho \rho \theta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative, wrt radius twice and poloidal angle |
|
|
|
\(\partial_{\rho \rho \theta} Z\) |
meters |
Vertical coordinate in lab frame, fourth derivative, wrt radius twice and poloidal angle twice |
|
|
|
\(\partial_{\rho \theta} Z\) |
meters |
Vertical coordinate in lab frame, second derivative wrt radius and poloidal angle |
|
|
|
\(\partial_{\rho \theta \theta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative wrt radius and poloidal angle twice |
|
|
|
\(\partial_{\rho \theta \theta \theta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative wrt radius and poloidal angle thrice |
|
|
|
\(\partial_{\theta} Z\) |
meters |
Vertical coordinate in lab frame, first poloidal derivative |
||
|
\(\partial_{\theta \theta} Z\) |
meters |
Vertical coordinate in lab frame, second poloidal derivative |
||
|
\(\partial_{\theta \theta \theta} Z\) |
meters |
Vertical coordinate in lab frame, third poloidal derivative |
||
|
\(a\) |
meters |
Average minor radius |
||
|
\(a_{\mathrm{major}} / a_{\mathrm{minor}}\) |
None |
Elongation at a toroidal cross-section (constant zeta surface), extrapolated to last closed flux surface. |
||
|
\(H_{\zeta}\) |
inverse meters |
Mean curvature of constant zeta surfaces |
||
|
\(K_{\zeta}\) |
inverse meters squared |
Gaussian curvature of constant zeta surfaces |
||
|
\(k_{1,\zeta}\) |
inverse meters |
First principle curvature of constant zeta surfaces |
||
|
\(k_{2,\zeta}\) |
inverse meters |
Second principle curvature of constant zeta surfaces |
||
|
\(\mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector |
||
|
\(\partial_{\rho} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, derivative wrt radial coordinate |
||
|
\(\partial_{\rho \rho} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, second derivative wrt radial and radial coordinates |
||
|
\(\partial_{\rho \rho \rho} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, third derivative wrt radial coordinate |
||
|
\(\partial_{\rho \rho \theta} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, third derivative wrt radial coordinate twice and poloidal once |
|
|
|
\(\partial_{\rho \theta} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, second derivative wrt radial and poloidal coordinates |
|
|
|
\(\partial_{\rho \theta \theta} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, third derivative wrt radial coordinateonce and poloidal twice |
|
|
|
\(\partial_{\theta} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, derivative wrt poloidal coordinate |
|
|
|
\(\partial_{\theta \theta} \mathbf{e}_{\rho}\) |
meters |
Covariant Radial basis vector, second derivative wrt poloidal and poloidal coordinates |
|
|
|
\(\mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector |
||
|
\(\partial_{\rho \theta \theta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, third derivative wrt radial coordinate once and poloidal twice |
|
|
|
\(\partial_{\theta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, second derivative wrt poloidal and poloidal coordinates |
||
|
\(g_{\rho\rho}\) |
square meters |
Radial/Radial element of covariant metric tensor |
||
|
\(g_{\rho\theta}\) |
square meters |
Radial/Poloidal element of covariant metric tensor |
|
|
|
\(g_{\theta\theta}\) |
square meters |
Poloidal/Poloidal element of covariant metric tensor |
||
|
\(\partial_{\rho} g_{\theta\theta}\) |
square meters |
Poloidal/Poloidal element of covariant metric tensor, derivative wrt rho |
||
|
\(\nabla \phi\) |
Inverse meters |
Gradient of cylindrical toroidal angle ϕ. |
||
|
\(\hat{\mathbf{n}}_{\zeta}\) |
None |
Unit vector normal to constant zeta surface (direction of e^zeta) |
||
|
\(\omega\) |
radians |
Toroidal stream function |
||
|
\(\partial_{\rho} \omega\) |
radians |
Toroidal stream function, first radial derivative |
||
|
\(\partial_{\rho \rho} \omega\) |
radians |
Toroidal stream function, second radial derivative |
||
|
\(\partial_{\rho \rho \rho} \omega\) |
radians |
Toroidal stream function, third radial derivative |
||
|
\(\partial_{\rho \rho \rho \rho} \omega\) |
radians |
Toroidal stream function, fourth radial derivative |
||
|
\(\partial_{\rho \rho \rho \theta} \omega\) |
radians |
Toroidal stream function, fourth derivative wrt radial coordinate thrice and poloidal once |
|
|
|
\(\partial_{\rho \rho \theta} \omega\) |
radians |
Toroidal stream function, third derivative, wrt radius twice and poloidal angle |
|
|
|
\(\partial_{\rho \rho \theta \theta} \omega\) |
radians |
Toroidal stream function, fourth derivative, wrt radius twice and poloidal angle twice |
|
|
|
\(\partial_{\rho \theta} \omega\) |
radians |
Toroidal stream function, second derivative wrt radius and poloidal angle |
|
|
|
\(\partial_{\rho \theta \theta} \omega\) |
radians |
Toroidal stream function, third derivative wrt radius and poloidal angle twice |
|
|
|
\(\partial_{\rho \theta \theta \theta} \omega\) |
radians |
Toroidal stream function, third derivative wrt radius and poloidal angle thrice |
|
|
|
\(\partial_{\theta} \omega\) |
radians |
Toroidal stream function, first poloidal derivative |
||
|
\(\partial_{\theta \theta} \omega\) |
radians |
Toroidal stream function, second poloidal derivative |
||
|
\(\partial_{\theta \theta \theta} \omega\) |
radians |
Toroidal stream function, third poloidal derivative |
||
|
\(P(\zeta)\) |
meters |
Perimeter of enclosed cross-section (enclosed constant zeta surface), extrapolated to last closed flux surface |
||
|
\(\phi\) |
radians |
Toroidal angle in lab frame |
||
|
\(\partial_{\rho} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt radial coordinate |
||
|
\(\partial_{\rho \rho} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt radial coordinate |
||
|
\(\partial_{\rho \theta} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt radial and poloidal coordinate |
|
|
|
\(\partial_{\theta} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt poloidal coordinate |
||
|
\(\rho\) |
None |
Radial coordinate, proportional to the square root of the toroidal flux |
||
|
\(\theta\) |
radians |
Poloidal angular coordinate (geometric, not magnetic) |
||
|
\(\mathbf{x}\) |
not applicable |
Coordinate triplet. This is not a position vector unless basis is cartesian. When basis is cartesian, the units are meters. |
||
|
\(\zeta\) |
radians |
Toroidal angular coordinate |
||
|
\(|\mathbf{e}_{\rho} \times \mathbf{e}_{\theta}|\) |
square meters |
2D Jacobian determinant for constant zeta surface |
||
|
\(\partial_{\rho} |\mathbf{e}_{\rho} \times \mathbf{e}_{\theta}|\) |
square meters |
2D Jacobian determinant for constant zeta surface derivative wrt radial coordinate |
||
|
\(\partial_{\rho \rho} |\mathbf{e}_{\rho} \times \mathbf{e}_{\theta}|\) |
square meters |
2D Jacobian determinant for constant zeta surface second derivative wrt radial coordinate |
desc.coils.FourierRZCoil
Name |
Label |
Units |
Description |
Aliases |
kwargs |
|---|---|---|---|---|---|
|
\(0\) |
None |
Zeros |
|
|
|
\(1\) |
None |
Ones |
|
|
|
\(R\) |
meters |
Cylindrical radial position along curve |
||
|
\(X\) |
meters |
Cartesian X coordinate. |
||
|
\(Y\) |
meters |
Cartesian Y coordinate. |
||
|
\(Z\) |
meters |
Cylindrical vertical position along curve |
||
|
\(\langle\mathbf{x}\rangle\) |
meters |
Centroid of the curve |
||
|
\(\kappa\) |
Inverse meters |
Scalar curvature of the curve, with the sign denoting the convexity/concavity relative to the center of the curve (a circle has positive curvature) |
||
|
\(ds\) |
None |
Quadrature weights for integration along the curve, i.e. an alias for |
||
|
\(\mathbf{B}_{\mathrm{Frenet-Serret}}\) |
None |
Binormal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{N}_{\mathrm{Frenet-Serret}}\) |
None |
Normal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{T}_{\mathrm{Frenet-Serret}}\) |
None |
Tangent unit vector to curve in Frenet-Serret frame |
||
|
\(L\) |
meters |
Length of the curve |
||
|
\(\phi\) |
radians |
Toroidal phi position along curve |
||
|
\(s\) |
None |
Curve parameter, on [0, 2pi) |
||
|
\(\tau\) |
Inverse meters |
Scalar torsion of the curve |
||
|
\(\mathbf{x}\) |
not applicable |
Coordinate triplet. This is not a position vector unless basis is cartesian. When basis is cartesian, the units are meters. |
||
|
\(\partial_{s} \mathbf{x}\) |
meters |
Position vector along curve, first derivative |
||
|
\(\partial_{ss} \mathbf{x}\) |
meters |
Position vector along curve, second derivative |
||
|
\(\partial_{sss} \mathbf{x}\) |
meters |
Position vector along curve, third derivative |
desc.coils.FourierXYZCoil
Name |
Label |
Units |
Description |
Aliases |
kwargs |
|---|---|---|---|---|---|
|
\(0\) |
None |
Zeros |
|
|
|
\(1\) |
None |
Ones |
|
|
|
\(R\) |
meters |
Cylindrical radial position along curve |
||
|
\(X\) |
meters |
Cartesian X coordinate. |
||
|
\(Y\) |
meters |
Cartesian Y coordinate. |
||
|
\(Z\) |
meters |
Cylindrical vertical position along curve |
||
|
\(\langle\mathbf{x}\rangle\) |
meters |
Centroid of the curve |
||
|
\(\kappa\) |
Inverse meters |
Scalar curvature of the curve, with the sign denoting the convexity/concavity relative to the center of the curve (a circle has positive curvature) |
||
|
\(ds\) |
None |
Quadrature weights for integration along the curve, i.e. an alias for |
||
|
\(\mathbf{B}_{\mathrm{Frenet-Serret}}\) |
None |
Binormal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{N}_{\mathrm{Frenet-Serret}}\) |
None |
Normal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{T}_{\mathrm{Frenet-Serret}}\) |
None |
Tangent unit vector to curve in Frenet-Serret frame |
||
|
\(L\) |
meters |
Length of the curve |
||
|
\(\phi\) |
radians |
Toroidal phi position along curve |
||
|
\(s\) |
None |
Curve parameter, on [0, 2pi) |
||
|
\(\tau\) |
Inverse meters |
Scalar torsion of the curve |
||
|
\(\mathbf{x}\) |
not applicable |
Coordinate triplet. This is not a position vector unless basis is cartesian. When basis is cartesian, the units are meters. |
||
|
\(\partial_{s} \mathbf{x}\) |
meters |
Position vector along curve, first derivative |
||
|
\(\partial_{ss} \mathbf{x}\) |
meters |
Position vector along curve, second derivative |
||
|
\(\partial_{sss} \mathbf{x}\) |
meters |
Position vector along curve, third derivative |
desc.coils.FourierPlanarCoil
Name |
Label |
Units |
Description |
Aliases |
kwargs |
|---|---|---|---|---|---|
|
\(0\) |
None |
Zeros |
|
|
|
\(1\) |
None |
Ones |
|
|
|
\(R\) |
meters |
Cylindrical radial position along curve |
||
|
\(X\) |
meters |
Cartesian X coordinate. |
||
|
\(Y\) |
meters |
Cartesian Y coordinate. |
||
|
\(Z\) |
meters |
Cylindrical vertical position along curve |
||
|
\(\langle\mathbf{x}\rangle\) |
meters |
Centroid of the curve |
|
|
|
\(\kappa\) |
Inverse meters |
Scalar curvature of the curve, with the sign denoting the convexity/concavity relative to the center of the curve (a circle has positive curvature) |
||
|
\(ds\) |
None |
Quadrature weights for integration along the curve, i.e. an alias for |
||
|
\(\mathbf{B}_{\mathrm{Frenet-Serret}}\) |
None |
Binormal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{N}_{\mathrm{Frenet-Serret}}\) |
None |
Normal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{T}_{\mathrm{Frenet-Serret}}\) |
None |
Tangent unit vector to curve in Frenet-Serret frame |
||
|
\(L\) |
meters |
Length of the curve |
||
|
\(\phi\) |
radians |
Toroidal phi position along curve |
||
|
\(s\) |
None |
Curve parameter, on [0, 2pi) |
||
|
\(\tau\) |
Inverse meters |
Scalar torsion of the curve |
||
|
\(\mathbf{x}\) |
not applicable |
Coordinate triplet. This is not a position vector unless basis is cartesian. When basis is cartesian, the units are meters. |
|
|
|
\(\partial_{s} \mathbf{x}\) |
meters |
Position vector along curve, first derivative |
|
|
|
\(\partial_{ss} \mathbf{x}\) |
meters |
Position vector along curve, second derivative |
|
|
|
\(\partial_{sss} \mathbf{x}\) |
meters |
Position vector along curve, third derivative |
|
desc.coils.FourierXYCoil
Name |
Label |
Units |
Description |
Aliases |
kwargs |
|---|---|---|---|---|---|
|
\(0\) |
None |
Zeros |
|
|
|
\(1\) |
None |
Ones |
|
|
|
\(R\) |
meters |
Cylindrical radial position along curve |
||
|
\(X\) |
meters |
Cartesian X coordinate. |
||
|
\(Y\) |
meters |
Cartesian Y coordinate. |
||
|
\(Z\) |
meters |
Cylindrical vertical position along curve |
||
|
\(\langle\mathbf{x}\rangle\) |
meters |
Centroid of the curve |
|
|
|
\(\kappa\) |
Inverse meters |
Scalar curvature of the curve, with the sign denoting the convexity/concavity relative to the center of the curve (a circle has positive curvature) |
||
|
\(ds\) |
None |
Quadrature weights for integration along the curve, i.e. an alias for |
||
|
\(\mathbf{B}_{\mathrm{Frenet-Serret}}\) |
None |
Binormal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{N}_{\mathrm{Frenet-Serret}}\) |
None |
Normal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{T}_{\mathrm{Frenet-Serret}}\) |
None |
Tangent unit vector to curve in Frenet-Serret frame |
||
|
\(L\) |
meters |
Length of the curve |
||
|
\(\phi\) |
radians |
Toroidal phi position along curve |
||
|
\(s\) |
None |
Curve parameter, on [0, 2pi) |
||
|
\(\tau\) |
Inverse meters |
Scalar torsion of the curve |
||
|
\(\mathbf{x}\) |
not applicable |
Coordinate triplet. This is not a position vector unless basis is cartesian. When basis is cartesian, the units are meters. |
|
|
|
\(\partial_{s} \mathbf{x}\) |
meters |
Position vector along curve, first derivative |
|
|
|
\(\partial_{ss} \mathbf{x}\) |
meters |
Position vector along curve, second derivative |
|
|
|
\(\partial_{sss} \mathbf{x}\) |
meters |
Position vector along curve, third derivative |
|
desc.magnetic_fields._current_potential.CurrentPotentialField
Name |
Label |
Units |
Description |
Aliases |
kwargs |
|---|---|---|---|---|---|
|
\(0\) |
None |
Zeros |
|
|
|
\(1\) |
None |
Ones |
|
|
|
\(A\) |
square meters |
Average enclosed cross-sectional (constant zeta surface) area |
||
|
\(A(\rho)\) |
square meters |
Average area of enclosed cross-section (enclosed constant zeta surface), as function of rho |
||
|
\(A(\zeta)\) |
square meters |
Area of enclosed cross-section (enclosed constant zeta surface) |
||
|
\(\mathbf{K}\) |
Amperes per meter |
Surface current density, defined as thesurface normal vector cross the gradient of the current potential. |
||
|
\(K^{\theta}\) |
Amperes per square meter |
Contravariant poloidal component of surface current density |
||
|
\(K^{\zeta}\) |
Amperes per square meter |
Contravariant toroidal component of surface current density |
||
|
\(L_{\mathrm{SFF},\rho}\) |
meters |
L coefficient of second fundamental form of constant rho surface |
||
|
\(M_{\mathrm{SFF},\rho}\) |
meters |
M coefficient of second fundamental form of constant rho surface |
||
|
\(N_{\mathrm{SFF},\rho}\) |
meters |
N coefficient of second fundamental form of constant rho surface |
||
|
\(\Phi\) |
Amperes |
Surface current potential |
||
|
\(\partial_{\theta}\Phi\) |
Amperes |
Surface current potential, poloidal derivative |
||
|
\(\partial_{\zeta}\Phi\) |
Amperes |
Surface current potential, toroidal derivative |
||
|
\(R\) |
meters |
Major radius in lab frame |
||
|
\(R_{0} = V / (2\pi A) = \int R(\rho=0) d\zeta / (2\pi)\) |
meters |
Average major radius |
||
|
\(R_{0} / a\) |
None |
Aspect ratio |
||
|
\(\partial_{\theta} R\) |
meters |
Major radius in lab frame, first poloidal derivative |
||
|
\(\partial_{\theta \theta} R\) |
meters |
Major radius in lab frame, second poloidal derivative |
||
|
\(\partial_{\theta \theta \theta} R\) |
meters |
Major radius in lab frame, third poloidal derivative |
||
|
\(\partial_{\theta \theta \zeta} R\) |
meters |
Major radius in lab frame, third derivative wrt poloidal angle twice and toroidal angle |
|
|
|
\(\partial_{\theta \zeta} R\) |
meters |
Major radius in lab frame, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\theta \zeta \zeta} R\) |
meters |
Major radius in lab frame, third derivative wrt poloidal angle and toroidal angle twice |
|
|
|
\(\partial_{\zeta} R\) |
meters |
Major radius in lab frame, first toroidal derivative |
||
|
\(\partial_{\zeta \zeta} R\) |
meters |
Major radius in lab frame, second toroidal derivative |
||
|
\(\partial_{\zeta \zeta \zeta} R\) |
meters |
Major radius in lab frame, third toroidal derivative |
||
|
\(S\) |
square meters |
Surface area |
||
|
\(S(\rho)\) |
square meters |
Surface area of flux surfaces |
||
|
\(V\) |
cubic meters |
Volume enclosed by surface |
||
|
\(V(\rho)\) |
cubic meters |
Volume enclosed by flux surfaces |
||
|
\(X = R \cos{\phi}\) |
meters |
Cartesian X coordinate |
||
|
\(Y = R \sin{\phi}\) |
meters |
Cartesian Y coordinate |
||
|
\(Z\) |
meters |
Vertical coordinate in lab frame |
||
|
\(\partial_{\theta} Z\) |
meters |
Vertical coordinate in lab frame, first poloidal derivative |
||
|
\(\partial_{\theta \theta} Z\) |
meters |
Vertical coordinate in lab frame, second poloidal derivative |
||
|
\(\partial_{\theta \theta \theta} Z\) |
meters |
Vertical coordinate in lab frame, third poloidal derivative |
||
|
\(\partial_{\theta \theta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative wrt poloidal angle twice and toroidal angle |
|
|
|
\(\partial_{\theta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\theta \zeta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative wrt poloidal angle and toroidal angle twice |
|
|
|
\(\partial_{\zeta} Z\) |
meters |
Vertical coordinate in lab frame, first toroidal derivative |
||
|
\(\partial_{\zeta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, second toroidal derivative |
||
|
\(\partial_{\zeta \zeta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, third toroidal derivative |
||
|
\(a\) |
meters |
Average minor radius |
||
|
\(a_{\mathrm{major}} / a_{\mathrm{minor}}\) |
None |
Elongation at a toroidal cross-section (constant zeta surface) |
||
|
\(H_{\rho}\) |
inverse meters |
Mean curvature of constant rho surfaces |
||
|
\(K_{\rho}\) |
inverse meters squared |
Gaussian curvature of constant rho surfaces |
||
|
\(k_{1,\rho}\) |
inverse meters |
First principle curvature of constant rho surfaces |
||
|
\(k_{2,\rho}\) |
inverse meters |
Second principle curvature of constant rho surfaces |
||
|
\(\mathbf{e}_{\phi} |_{\rho, \theta}\) |
meters |
Covariant toroidal basis vector in (ρ,θ,ϕ) coordinates |
|
|
|
\(\mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector |
||
|
\(\partial_{\theta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, second derivative wrt poloidal and poloidal coordinates |
||
|
\(\partial_{\theta \zeta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, second derivative wrt poloidal and toroidal coordinates |
|
|
|
\(\partial_{\zeta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, derivative wrt toroidal coordinate |
|
|
|
\(\partial_{\zeta \zeta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, second derivative wrt toroidal and toroidal coordinates |
|
|
|
\(\mathbf{e}_{\theta} |_{\rho, \phi}\) |
meters |
Covariant poloidal basis vector in (ρ,θ,ϕ) coordinates. ϕ increases counterclockwise when viewed from above (cylindrical R,ϕ plane with Z out of page). |
||
|
\(\mathbf{e}_{\zeta}\) |
meters |
Covariant Toroidal basis vector |
||
|
\(\partial_{\zeta} \mathbf{e}_{\zeta}\) |
meters |
Covariant Toroidal basis vector, derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta \zeta} \mathbf{e}_{\zeta}\) |
meters |
Covariant Toroidal basis vector, second derivative wrt toroidal and toroidal coordinates |
||
|
\(g_{\theta\theta}\) |
square meters |
Poloidal/Poloidal element of covariant metric tensor |
||
|
\(g_{\theta\zeta}\) |
square meters |
Poloidal/Toroidal element of covariant metric tensor |
|
|
|
\(g_{\zeta\zeta}\) |
square meters |
Toroidal/Toroidal element of covariant metric tensor |
||
|
\(\nabla \phi\) |
Inverse meters |
Gradient of cylindrical toroidal angle ϕ. |
||
|
\(\hat{\mathbf{n}}_{\rho}\) |
None |
Unit vector normal to constant rho surface (direction of e^rho) |
||
|
\(\partial_{\zeta}\hat{\mathbf{n}}_{\rho}\) |
None |
Unit vector normal to constant rho surface (direction of e^rho), derivative wrt toroidal angle |
||
|
\(\omega\) |
radians |
Toroidal stream function |
||
|
\(\partial_{\rho} \omega\) |
radians |
Toroidal stream function, first radial derivative |
||
|
\(\partial_{\theta} \omega\) |
radians |
Toroidal stream function, first poloidal derivative |
||
|
\(\partial_{\theta \theta} \omega\) |
radians |
Toroidal stream function, second poloidal derivative |
||
|
\(\partial_{\theta \theta \theta} \omega\) |
radians |
Toroidal stream function, third poloidal derivative |
||
|
\(\partial_{\theta \theta \zeta} \omega\) |
radians |
Toroidal stream function, third derivative wrt poloidal angle twice and toroidal angle |
|
|
|
\(\partial_{\theta \zeta} \omega\) |
radians |
Toroidal stream function, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\theta \zeta \zeta} \omega\) |
radians |
Toroidal stream function, third derivative wrt poloidal angle and toroidal angle twice |
|
|
|
\(\partial_{\zeta} \omega\) |
radians |
Toroidal stream function, first toroidal derivative |
||
|
\(\partial_{\zeta \zeta} \omega\) |
radians |
Toroidal stream function, second toroidal derivative |
||
|
\(\partial_{\zeta \zeta \zeta} \omega\) |
radians |
Toroidal stream function, third toroidal derivative |
||
|
\(P(\zeta)\) |
meters |
Perimeter of enclosed cross-section (enclosed constant zeta surface) |
||
|
\(\phi\) |
radians |
Toroidal angle in lab frame |
||
|
\(\partial_{\rho} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt radial coordinate |
||
|
\(\partial_{\theta} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt poloidal coordinate and first derivative wrt toroidal coordinate |
|
|
|
\(\partial_{\theta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt poloidal and toroidal coordinate |
|
|
|
\(\partial_{\theta \zeta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt poloidal coordinate and second derivative wrt toroidal coordinate |
|
|
|
\(\partial_{\zeta} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta \zeta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, third derivative wrt toroidal coordinate |
||
|
\(\rho\) |
None |
Radial coordinate, proportional to the square root of the toroidal flux |
||
|
\(\theta\) |
radians |
Poloidal angular coordinate (geometric, not magnetic) |
||
|
\(\mathbf{x}\) |
not applicable |
Coordinate triplet. This is not a position vector unless basis is cartesian. When basis is cartesian, the units are meters. |
||
|
\(\zeta\) |
radians |
Toroidal angular coordinate |
||
|
\(| \mathbf{e}_{\theta} \times \mathbf{e}_{\zeta} |\) |
square meters |
2D Jacobian determinant for constant rho surface |
||
|
\(\partial_{\zeta}|\mathbf{e}_{\theta} \times \mathbf{e}_{\zeta}|\) |
square meters |
2D Jacobian determinant for constant rho surface,derivative wrt toroidal angle |
desc.magnetic_fields._current_potential.FourierCurrentPotentialField
Name |
Label |
Units |
Description |
Aliases |
kwargs |
|---|---|---|---|---|---|
|
\(0\) |
None |
Zeros |
|
|
|
\(1\) |
None |
Ones |
|
|
|
\(A\) |
square meters |
Average enclosed cross-sectional (constant zeta surface) area |
||
|
\(A(\rho)\) |
square meters |
Average area of enclosed cross-section (enclosed constant zeta surface), as function of rho |
||
|
\(A(\zeta)\) |
square meters |
Area of enclosed cross-section (enclosed constant zeta surface) |
||
|
\(\mathbf{K}\) |
Amperes per meter |
Surface current density, defined as thesurface normal vector cross the gradient of the current potential. |
||
|
\(K^{\theta}\) |
Amperes per square meter |
Contravariant poloidal component of surface current density |
||
|
\(K^{\zeta}\) |
Amperes per square meter |
Contravariant toroidal component of surface current density |
||
|
\(L_{\mathrm{SFF},\rho}\) |
meters |
L coefficient of second fundamental form of constant rho surface |
||
|
\(M_{\mathrm{SFF},\rho}\) |
meters |
M coefficient of second fundamental form of constant rho surface |
||
|
\(N_{\mathrm{SFF},\rho}\) |
meters |
N coefficient of second fundamental form of constant rho surface |
||
|
\(\Phi\) |
Amperes |
Surface current potential |
||
|
\(\partial_{\theta}\Phi\) |
Amperes |
Surface current potential, poloidal derivative |
||
|
\(\partial_{\zeta}\Phi\) |
Amperes |
Surface current potential, toroidal derivative |
||
|
\(R\) |
meters |
Major radius in lab frame |
||
|
\(R_{0} = V / (2\pi A) = \int R(\rho=0) d\zeta / (2\pi)\) |
meters |
Average major radius |
||
|
\(R_{0} / a\) |
None |
Aspect ratio |
||
|
\(\partial_{\theta} R\) |
meters |
Major radius in lab frame, first poloidal derivative |
||
|
\(\partial_{\theta \theta} R\) |
meters |
Major radius in lab frame, second poloidal derivative |
||
|
\(\partial_{\theta \theta \theta} R\) |
meters |
Major radius in lab frame, third poloidal derivative |
||
|
\(\partial_{\theta \theta \zeta} R\) |
meters |
Major radius in lab frame, third derivative wrt poloidal angle twice and toroidal angle |
|
|
|
\(\partial_{\theta \zeta} R\) |
meters |
Major radius in lab frame, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\theta \zeta \zeta} R\) |
meters |
Major radius in lab frame, third derivative wrt poloidal angle and toroidal angle twice |
|
|
|
\(\partial_{\zeta} R\) |
meters |
Major radius in lab frame, first toroidal derivative |
||
|
\(\partial_{\zeta \zeta} R\) |
meters |
Major radius in lab frame, second toroidal derivative |
||
|
\(\partial_{\zeta \zeta \zeta} R\) |
meters |
Major radius in lab frame, third toroidal derivative |
||
|
\(S\) |
square meters |
Surface area |
||
|
\(S(\rho)\) |
square meters |
Surface area of flux surfaces |
||
|
\(V\) |
cubic meters |
Volume enclosed by surface |
||
|
\(V(\rho)\) |
cubic meters |
Volume enclosed by flux surfaces |
||
|
\(X = R \cos{\phi}\) |
meters |
Cartesian X coordinate |
||
|
\(Y = R \sin{\phi}\) |
meters |
Cartesian Y coordinate |
||
|
\(Z\) |
meters |
Vertical coordinate in lab frame |
||
|
\(\partial_{\theta} Z\) |
meters |
Vertical coordinate in lab frame, first poloidal derivative |
||
|
\(\partial_{\theta \theta} Z\) |
meters |
Vertical coordinate in lab frame, second poloidal derivative |
||
|
\(\partial_{\theta \theta \theta} Z\) |
meters |
Vertical coordinate in lab frame, third poloidal derivative |
||
|
\(\partial_{\theta \theta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative wrt poloidal angle twice and toroidal angle |
|
|
|
\(\partial_{\theta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\theta \zeta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, third derivative wrt poloidal angle and toroidal angle twice |
|
|
|
\(\partial_{\zeta} Z\) |
meters |
Vertical coordinate in lab frame, first toroidal derivative |
||
|
\(\partial_{\zeta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, second toroidal derivative |
||
|
\(\partial_{\zeta \zeta \zeta} Z\) |
meters |
Vertical coordinate in lab frame, third toroidal derivative |
||
|
\(a\) |
meters |
Average minor radius |
||
|
\(a_{\mathrm{major}} / a_{\mathrm{minor}}\) |
None |
Elongation at a toroidal cross-section (constant zeta surface) |
||
|
\(H_{\rho}\) |
inverse meters |
Mean curvature of constant rho surfaces |
||
|
\(K_{\rho}\) |
inverse meters squared |
Gaussian curvature of constant rho surfaces |
||
|
\(k_{1,\rho}\) |
inverse meters |
First principle curvature of constant rho surfaces |
||
|
\(k_{2,\rho}\) |
inverse meters |
Second principle curvature of constant rho surfaces |
||
|
\(\mathbf{e}_{\phi} |_{\rho, \theta}\) |
meters |
Covariant toroidal basis vector in (ρ,θ,ϕ) coordinates |
|
|
|
\(\mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector |
||
|
\(\partial_{\theta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, second derivative wrt poloidal and poloidal coordinates |
||
|
\(\partial_{\theta \zeta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, second derivative wrt poloidal and toroidal coordinates |
|
|
|
\(\partial_{\zeta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, derivative wrt toroidal coordinate |
|
|
|
\(\partial_{\zeta \zeta} \mathbf{e}_{\theta}\) |
meters |
Covariant Poloidal basis vector, second derivative wrt toroidal and toroidal coordinates |
|
|
|
\(\mathbf{e}_{\theta} |_{\rho, \phi}\) |
meters |
Covariant poloidal basis vector in (ρ,θ,ϕ) coordinates. ϕ increases counterclockwise when viewed from above (cylindrical R,ϕ plane with Z out of page). |
||
|
\(\mathbf{e}_{\zeta}\) |
meters |
Covariant Toroidal basis vector |
||
|
\(\partial_{\zeta} \mathbf{e}_{\zeta}\) |
meters |
Covariant Toroidal basis vector, derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta \zeta} \mathbf{e}_{\zeta}\) |
meters |
Covariant Toroidal basis vector, second derivative wrt toroidal and toroidal coordinates |
||
|
\(g_{\theta\theta}\) |
square meters |
Poloidal/Poloidal element of covariant metric tensor |
||
|
\(g_{\theta\zeta}\) |
square meters |
Poloidal/Toroidal element of covariant metric tensor |
|
|
|
\(g_{\zeta\zeta}\) |
square meters |
Toroidal/Toroidal element of covariant metric tensor |
||
|
\(\nabla \phi\) |
Inverse meters |
Gradient of cylindrical toroidal angle ϕ. |
||
|
\(\hat{\mathbf{n}}_{\rho}\) |
None |
Unit vector normal to constant rho surface (direction of e^rho) |
||
|
\(\partial_{\zeta}\hat{\mathbf{n}}_{\rho}\) |
None |
Unit vector normal to constant rho surface (direction of e^rho), derivative wrt toroidal angle |
||
|
\(\omega\) |
radians |
Toroidal stream function |
||
|
\(\partial_{\rho} \omega\) |
radians |
Toroidal stream function, first radial derivative |
||
|
\(\partial_{\theta} \omega\) |
radians |
Toroidal stream function, first poloidal derivative |
||
|
\(\partial_{\theta \theta} \omega\) |
radians |
Toroidal stream function, second poloidal derivative |
||
|
\(\partial_{\theta \theta \theta} \omega\) |
radians |
Toroidal stream function, third poloidal derivative |
||
|
\(\partial_{\theta \theta \zeta} \omega\) |
radians |
Toroidal stream function, third derivative wrt poloidal angle twice and toroidal angle |
|
|
|
\(\partial_{\theta \zeta} \omega\) |
radians |
Toroidal stream function, second derivative wrt poloidal and toroidal angles |
|
|
|
\(\partial_{\theta \zeta \zeta} \omega\) |
radians |
Toroidal stream function, third derivative wrt poloidal angle and toroidal angle twice |
|
|
|
\(\partial_{\zeta} \omega\) |
radians |
Toroidal stream function, first toroidal derivative |
||
|
\(\partial_{\zeta \zeta} \omega\) |
radians |
Toroidal stream function, second toroidal derivative |
||
|
\(\partial_{\zeta \zeta \zeta} \omega\) |
radians |
Toroidal stream function, third toroidal derivative |
||
|
\(P(\zeta)\) |
meters |
Perimeter of enclosed cross-section (enclosed constant zeta surface) |
||
|
\(\phi\) |
radians |
Toroidal angle in lab frame |
||
|
\(\partial_{\rho} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt radial coordinate |
||
|
\(\partial_{\theta} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt poloidal coordinate |
||
|
\(\partial_{\theta \theta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt poloidal coordinate and first derivative wrt toroidal coordinate |
|
|
|
\(\partial_{\theta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt poloidal and toroidal coordinate |
|
|
|
\(\partial_{\theta \zeta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt poloidal coordinate and second derivative wrt toroidal coordinate |
|
|
|
\(\partial_{\zeta} \phi\) |
radians |
Toroidal angle in lab frame, derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, second derivative wrt toroidal coordinate |
||
|
\(\partial_{\zeta \zeta \zeta} \phi\) |
radians |
Toroidal angle in lab frame, third derivative wrt toroidal coordinate |
||
|
\(\rho\) |
None |
Radial coordinate, proportional to the square root of the toroidal flux |
||
|
\(\theta\) |
radians |
Poloidal angular coordinate (geometric, not magnetic) |
||
|
\(\mathbf{x}\) |
not applicable |
Coordinate triplet. This is not a position vector unless basis is cartesian. When basis is cartesian, the units are meters. |
||
|
\(\zeta\) |
radians |
Toroidal angular coordinate |
||
|
\(| \mathbf{e}_{\theta} \times \mathbf{e}_{\zeta} |\) |
square meters |
2D Jacobian determinant for constant rho surface |
||
|
\(\partial_{\zeta}|\mathbf{e}_{\theta} \times \mathbf{e}_{\zeta}|\) |
square meters |
2D Jacobian determinant for constant rho surface,derivative wrt toroidal angle |
desc.coils.SplineXYZCoil
Name |
Label |
Units |
Description |
Aliases |
kwargs |
|---|---|---|---|---|---|
|
\(0\) |
None |
Zeros |
|
|
|
\(1\) |
None |
Ones |
|
|
|
\(R\) |
meters |
Cylindrical radial position along curve |
||
|
\(X\) |
meters |
Cartesian X coordinate. |
||
|
\(Y\) |
meters |
Cartesian Y coordinate. |
||
|
\(Z\) |
meters |
Cylindrical vertical position along curve |
||
|
\(\langle\mathbf{x}\rangle\) |
meters |
Centroid of the curve |
||
|
\(\kappa\) |
Inverse meters |
Scalar curvature of the curve, with the sign denoting the convexity/concavity relative to the center of the curve (a circle has positive curvature) |
||
|
\(ds\) |
None |
Quadrature weights for integration along the curve, i.e. an alias for |
||
|
\(\mathbf{B}_{\mathrm{Frenet-Serret}}\) |
None |
Binormal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{N}_{\mathrm{Frenet-Serret}}\) |
None |
Normal unit vector to curve in Frenet-Serret frame |
||
|
\(\mathbf{T}_{\mathrm{Frenet-Serret}}\) |
None |
Tangent unit vector to curve in Frenet-Serret frame |
||
|
\(L\) |
meters |
Length of the curve |
|
|
|
\(\phi\) |
radians |
Toroidal phi position along curve |
||
|
\(s\) |
None |
Curve parameter, on [0, 2pi) |
||
|
\(\tau\) |
Inverse meters |
Scalar torsion of the curve |
||
|
\(\mathbf{x}\) |
not applicable |
Coordinate triplet. This is not a position vector unless basis is cartesian. When basis is cartesian, the units are meters. |
|
|
|
\(\partial_{s} \mathbf{x}\) |
meters |
Position vector along curve, first derivative |
|
|
|
\(\partial_{ss} \mathbf{x}\) |
meters |
Position vector along curve, second derivative |
|
|
|
\(\partial_{sss} \mathbf{x}\) |
meters |
Position vector along curve, third derivative |
|
desc.magnetic_fields._core.OmnigenousField
Name |
Label |
Units |
Description |
Aliases |
kwargs |
|---|---|---|---|---|---|
|
\(\alpha\) |
radians |
Field line label, defined on [0, 2pi) |
||
|
\(\eta\) |
radians |
Intermediate omnigenity coordinate along field lines |
||
|
\(h = \theta + (N / M) \zeta\) |
radians |
Omnigenity symmetry angle |
||
|
\(\max_{\theta \zeta} |\mathbf{B}|\) |
Tesla |
Maximum field strength on each flux surface |
||
|
\(\min_{\theta \zeta} |\mathbf{B}|\) |
Tesla |
Minimum field strength on each flux surface |
||
|
\((B_{max} - B_{min}) / (B_{min} + B_{max})\) |
None |
Mirror ratio on each flux surface |
||
|
\(\rho\) |
None |
Radial coordinate, proportional to the square root of the toroidal flux |
||
|
\(\theta_{B}\) |
radians |
Boozer poloidal angle |
|
|
|
\(\zeta_{B}\) |
radians |
Boozer toroidal angle |
||
|
\(|\mathbf{B}|\) |
Tesla |
Magnitude of omnigenous magnetic field |
Optional Keyword arguments
Name |
Description |
|---|---|
|
float: ISS04 confinement enhancement factor. Default 1. |
|
int: Maximum poloidal mode number for Boozer harmonics. Default 2*eq.M |
|
int: Maximum toroidal mode number for Boozer harmonics. Default 2*eq.N |
|
int: number of largest eigenvalues to return, default value is 1.`If Neigvals=2 eigenvalues are [-1, 0, 1] we get [1, 0] |
|
|
|
|
|
|
|
|
|
{‘rpz’, ‘xyz’}: Basis for input params vectors, Default ‘xyz’ |
|
int: Degree of polynomial used for fitting current profile. Default grid.num_rho-1 |
|
str: Fusion fuel, assuming a 50/50 mix. One of {‘DT’}. Default is ‘DT’. |
|
float: Adiabatic index. Default 0 |
|
tuple: Type of quasisymmetry, (M,N). Default (1,0) |
|
float: Value of rotational transform on the Omnigenous surface. Default 1.0 |
|
Interpolation type, Default ‘cubic’. See SplineXYZCurve docs for options. |
|
int: Number of quadrature points to use for estimating trapped fraction. Default 20. |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
array: points of vanishing integrated local shear to scan over. Default 15 points linearly spaced in [-π/2,π/2]. The values |