Source code for pyrfu.pyrf.calc_dng
#!/usr/bin/env python
# -*- coding: utf-8 -*-
# 3rd party imports
import numpy as np
import xarray as xr
from xarray.core.dataarray import DataArray
# Local imports
from pyrfu.pyrf.ts_scalar import ts_scalar
__author__ = "Louis Richard"
__email__ = "louisr@irfu.se"
__copyright__ = "Copyright 2020-2024"
__license__ = "MIT"
__version__ = "2.4.13"
__status__ = "Prototype"
[docs]def calc_dng(p_xyz: DataArray) -> DataArray:
r"""Computes Aunai's agyrotropy coefficient.
Aunai's agyrotropy is [15]_
.. math::
D_{ng} = \frac{\sqrt{8 (P_{12}^2 + P_{13}^2 + P_{23}^2)}}
{P_\parallel + 2 P_\perp}
Parameters
----------
p_xyz : DataArray
Time series of the pressure tensor
Returns
-------
DataArray
Time series of the agyrotropy coefficient of the specie.
Raises
------
TypeError
If input is not a xarray.DataArray.
ValueError
If input is not a time series of a tensor (n_time, 3, 3).
References
----------
.. [15] Aunai, N., M. Hesse, and M. Kuznetsova (2013), Electron
nongyrotropy in the context of collisionless magnetic
reconnection, Phys. Plasmas, 20(6), 092903,
doi: https://doi.org/10.1063/1.4820953.
Examples
--------
>>> from pyrfu import mms, pyrf
Time interval
>>> tint = ["2019-09-14T07:54:00.000","2019-09-14T08:11:00.000"]
Spacecraft index
>>> ic = 1
Load magnetic field and electron pressure tensor
>>> b_xyz = mms.get_data("b_gse_fgm_srvy_l2", tint, 1)
>>> p_xyz_e = mms.get_data("pe_gse_fpi_fast_l2", tint, 1)
Rotate electron pressure tensor to field aligned coordinates
>>> p_fac_e_pp = mms.rotate_tensor(p_xyz_e, "fac", b_xyz, "pp")
Compute agyrotropy coefficient
>>> d_ng_e = pyrf.calc_dng(p_fac_e_pp)
"""
# Check input type
if not isinstance(p_xyz, xr.DataArray):
raise TypeError("p_xyz must be a xarray.DataArray")
# Check input shape
if p_xyz.data.ndim != 3 or p_xyz.shape[1] != 3 or p_xyz.shape[2] != 3:
raise ValueError("p_xyz must be a time series of a tensor")
# Parallel and perpendicular components
p_para: np.ndarray = p_xyz.data[:, 0, 0]
p_perp: np.ndarray = (p_xyz.data[:, 1, 1] + p_xyz.data[:, 2, 2]) / 2
# Off-diagonal terms
p_12: np.ndarray = p_xyz.data[:, 0, 1]
p_13: np.ndarray = p_xyz.data[:, 0, 2]
p_23: np.ndarray = p_xyz.data[:, 1, 2]
d_ng: np.ndarray = np.sqrt(8 * (p_12**2 + p_13**2 + p_23**2))
d_ng /= p_para + 2 * p_perp
d_ng_ts: DataArray = ts_scalar(p_xyz.time.data, d_ng)
return d_ng_ts