Source code for pyrfu.pyrf.convert_fac

#!/usr/bin/env python
# -*- coding: utf-8 -*-

# 3rd party imports
import numpy as np
import xarray as xr

from .calc_fs import calc_fs

# Local imports
from .resample import resample
from .ts_vec_xyz import ts_vec_xyz

__author__ = "Louis Richard"
__email__ = "louisr@irfu.se"
__copyright__ = "Copyright 2020-2023"
__license__ = "MIT"
__version__ = "2.4.2"
__status__ = "Prototype"


[docs]def convert_fac(inp, b_bgd, r_xyz: list = None): r"""Transforms to a field-aligned coordinate (FAC) system defined as : * R_parallel_z aligned with the background magnetic field * R_perp_y defined by R_parallel cross the position vector of the spacecraft (nominally eastward at the equator) * R_perp_x defined by R_perp_y cross R_par If inp is one vector along r direction, out is inp[perp, para] projection. Parameters ---------- inp : xarray.DataArray Time series of the input field. b_bgd : xarray.DataArray Time series of the background magnetic field. r_xyz : xarray.DataArray or ndarray or list Position vector of spacecraft. Returns ------- out : xarray.DataArray Time series of the input field in field aligned coordinates system. Notes ----- All input parameters must be in the same coordinate system. Examples -------- >>> import numpy >>> from pyrfu import mms, pyrf Time interval >>> tint = ["2019-09-14T07:54:00.000", "2019-09-14T08:11:00.000"] Spacecraft index >>> mms_id = 1 Load magnetic field (FGM) and electric field (EDP) >>> b_xyz = mms.get_data("B_gse_fgm_brst_l2", tint, mms_id) >>> e_xyz = mms.get_data("E_gse_edp_brst_l2", tint, mms_id) Convert to field aligned coordinates >>> e_xyzfac = pyrf.convert_fac(e_xyz, b_xyz, numpy.array([1, 0, 0])) """ # Check input type assert isinstance(inp, xr.DataArray), "inp must be a xarray.DataArray" assert isinstance(b_bgd, xr.DataArray), "b_xyz must be a xarray.DataArray" assert r_xyz is None or isinstance( r_xyz, (xr.DataArray, list, np.ndarray), ) if len(inp) != len(b_bgd): b_bgd = resample(b_bgd, inp, f_s=calc_fs(inp)) time, inp_data = [inp.time.data, inp.data] if r_xyz is None: r_xyz = np.array([1, 0, 0]) if isinstance(r_xyz, xr.DataArray): r_xyz = resample(r_xyz, b_bgd, f_s=calc_fs(b_bgd)) elif isinstance(r_xyz, (list, np.ndarray)) and len(r_xyz) == 3: r_xyz = np.tile(r_xyz, (len(b_bgd), 1)) if b_bgd.ndim == 2 and b_bgd.shape[1] == 3: # Normalize background magnetic field b_hat = b_bgd / np.linalg.norm(b_bgd, axis=1, keepdims=True) # Perpendicular r_perp_y = np.cross(b_hat, r_xyz, axis=1) r_perp_y /= np.linalg.norm(r_perp_y, axis=1, keepdims=True) r_perp_x = np.cross(r_perp_y, b_bgd, axis=1) r_perp_x /= np.linalg.norm(r_perp_x, axis=1, keepdims=True) r_para = b_hat elif b_bgd.ndim == 3 and b_bgd.shape[1] == 3 and b_bgd.shape[2] == 3: r_perp_x = ts_vec_xyz(b_bgd.time.data, b_bgd.data[:, 0]) r_perp_y = ts_vec_xyz(b_bgd.time.data, b_bgd.data[:, 1]) r_para = ts_vec_xyz(b_bgd.time.data, b_bgd.data[:, 2]) else: raise TypeError("b_bgd must be a vector or a tensor time series") if inp_data.ndim == 2 and inp_data.shape[1] == 3: out_data = np.zeros(inp.shape, dtype=inp_data.dtype) out_data[:, 0] = np.sum(r_perp_x * inp_data, axis=1) out_data[:, 1] = np.sum(r_perp_y * inp_data, axis=1) out_data[:, 2] = np.sum(r_para * inp_data, axis=1) # To xarray out = ts_vec_xyz(time, out_data, attrs=inp.attrs) elif inp_data.ndim == 1: out_data = np.zeros([inp_data.shape[0], 2]) out_data[:, 0] = inp * np.sum(r_perp_x * r_xyz, axis=1) out_data[:, 1] = inp * np.sum(r_para * r_xyz, axis=1) out = xr.DataArray( out_data, coords=[time, ["perp", "para"]], dims=["time", "comp"] ) else: raise TypeError("inp must be a vector or scalar") return out