Source code for magic.spectralTransforms

# -*- coding: utf-8 -*-
import numpy as np
from .setup import buildSo

if buildSo:
    import magic.legendre as leg


[docs]class SpectralTransforms(object): """ This python class is used to compute Legendre and Fourier transforms from spectral to physical space. It works in two steps: one first needs to initialize the transform >>> sh = SpectralTransforms( l_max=256, lm_max=33153, n_theta_max=384) >>> print(Tlm[:, 10].shape) # lm_max (Temperature at ir=10) >>> T = sh.spec_spat(Tlm) # T[n_phi_max, n_theta_max] """ def __init__(self, l_max=32, minc=1, lm_max=561, n_theta_max=64, m_max = None, verbose=True): """ :param l_max: maximum spherical harmonic degree :type l_max: int :param minc: azimuthal symmetry :type minc: int :param lm_max: maximum l,m combination :type lm_max: int :param n_theta_max: number of grid points in the latitudinal direction :type n_theta_max: int :param verbose: some info about the SHT layout :type verbose: bool """ self._legF90 = leg.legendre if m_max is None: self.m_max = int((l_max/minc) * minc) else: self.m_max = int(m_max) self._legF90.init(l_max, minc, lm_max, n_theta_max, self.m_max) self.l_max = self._legF90.l_max self.minc = self._legF90.minc self.lm_max = self._legF90.lm_max self.n_theta_max = self._legF90.n_theta_max self.n_phi_max = self._legF90.n_phi_max if verbose: print('Spectral transform setup:') print('l_max, m_max, minc, lm_max: {}, {}, {}, {}'.format( self.l_max, self.m_max, self.minc, self.lm_max)) print('n_phi_max, n_theta_max: {}, {}'.format( self.n_phi_max, self.n_theta_max)) self.colat = self._legF90.sinth self.idx = np.zeros((self.l_max+1, self.m_max+1), 'i') self.ell = np.zeros((self.lm_max), 'i') self.m = np.zeros((self.lm_max), 'i') k = 0 for m in range(0, self.m_max+1, self.minc): for l in range(m, self.l_max+1): self.idx[l, m] = k self.ell[self.idx[l,m]] = l self.m[self.idx[l,m]] = m k += 1
[docs] def spec_spat(self, *args, **kwargs): """ This subroutine computes a transfrom from spectral to spatial for all latitudes. It returns either one or two 2-D arrays (dimension(n_phi_max,n_theta_max)) depending if only the poloidal or both the poloidal and the toroidal potentials are given as input quantities. >>> print(wlmr.shape) # lm_max >>> vr = spec_spat_equat(wlmr) >>> print(vr.shape) # n_phi, n_theta >>> vt, vp = spec_spat_equat(dwdrlmr, zlmr) """ if 'l_axi' in kwargs: l_axi = kwargs['l_axi'] if l_axi: n_phi = 1 else: n_phi = self.n_phi_max else: n_phi = self.n_phi_max if len(args) == 1: polo = args[0] out = self._legF90.specspat_scal(polo, self.n_theta_max, n_phi) if n_phi > 1: out = np.fft.ifft(out, axis=0)*self.n_phi_max out = out.real return out elif len(args) == 2: polo = args[0] toro = args[1] vt, vp = self._legF90.specspat_vec(polo, toro, self.n_theta_max, n_phi) if n_phi > 1: vt = np.fft.ifft(vt, axis=0)*self.n_phi_max vp = np.fft.ifft(vp, axis=0)*self.n_phi_max vt = vt.real vp = vp.real return vt, vp
[docs] def spec_spat_dtheta(self, polo, l_axi=False): """ This routine computes the theta-derivative and the transform from spectral to spatrial spaces. It returns a 2-D array of dimension (n_phi,n_theta) >>> p = MagicPotential('V') >>> vrlm = p.pol*p.ell*(p.ell+1)/p.radius[ir]**2/p.rho0[ir] # vr at r=ir >>> dvrdt = p.sh.spec_spat_dtheta(vrlm) # theta-derivative of vr :param polo: the input array(lm_max) in spectral space :type polo: numpy.ndarray :param l_axi: switch to True, if only the axisymmetric field is needed :type l_axi: bool :returns: the theta derivative in the physical space (n_phi, n_theta) :rtype: numpy.ndarray """ if l_axi: n_phi = 1 else: n_phi = self.n_phi_max out = self._legF90.specspat_dtheta(polo, self.n_theta_max, n_phi) if n_phi > 1: out = np.fft.ifft(out, axis=0)*self.n_phi_max out = out.real return out
[docs] def spec_spat_dphi(self, polo): """ This routine computes the phi-derivative and the transform from spectral to spatrial spaces. It returns a 2-D array of dimension (n_phi,n_theta) >>> p = MagicPotential('V') >>> vrlm = p.pol*p.ell*(p.ell+1)/p.radius[ir]**2/p.rho0[ir] # vr at r=ir >>> dvrdp = p.sh.spec_spat_dphi(vrlm) # phi-derivative of vr :param polo: the input array(lm_max) in spectral space :type polo: numpy.ndarray :returns: the phi derivative in the physical space (n_phi, n_theta) :rtype: numpy.ndarray """ out = self._legF90.specspat_dphi(polo, self.n_theta_max, self.n_phi_max) out = np.fft.ifft(out, axis=0)*self.n_phi_max # since dPhilm contains a 1/sin(theta) one has to multiply by sin(theta) out = out.real * np.sin(self.colat) return out
[docs] def spec_spat_equat(self, *args): """ This subroutine computes a transfrom from spectral to spatial at the equator. It returns either one or two 1-D arrays (dimension(n_phi_max)) depending if only the poloidal or both the poloidal and the toroidal potentials are given as input quantities. >>> print(wlmr.shape) # lm_max >>> vr = spec_spat_equat(wlmr) >>> print(vr.shape) # n_phi >>> vt, vp = spec_spat_equat(dwdrlmr, zlmr) """ if len(args) == 1: polo = args[0] out = np.zeros((self.n_phi_max), np.complex128) self._legF90.specspat_equat_scal(polo, out) out = np.fft.ifft(out)*self.n_phi_max out = out.real return out elif len(args) == 2: polo = args[0] toro = args[1] vt = np.zeros((self.n_phi_max), np.complex128) vp = np.zeros((self.n_phi_max), np.complex128) self._legF90.specspat_equat_vec(polo, toro, vt, vp) vt = np.fft.ifft(vt)*self.n_phi_max vp = np.fft.ifft(vp)*self.n_phi_max vt = vt.real vp = vp.real return vt, vp
[docs] def spat_spec(self, *args): """ This subroutine computes a transfrom from spatial representation (n_phi,n_theta) to spectral representation (lm_max). It returns one complex 1-D array (dimension(n_phi_max)) >>> gr = MagicGraph() >>> sh = SpectralTransforms(gr.l_max, gr.minc, gr.lm_max, gr.n_theta_max) >>> vr = gr.vr[:,:,30] # Radius ir=30 >>> vrlm = sh.spat_spec(vr) # vrlm is a complex array (lm_max) >>> # Caculation of the poloidal potential from vr: >>> wlm = np.zeros_like(vrlm) >>> wlm[1:] = vrlm[1:]/(sh.ell[1:]*(sh.ell[1:]+1))*gr.radius[30]**2 >>> # Spheroidal/Toroidal transform >>> vtlm, vplm = spec_spat(gr.vtheta, gr.vphi) :param input: input array in the physical space (n_phi,n_theta) :type input: numpy.ndarray :returns: output array in the spectral space (lm_max) :rtype: numpy.ndarray """ if len(args) == 1: input = args[0] out = np.fft.fft(input, axis=0)/self.n_phi_max outLM = self._legF90.spatspec(out, self.lm_max) return outLM elif len(args) == 2: in1 = args[0] in2 = args[1] out1 = np.fft.fft(in1, axis=0)/self.n_phi_max out2 = np.fft.fft(in2, axis=0)/self.n_phi_max utLM, upLM = self._legF90.spatspec_sphertor(out1, out2, self.lm_max) return utLM, upLM
if __name__ == '__main__': sh = SpectralTransforms( l_max=256, lm_max=33153, n_theta_max=384) print( a.lm_max )