pyrokinetics.local_geometry.fourier_cgyro.LocalGeometryFourierCGYRO#
- class pyrokinetics.local_geometry.fourier_cgyro.LocalGeometryFourierCGYRO(*args, **kwargs)[source]#
Bases:
LocalGeometryLocal equilibrium representation defined as in: PPCF 51 (2009) 105009 J Candy
FourierCGYRO
\[\begin{split}\begin{align} R(r, \theta) &= 0.5 aR_0(r) + \sum_{n=1}^N [aR_n(r) \cos(n \theta) + bR_n(r) \sin(n \theta)] \\ Z(r, \theta) &= 0.5 aZ_0(r) + \sum_{n=1}^N [aZ_n(r) \cos(n \theta) + bZ_n(r) \sin(n \theta)] \\ r = (\max(R) - \min(R)) / 2 \end{align}\end{split}\]Data stored in a CleverDict Object
- psi_n#
Normalised Psi
- Type:
Float
- rho#
r/a
- Type:
Float
- r_minor#
Minor radius of flux surface
- Type:
Float
- a_minor#
Minor radius of LCFS [m]
- Type:
Float
- Rmaj#
Normalised Major radius (Rmajor/a_minor)
- Type:
Float
- Rgeo#
Normalisd major radius of normalising field (Rreference/a)
- Type:
Float
- Z0#
Normalised vertical position of midpoint (Zmid / a_minor)
- Type:
Float
- f_psi#
Torodial field function
- Type:
Float
- B0#
Toroidal field at major radius (Fpsi / Rmajor) [T]
- Type:
Float
- bunit_over_b0#
Ratio of GACODE normalising field = \(q/r \partial \psi/\partial r\) [T] to B0
- Type:
Float
- dpsidr#
\(\frac{\partial \psi}{\partial r}\)
- Type:
Float
- q#
Safety factor
- Type:
Float
- shat#
Magnetic shear
- Type:
Float
- beta_prime#
\(\beta = \beta a/L_p\)
- Type:
Float
- aR#
cosine moments of R
- Type:
ArrayLike
- aZ#
cosine moments of Z
- Type:
ArrayLike
- bR#
sine moments of R
- Type:
ArrayLike
- bZ#
sine moments of Z
- Type:
ArrayLike
- daRdr#
Derivative of aR w.r.t r
- Type:
ArrayLike
- daZdr#
Derivative of aZ w.r.t r
- Type:
ArrayLike
- dbRdr#
Derivative of bR w.r.t r
- Type:
ArrayLike
- dbZdr#
Derivative of bZ w.r.t r
- Type:
ArrayLike
- R_eq#
Equilibrium R data used for fitting
- Type:
Array
- Z_eq#
Equilibrium Z data used for fitting
- Type:
Array
- b_poloidal_eq#
Equilibrium B_poloidal data used for fitting
- Type:
Array
- theta_eq#
theta values for equilibrium data
- Type:
Float
- R#
Fitted R data
- Type:
Array
- Z#
Fitted Z data
- Type:
Array
- b_poloidal#
Fitted B_poloidal data
- Type:
Array
- theta#
Fitted theta data
- Type:
Float
- dRdtheta#
Derivative of fitted \(R\) w.r.t \(\theta\)
- Type:
Array
- dRdr#
Derivative of fitted \(R\) w.r.t \(r\)
- Type:
Array
- dZdtheta#
Derivative of fitted \(Z\) w.r.t \(\theta\)
- Type:
Array
- dZdr#
Derivative of fitted \(Z\) w.r.t \(r\)
- Type:
Array
Methods
__init__(*args, **kwargs)convert_physical_units(norms)Convert physical-unit attributes to generic simulation units of
norms.default()Default parameters for geometry Same as GA-STD case
from_gk_data(params)Initialise from data gathered from GKCode object, and additionally set bunit_over_b0
from_global_eq(eq, psi_n, norms[, show_fit, ...])Loads LocalGeometry object from an Equilibrium Object
from_local_geometry(local_geometry[, ...])Loads LocalGeometry object of one type from a LocalGeometry Object of a different type
get_RZ_derivatives(theta[, params])Calculates the derivatives of \(R(r, \theta)\) and \(Z(r, \theta)\) w.r.t \(r\) and \(\theta\), used in B_poloidal calc
get_RZ_second_derivatives(theta)Calculates the second derivatives of \(R(r, \theta)\) and \(Z(r, \theta)\) w.r.t \(r\) and \(\theta\), used in geometry terms
get_b_poloidal(theta[, params])Returns Miller prediction for get_b_poloidal given flux surface parameters
get_bunit_over_b0()Get Bunit/B0 using q and loop integral of Bp
get_d2Rdrdtheta(theta, daRdr, dbRdr)Calculate the second derivative of \(R(r, \theta)\) w.r.t \(r\) and \(\theta\)
get_d2Rdtheta2(theta)Calculates the second derivative of \(R(r, \theta)\) w.r.t \(\theta\)
get_d2Zdrdtheta(theta, daZdr, dbZdr)Calculates the second derivative of \(Z(r, \theta)\) w.r.t \(r\) and \(\theta\)
get_d2Zdtheta2(theta)Calculates the second derivative of \(Z(r, theta)\) w.r.t \(\theta\)
get_dLdtheta(theta)Returns dLdtheta used in loop integrals
get_dRdr(theta, daRdr, dbRdr)Calculates the derivatives of \(R(r, \theta)\) w.r.t \(r\)
get_dRdtheta(theta)Calculates the derivatives of \(R(r, theta)\) w.r.t \(\theta\)
get_dZdr(theta, daZdr, dbZdr)Calculates the derivatives of \(Z(r, \theta)\) w.r.t \(r\)
get_dZdtheta(theta)Calculates the derivatives of \(Z(r, theta)\) w.r.t \(\theta\)
get_f_prime([ntheta])Calculate F' from and other geometry terms
get_f_psi()Calculate safety factor from b poloidal field, R, Z and q \(f = \frac{2\pi q}{\oint \frac{dl}{R^2 B_{\theta}}}\)
get_flux_surface(theta)Generates (R,Z) of a flux surface given a set of FourierCGYRO fits
get_flux_surface_area_volume()Calculate the poloidal and toroidal area of the flux surface and the toroidal volume in units of lref
get_flux_surface_area_volume_derivatives()Calculate the derivative of the poloidal and toroidal area of the flux surface and the toroidal volume with respect to r
get_grad_r(theta[, params])MXH definition of grad r from MXH, R.
get_s_hat([Fprime, ntheta])Calculate magnetic shear from F' and other geometry terms
keys()minimise_b_poloidal(params[, even_space_theta])Function for least squares minimisation of poloidal field
normalise(norms[, context])Convert LocalGeometry Parameters to current NormalisationConvention Note this creates the attribute unit_mapping which is used to apply units to the LocalGeometry object :type norms: :param norms: Normalisation convention to convert to :type norms:
SimulationNormalisationplot_equilibrium_to_local_geometry_fit([...])test_safety_factor()Calculate safety factor from LocalGeometry object b poloidal field \(q = \frac{1}{2\pi} \oint \frac{f dl}{R^2 B_{\theta}}\)
to(norms[, context])Thin wrapper for normalise
Attributes
- get_RZ_derivatives(theta, params=None)[source]#
Calculates the derivatives of \(R(r, \theta)\) and \(Z(r, \theta)\) w.r.t \(r\) and \(\theta\), used in B_poloidal calc
- Parameters:
theta (
ArrayLike) – Array of theta points to evaluate grad_r onparams (
Array [Optional]) – If given then will use params = [daRdr[nmoments], daZdr[nmoments], dbRdr[nmoments], dbZdr[nmoments] ] when calculating derivatives, otherwise will use object attributes
- Return type:
- Returns:
dRdtheta (
Array) – Derivative of \(R\) w.r.t \(\theta\)dRdr (
Array) – Derivative of \(R\) w.r.t \(r\)dZdtheta (
Array) – Derivative of \(Z\) w.r.t \(\theta\)dZdr (
Array) – Derivative of \(Z\) w.r.t \(r\)
- get_RZ_second_derivatives(theta)[source]#
Calculates the second derivatives of \(R(r, \theta)\) and \(Z(r, \theta)\) w.r.t \(r\) and \(\theta\), used in geometry terms
- Parameters:
theta (
ArrayLike) – Array of theta points to evaluate grad_r onnormalised (
Boolean) – Control whether or not to return normalised values
- Return type:
- Returns:
d2Rdtheta2 (
Array) – Second derivative of \(R\) w.r.t \(\theta\)d2Rdrdtheta (
Array) – Second derivative of \(R\) w.r.t \(r\) and \(\theta\)d2Zdtheta2 (
Array) – Second derivative of \(Z\) w.r.t \(\theta\)d2Zdrdtheta (
Array) – Second derivative of \(Z\) w.r.t \(r\) and \(\theta\)
- get_d2Rdrdtheta(theta, daRdr, dbRdr)[source]#
Calculate the second derivative of \(R(r, \theta)\) w.r.t \(r\) and \(\theta\)
- Parameters:
theta (
ArrayLike) – Array of theta points to evaluate dZdr ondaRdr (
ArrayLike) – Derivative in aR w.r.t rdbRdr (
ArrayLike) – Derivative of bR w.r.t r
- Returns:
d2Rdrdtheta – Second derivative of R w.r.t \(r\) and \(\theta\)
- Return type:
Array
- get_d2Rdtheta2(theta)[source]#
Calculates the second derivative of \(R(r, \theta)\) w.r.t \(\theta\)
- Parameters:
theta (
ArrayLike) – Array of theta points to evaluate dRdtheta on- Returns:
d2Rdtheta2 – Second derivative of \(R\) w.r.t \(\theta\)
- Return type:
Array
- get_d2Zdrdtheta(theta, daZdr, dbZdr)[source]#
Calculates the second derivative of \(Z(r, \theta)\) w.r.t \(r\) and \(\theta\)
- Parameters:
theta (
ArrayLike) – Array of theta points to evaluate dZdr ondaZdr (
ArrayLike) – Derivative in aZ w.r.t rdbZdr (
ArrayLike) – Derivative of bZ w.r.t r
- Returns:
d2Zdrdtheta – Second derivative of \(Z\) w.r.t \(r\) and \(\theta\)
- Return type:
Array
- get_d2Zdtheta2(theta)[source]#
Calculates the second derivative of \(Z(r, theta)\) w.r.t \(\theta\)
- Parameters:
theta (
ArrayLike) – Array of theta points to evaluate dZdtheta on- Returns:
d2Zdtheta2 – Second derivative of \(Z\) w.r.t \(\theta\)
- Return type:
Array
- get_dRdr(theta, daRdr, dbRdr)[source]#
Calculates the derivatives of \(R(r, \theta)\) w.r.t \(r\)
- Parameters:
theta (
ArrayLike) – Array of theta points to evaluate dZdr ondaRdr (
ArrayLike) – Derivative in aR w.r.t rdbRdr (
ArrayLike) – Derivative of bR w.r.t r
- Returns:
dRdr – Derivative of \(R\) w.r.t \(r\)
- Return type:
Array
- get_dRdtheta(theta)[source]#
Calculates the derivatives of \(R(r, theta)\) w.r.t \(\theta\)
- Parameters:
theta (
ArrayLike) – Array of theta points to evaluate dRdtheta on- Returns:
dRdtheta – Derivative of \(R\) w.r.t \(\theta\)
- Return type:
Array
- get_dZdr(theta, daZdr, dbZdr)[source]#
Calculates the derivatives of \(Z(r, \theta)\) w.r.t \(r\)
- Parameters:
theta (
ArrayLike) – Array of theta points to evaluate dZdr ondaZdr (
ArrayLike) – Derivative in aZ w.r.t rdbZdr (
ArrayLike) – Derivative of bZ w.r.t r
- Returns:
dZdr – Derivative of \(Z\) w.r.t \(r\)
- Return type:
Array
- get_dZdtheta(theta)[source]#
Calculates the derivatives of \(Z(r, theta)\) w.r.t \(\theta\)
- Parameters:
theta (
ArrayLike) – Array of theta points to evaluate dZdtheta on- Returns:
dZdtheta – Derivative of \(Z\) w.r.t \(\theta\)
- Return type:
Array
- get_flux_surface(theta)[source]#
Generates (R,Z) of a flux surface given a set of FourierCGYRO fits
- Parameters:
theta (
Array) – Values of theta to evaluate flux surfacenormalised (
Boolean) – Control whether or not to return normalised flux surface
- Return type:
- Returns:
R (
Array) – R values for this flux surface (if not normalised then in [m])Z (
Array) – Z Values for this flux surface (if not normalised then in [m])
- property n#
- property n_moments#