Source code for joseki.profiles.ussa_1976.core

"""
U.S. Standard Atmosphere 1976 thermophysical model.

The U.S. Standard Atmosphere 1976 model :cite:`NASA1976USStandardAtmosphere`
divides the atmosphere into two altitude regions:

1. the low-altitude region, from 0 to 86 kilometers
2. the high-altitude region, from 86 to 1000 kilometers.

A number of computational functions hereafter are specialized for one or
the other altitude region and is valid only in that altitude region, not in
the other.
Their name include a ``low_altitude`` or a ``high_altitude`` part to reflect
that they are valid only in the low altitude region and high altitude region,
respectively.
"""

# IMPORTANT: This is a quick port of the external ussa1976 package, which is
# no longer maintained. The code was pasted here with minimal changes and has
# redundancies and inconsistencies with respect to the rest of the codebase.
# TODO: Refactor this module

import datetime
from typing import Callable, List, Optional, Tuple, Union

import numpy as np
import numpy.ma as ma
import xarray as xr
from numpy.typing import NDArray
from scipy.integrate import cumulative_trapezoid
from scipy.interpolate import interp1d

from .constants import (
    ALPHA,
    AR_7,
    BETA,
    G0,
    GAMMA,
    H_11,
    HE_7,
    K_7,
    LAMBDA,
    LK,
    LK7,
    LK9,
    M0,
    N2_7,
    NA,
    O2_7,
    O_7,
    P0,
    PHI,
    Q1,
    Q2,
    R0,
    SIGMA,
    T0,
    T7,
    T9,
    T10,
    T11,
    TINF,
    U1,
    U2,
    W1,
    W2,
    Z7,
    Z8,
    Z9,
    Z10,
    Z12,
    A,
    B,
    H,
    K,
    M,
    R,
    S,
)
from ..._version import __version__
from ...constants import F

# List of all gas species
SPECIES = [
    "N2",
    "O2",
    "Ar",
    "CO2",
    "Ne",
    "He",
    "Kr",
    "Xe",
    "CH4",
    "H2",
    "O",
    "H",
]

# List of variables computed by the model
VARIABLES = [
    "t",
    "p",
    "n",
    "n_tot",
    "rho",
    "mv",
    "hp",
    "v",
    "mfp",
    "f",
    "cs",
    "mu",
    "nu",
    "kt",
]

# Variables standard names with respect to the Climate and Forecast (CF)
# convention
STANDARD_NAME = {
    "t": "air_temperature",
    "p": "air_pressure",
    "n": "number_density",
    "n_tot": "air_number_density",
    "rho": "air_density",
    "mv": "air_molar_volume",
    "hp": "air_pressure_scale_height",
    "v": "air_particles_mean_speed",
    "mfp": "air_particles_mean_free_path",
    "f": "air_particles_mean_collision_frequency",
    "cs": "speed_of_sound_in_air",
    "mu": "air_dynamic_viscosity",
    "nu": "air_kinematic_viscosity",
    "kt": "air_thermal_conductivity_coefficient",
    "z": "altitude",
    "h": "geopotential_height",
}

# Variables long names
LONG_NAME = {
    "t": "air temperature",
    "p": "air pressure",
    "n": "number_density",
    "n_tot": "air number density",
    "rho": "air density",
    "mv": "air molar volume",
    "hp": "air pressure scale height",
    "v": "air particles mean speed",
    "mfp": "air particles mean free path",
    "f": "air particles mean collision frequency",
    "cs": "speed of sound in air",
    "mu": "air dynamic viscosity",
    "nu": "air kinematic viscosity",
    "kt": "air thermal conductivity coefficient",
    "z": "altitude",
    "h": "geopotential height",
}

# Units of relevant quantities
UNITS = {
    "t": "K",
    "p": "Pa",
    "n": "m^-3",
    "n_tot": "m^-3",
    "rho": "kg/m^3",
    "mv": "m^3/mole",
    "hp": "m",
    "v": "m/s",
    "mfp": "m",
    "f": "s^-1",
    "cs": "m/s",
    "mu": "kg/(m*s)",
    "nu": "m^2/s",
    "kt": "W/(m*K)",
    "z": "m",
    "h": "m",
    "s": "",
}

# Variables dimensions
DIMS = {
    "t": "z",
    "p": "z",
    "n": ("s", "z"),
    "n_tot": "z",
    "rho": "z",
    "mv": "z",
    "hp": "z",
    "v": "z",
    "mfp": "z",
    "f": "z",
    "cs": "z",
    "mu": "z",
    "nu": "z",
    "kt": "z",
}


DEFAULT_Z = np.concatenate(
    [
        np.arange(0.0, 11000.0, 50.0),
        np.arange(11000.0, 32000.0, 100.0),
        np.arange(32000.0, 50000.0, 200.0),
        np.arange(50000.0, 100000.0, 500.0),
        np.arange(100000.0, 300000.0, 1000.0),
        np.arange(300000.0, 500000.0, 2000.0),
        np.arange(500000.0, 1000001.0, 5000.0),
    ]
)


[docs] def compute( z: NDArray[np.float64] = DEFAULT_Z, variables: Optional[List[str]] = None, ) -> xr.Dataset: """Compute U.S. Standard Atmosphere 1976 data set on specified altitude grid. Parameters ---------- z: array Altitude [m]. variables: list, optional Names of the variables to compute. Returns ------- Dataset Data set holding the values of the different atmospheric variables. Raises ------ ValueError When altitude is out of bounds, or when variables are invalid. """ if np.any(z < 0.0): raise ValueError("altitude values must be greater than or equal to zero") if np.any(z > 1000e3): raise ValueError("altitude values must be less then or equal to 1000 km") if variables is None: variables = VARIABLES else: for var in variables: if var not in VARIABLES: raise ValueError(var, " is not a valid variable name") # initialise data set ds = init_data_set(z=z) z_delim = 86e3 # compute the model in the low-altitude region low_altitude_region = ds.z.values <= z_delim compute_low_altitude(data_set=ds, mask=low_altitude_region, inplace=True) # compute the model in the high-altitude region high_altitude_region = ds.z.values > z_delim compute_high_altitude(data_set=ds, mask=high_altitude_region, inplace=True) # replace all np.nan with 0.0 in number densities values n = ds.n.values n[np.isnan(n)] = 0.0 ds.n.values = n # list names of variables to drop from the data set names = [] for var in ds.data_vars: # type: ignore if var not in variables: names.append(var) return ds.drop_vars(names) # type: ignore
[docs] def compute_low_altitude( data_set: xr.Dataset, mask: Optional[NDArray[bool]] = None, # type: ignore inplace: bool = False, ) -> Optional[xr.Dataset]: """Compute U.S. Standard Atmosphere 1976 in low-altitude region. Parameters ---------- data_set: Dataset Data set to compute. mask: DataArray, optional Mask to select the region of the data set to compute. By default, the mask selects the entire data set. inplace: bool, default=False If ``True``, modifies ``data_set`` in place, else returns a copy of ``data_set``. Returns ------- Dataset If ``inplace`` is ``True``, returns nothing, else returns a copy of ``data_set``. """ if mask is None: mask = np.full_like(data_set.coords["z"].values, True, dtype=bool) if inplace: ds = data_set else: ds = data_set.copy(deep=True) z = ds.z[mask].values # compute levels temperature and pressure values tb, pb = compute_levels_temperature_and_pressure_low_altitude() # compute geopotential height, temperature and pressure h = to_geopotential_height(z) t = compute_temperature_low_altitude(h=h, tb=tb) p = compute_pressure_low_altitude(h=h, pb=pb, tb=tb) # compute the auxiliary atmospheric variables n_tot = NA * p / (R * t) rho = p * M0 / (R * t) g = compute_gravity(z) mu = BETA * np.power(t, 1.5) / (t + S) # assign data set with computed values ds["t"].loc[dict(z=z)] = t ds["p"].loc[dict(z=z)] = p ds["n_tot"].loc[dict(z=z)] = n_tot species = ["N2", "O2", "Ar", "CO2", "Ne", "He", "Kr", "Xe", "CH4", "H2"] for i, s in enumerate(SPECIES): if s in species: ds["n"][i].loc[dict(z=z)] = F[s] * n_tot ds["rho"].loc[dict(z=z)] = rho ds["mv"].loc[dict(z=z)] = NA / n_tot ds["hp"].loc[dict(z=z)] = R * t / (g * M0) ds["v"].loc[dict(z=z)] = np.sqrt(8.0 * R * t / (np.pi * M0)) ds["mfp"].loc[dict(z=z)] = np.sqrt(2.0) / ( 2.0 * np.pi * np.power(SIGMA, 2.0) * n_tot ) ds["f"].loc[dict(z=z)] = ( 4.0 * NA * np.power(SIGMA, 2.0) * np.sqrt(np.pi * np.power(p, 2.0) / (R * M0 * t)) ) ds["cs"].loc[dict(z=z)] = np.sqrt(GAMMA * R * t / M0) ds["mu"].loc[dict(z=z)] = mu ds["nu"].loc[dict(z=z)] = mu / rho ds["kt"].loc[dict(z=z)] = ( 2.64638e-3 * np.power(t, 1.5) / (t + 245.4 * np.power(10.0, -12.0 / t)) ) if not inplace: return ds else: return None
[docs] def compute_high_altitude( data_set: xr.Dataset, mask: Optional[NDArray[bool]] = None, inplace: bool = False, ) -> Optional[xr.Dataset]: """Compute U.S. Standard Atmosphere 1976 in high-altitude region. Parameters ---------- data_set: Dataset Data set to compute. mask: DataArray, optional Mask to select the region of the data set to compute. By default, the mask selects the entire data set. inplace: bool, default False If ``True``, modifies ``data_set`` in place, else returns a copy of ``data_set``. Returns ------- Dataset If ``inplace`` is True, returns nothing, else returns a copy of ``data_set``. """ if mask is None: mask = np.full_like(data_set.coords["z"].values, True, dtype=bool) if inplace: ds = data_set else: ds = data_set.copy(deep=True) z = ds.coords["z"][mask].values if len(z) == 0: return ds n = compute_number_densities_high_altitude(z) species = ["N2", "O", "O2", "Ar", "He", "H"] ni: NDArray[np.float64] = np.array([n.sel(s=s).values for s in species]) n_tot = np.sum(ni, axis=0) fi = ni / n_tot[np.newaxis, :] mi: NDArray[np.float64] = np.array([M[s] for s in species]) m = np.sum(fi * mi[:, np.newaxis], axis=0) t = compute_temperature_high_altitude(z) p = K * n_tot * t rho = np.sum(ni * mi[:, np.newaxis], axis=0) / NA g = compute_gravity(z) # assign data set with computed values ds["t"].loc[dict(z=z)] = t ds["p"].loc[dict(z=z)] = p ds["n_tot"].loc[dict(z=z)] = n_tot for i, s in enumerate(SPECIES): if s in species: ds["n"][i].loc[dict(z=z)] = n.sel(s=s).values ds["rho"].loc[dict(z=z)] = rho ds["mv"].loc[dict(z=z)] = NA / n_tot ds["hp"].loc[dict(z=z)] = R * t / (g * m) ds["v"].loc[dict(z=z)] = np.sqrt(8.0 * R * t / (np.pi * m)) ds["mfp"].loc[dict(z=z)] = np.sqrt(2.0) / ( 2.0 * np.pi * np.power(SIGMA, 2.0) * n_tot ) ds["f"].loc[dict(z=z)] = ( 4.0 * NA * np.power(SIGMA, 2.0) * np.sqrt(np.pi * np.power(p, 2.0) / (R * m * t)) ) if not inplace: return ds else: return None
[docs] def init_data_set(z: NDArray[np.float64]) -> xr.Dataset: # type: ignore """Initialise data set. Parameters ---------- z: array Altitudes [m]. Returns ------- Dataset Initialised data set. """ data_vars = {} for var in VARIABLES: if var != "n": data_vars[var] = ( DIMS[var], np.full(z.shape, np.nan), { "units": UNITS[var], "long_name": LONG_NAME[var], "standard_name": STANDARD_NAME[var], }, ) else: data_vars[var] = ( DIMS[var], np.full((len(SPECIES), len(z)), np.nan), { "units": UNITS[var], "long_name": LONG_NAME[var], "standard_name": STANDARD_NAME["n"], }, ) coords = { "z": ( "z", z, { "standard_name": "altitude", "long_name": "altitude", "units": "m", }, ), "s": ("s", SPECIES, {"long_name": "species", "standard_name": "species"}), } attrs = { "convention": "CF-1.9", "title": "U.S. Standard Atmosphere 1976", "history": ( f"{datetime.datetime.utcnow().strftime('%Y-%m-%d %H:%M:%S')}" f" - data set creation - ussa1976, version {__version__}" ), "source": f"ussa1976, version {__version__}", "references": ( "U.S. Standard Atmosphere, 1976, NASA-TM-X-74335NOAA-S/T-76-1562" ), } return xr.Dataset(data_vars, coords, attrs) # type: ignore
[docs] def compute_levels_temperature_and_pressure_low_altitude() -> Tuple[ NDArray[np.float64], NDArray[np.float64] ]: """Compute temperature and pressure at low-altitude region' levels. Returns ------- tuple of arrays: Levels temperatures [K] and pressures [Pa]. """ tb = [T0] pb = [P0] for i in range(1, len(H)): t_next = tb[i - 1] + LK[i - 1] * (H[i] - H[i - 1]) tb.append(t_next) if LK[i - 1] == 0: p_next = compute_pressure_low_altitude_zero_gradient( h=H[i], hb=H[i - 1], pb=pb[i - 1], tb=tb[i - 1], ) else: p_next = compute_pressure_low_altitude_non_zero_gradient( h=H[i], hb=H[i - 1], pb=pb[i - 1], tb=tb[i - 1], lkb=LK[i - 1], ) pb.append(float(p_next)) return np.array(tb, dtype=np.float64), np.array(pb, dtype=np.float64)
[docs] def compute_number_densities_high_altitude( altitudes: NDArray[np.float64], ) -> xr.DataArray: """Compute number density of individual species in high-altitude region. Parameters ---------- altitudes: array Altitudes [m]. Returns ------- DataArray Number densities of the individual species and total number density at the given altitudes. Notes ----- A uniform altitude grid is generated and used for the computation of the integral as well as for the computation of the number densities of the individual species. This gridded data is then interpolated at the query ``altitudes`` using a linear interpolation scheme in logarithmic space. """ # altitude grid grid: NDArray[np.float64] = np.concatenate( ( np.linspace(start=Z7, stop=150e3, num=640, endpoint=False), np.geomspace(start=150e3, stop=Z12, num=100, endpoint=True), ) ) # pre-computed variables m = compute_mean_molar_mass_high_altitude(z=grid) g = compute_gravity(z=grid) t = compute_temperature_high_altitude(z=grid) dt_dz = compute_temperature_gradient_high_altitude(z=grid) below_115 = grid < 115e3 k = eddy_diffusion_coefficient(grid[below_115]) n_grid = {} # ************************************************************************* # Molecular nitrogen # ************************************************************************* y = m * g / (R * t) # m^-1 n_grid["N2"] = N2_7 * (T7 / t) * np.exp(-cumulative_trapezoid(y, grid, initial=0.0)) # ************************************************************************* # Atomic oxygen # ************************************************************************* d = thermal_diffusion_coefficient( nb=n_grid["N2"][below_115], t=t[below_115], a=A["O"], b=B["O"], ) y = thermal_diffusion_term_atomic_oxygen( grid, g, t, dt_dz, d, k, ) + velocity_term_atomic_oxygen(grid) n_grid["O"] = O_7 * (T7 / t) * np.exp(-cumulative_trapezoid(y, grid, initial=0.0)) # ************************************************************************* # Molecular oxygen # ************************************************************************* d = thermal_diffusion_coefficient( nb=n_grid["N2"][below_115], t=t[below_115], a=A["O2"], b=B["O2"], ) y = thermal_diffusion_term( s="O2", z_grid=grid, g=g, t=t, dt_dz=dt_dz, m=m, d=d, k=k, ) + velocity_term("O2", grid) n_grid["O2"] = O2_7 * (T7 / t) * np.exp(-cumulative_trapezoid(y, grid, initial=0.0)) # ************************************************************************* # Argon # ************************************************************************* background = ( n_grid["N2"][below_115] + n_grid["O"][below_115] + n_grid["O2"][below_115] ) d = thermal_diffusion_coefficient( nb=background, t=t[below_115], a=A["Ar"], b=B["Ar"], ) y = thermal_diffusion_term( s="Ar", z_grid=grid, g=g, t=t, dt_dz=dt_dz, m=m, d=d, k=k, ) + velocity_term("Ar", grid) n_grid["Ar"] = AR_7 * (T7 / t) * np.exp(-cumulative_trapezoid(y, grid, initial=0.0)) # ************************************************************************* # Helium # ************************************************************************* background = ( n_grid["N2"][below_115] + n_grid["O"][below_115] + n_grid["O2"][below_115] ) d = thermal_diffusion_coefficient( nb=background, t=t[below_115], a=A["He"], b=B["He"], ) y = thermal_diffusion_term( s="He", z_grid=grid, g=g, t=t, dt_dz=dt_dz, m=m, d=d, k=k, ) + velocity_term("He", grid) n_grid["He"] = HE_7 * (T7 / t) * np.exp(-cumulative_trapezoid(y, grid, initial=0.0)) # ************************************************************************* # Hydrogen # ************************************************************************* # below 500 km mask = (grid >= 150e3) & (grid <= 500e3) background = ( n_grid["N2"][mask] + n_grid["O"][mask] + n_grid["O2"][mask] + n_grid["Ar"][mask] + n_grid["He"][mask] ) d = thermal_diffusion_coefficient( background, t[mask], A["H"], B["H"], ) alpha = ALPHA["H"] _tau = tau_function(z_grid=grid[mask], below_500=True) y = (PHI / d) * np.power(t[mask] / T11, 1 + alpha) * np.exp(_tau) # m^-4 integral_values = cumulative_trapezoid( y[::-1], grid[mask][::-1], initial=0.0 ) # m^-3 integral_values = integral_values[::-1] n_below_500 = ( (H_11 - integral_values) * np.power(T11 / t[mask], 1 + alpha) * np.exp(-_tau) ) # above 500 km _tau = tau_function( z_grid=grid[grid > 500e3], below_500=False, ) n_above_500 = H_11 * np.power(T11 / t[grid > 500e3], 1 + alpha) * np.exp(-_tau) n_grid["H"] = np.concatenate((n_below_500, n_above_500)) n = { s: log_interp1d(grid, n_grid[s])(altitudes) for s in ["N2", "O", "O2", "Ar", "He"] } # Below 150 km, the number density of atomic hydrogen is zero. n_h_below_150 = np.zeros(len(altitudes[altitudes < 150e3])) n_h_above_150 = log_interp1d(grid[grid >= 150e3], n_grid["H"])( altitudes[altitudes >= 150e3] ) n["H"] = np.concatenate((n_h_below_150, n_h_above_150)) n_concat: NDArray[np.float64] = np.array([n[species] for species in n]) return xr.DataArray( n_concat, dims=["s", "z"], coords={ "s": ("s", [s for s in n]), "z": ("z", altitudes, dict(units="m")), }, attrs=dict(units="m^-3"), )
[docs] def compute_mean_molar_mass_high_altitude( z: NDArray[np.float64], ) -> NDArray[np.float64]: """Compute mean molar mass in high-altitude region. Parameters ---------- z: array Altitude [m]. Returns ------- array Mean molar mass [kg/mole]. """ return np.where(z <= 100e3, M0, M["N2"])
[docs] def compute_temperature_high_altitude( z: NDArray[np.float64], ) -> NDArray[np.float64]: """Compute temperature in high-altitude region. Parameters ---------- z: array Altitude [m]. Returns ------- array Temperature [K]. """ a = -76.3232 # K b = -19942.9 # m tc = 263.1905 # K def t(z: float) -> float: """Compute temperature at given altitude. Parameters ---------- z: float Altitude [m]. Returns ------- float Temperature [K]. Raises ------ ValueError If the altitude is out of range. """ if Z7 <= z <= Z8: return T7 elif Z8 < z <= Z9: return tc + a * float(np.sqrt(1.0 - np.power((z - Z8) / b, 2.0))) elif Z9 < z <= Z10: return T9 + LK9 * (z - Z9) elif Z10 < z <= Z12: return TINF - (TINF - T10) * float( np.exp(-LAMBDA * (z - Z10) * (R0 + Z10) / (R0 + z)) ) else: raise ValueError(f"altitude value '{z}' is out of range") temperature = np.vectorize(t)(z) return np.array(temperature, dtype=np.float64)
[docs] def compute_temperature_gradient_high_altitude( z: NDArray[np.float64], ) -> NDArray[np.float64]: """Compute temperature gradient in high-altitude region. Parameters ---------- z: array Altitude [m]. Returns ------- array Temperature gradient [K/m]. """ a = -76.3232 # [dimensionless] b = -19942.9 # m def gradient(z_value: float) -> float: """Compute temperature gradient at given altitude. Parameters ---------- z_value: float Altitude [m]. Raises ------ ValueError When altitude is out of bounds. Returns ------- float Temperature gradient [K / m]. """ if Z7 <= z_value <= Z8: return LK7 elif Z8 < z_value <= Z9: return ( -a / b * ((z_value - Z8) / b) / float(np.sqrt(1 - np.square((z_value - Z8) / b))) ) elif Z9 < z_value <= Z10: return LK9 elif Z10 < z_value <= Z12: zeta = (z_value - Z10) * (R0 + Z10) / (R0 + z_value) return ( LAMBDA * (TINF - T10) * float(np.square((R0 + Z10) / (R0 + z_value))) * float(np.exp(-LAMBDA * zeta)) ) else: raise ValueError( f"altitude z ({z_value}) out of range, should be in [{Z7}, {Z12}] m" ) z_values: NDArray[np.float64] = np.array(z, dtype=float) dt_dz = np.vectorize(gradient)(z_values) return np.array(dt_dz, dtype=np.float64)
[docs] def thermal_diffusion_coefficient( nb: NDArray[np.float64], t: NDArray[np.float64], a: float, b: float, ) -> NDArray[np.float64]: r"""Compute thermal diffusion coefficient values in high-altitude region. Parameters ---------- nb: array Background number density [m^-3]. t: array Temperature [K]. a: float Thermal diffusion constant :math:`a` [m^-1 * s^-1]. b: float Thermal diffusion constant :math:`b` [dimensionless]. Returns ------- array Thermal diffusion coefficient [m^2 * s^-1]. """ k = (a / nb) * np.power(t / 273.15, b) return np.array(k, dtype=np.float64)
[docs] def eddy_diffusion_coefficient(z: NDArray[np.float64]) -> NDArray[np.float64]: r"""Compute Eddy diffusion coefficient in high-altitude region. Parameters ---------- z: array Altitude [m]. Returns ------- array Eddy diffusion coefficient [m^2 * s^-1]. Notes ----- Valid in the altitude region :math:`86 \leq z \leq 150` km. """ return np.where( z < 95e3, K_7, K_7 * np.exp(1.0 - (4e8 / (4e8 - np.square(z - 95e3)))), )
[docs] def f_below_115_km( g: NDArray[np.float64], t: NDArray[np.float64], dt_dz: NDArray[np.float64], m: Union[float, NDArray[np.float64]], mi: float, alpha: float, d: NDArray[np.float64], k: NDArray[np.float64], ) -> NDArray[np.float64]: r"""Evaluate function :math:`f` below 115 km altitude. Evaluates the function :math:`f` defined by equation (36) in :cite:`NASA1976USStandardAtmosphere` in the altitude region :math:`86` km :math:`\leq z \leq 115` km. Parameters ---------- g: array Gravity values at the different altitudes [m * s^-2]. t: array Temperature values at the different altitudes [K]. dt_dz: array Temperature gradient values at the different altitudes [K * m^-1]. m: array Molar mass [kg * mole^-1]. mi: float Species molar masses [kg * mole^-1]. alpha: float Alpha thermal diffusion constant [dimensionless]. d: array Thermal diffusion coefficient values at the different altitudes [m^2 * s^-1]. k: array Eddy diffusion coefficient values at the different altitudes [m^2 * s^-1]. Returns ------- array Function :math:`f` at the different altitudes. """ term_1 = g * d / ((d + k) * (R * t)) term_2 = mi + (m * k) / d + (alpha * R * dt_dz) / g return term_1 * term_2
[docs] def f_above_115_km( g: NDArray[np.float64], t: NDArray[np.float64], dt_dz: NDArray[np.float64], mi: float, alpha: float, ) -> NDArray[np.float64]: r"""Evaluate function :math:`f` above 115 km altitude. Evaluate the function :math:`f` defined by equation (36) in :cite:`NASA1976USStandardAtmosphere` in the altitude region :math:`115` :math:`\lt z \leq 1000` km. Parameters ---------- g: array Gravity at the different altitudes [m * s^-2]. t: array Temperature at the different altitudes [K]. dt_dz: array Temperature gradient at the different altitudes [K * m^-1]. mi: float Species molar masses [kg * mole^-1]. alpha: float Alpha thermal diffusion constant [dimensionless]. Returns ------- array Function :math:`f` at the different altitudes. """ return (g / (R * t)) * (mi + ((alpha * R) / g) * dt_dz) # type: ignore
[docs] def thermal_diffusion_term( s: str, z_grid: NDArray[np.float64], g: NDArray[np.float64], t: NDArray[np.float64], dt_dz: NDArray[np.float64], m: NDArray[np.float64], d: NDArray[np.float64], k: NDArray[np.float64], ) -> NDArray[np.float64]: """Compute thermal diffusion term of given species in high-altitude region. Parameters ---------- s: str Species. z_grid: array Altitude grid [m]. g: array Gravity values on the altitude grid [m * s^-2]. t: array Temperature values on the altitude grid [K]. dt_dz: array Temperature gradient values on the altitude grid [K * m^-1]. m: array Values of the mean molar mass on the altitude grid [kg * mole^-1]. d: array Molecular diffusion coefficient values on the altitude grid, for altitudes strictly less than 115 km [m^2 * s^-1]. k: array Eddy diffusion coefficient values on the altitude grid, for altitudes strictly less than 115 km [m^2 * s^-1]. Returns ------- array Thermal diffusion term [m^-1]. """ below_115_km = z_grid < 115e3 fo1 = f_below_115_km( g[below_115_km], t[below_115_km], dt_dz[below_115_km], m[below_115_km], M[s], ALPHA[s], d, k, ) above_115_km = z_grid >= 115e3 fo2 = f_above_115_km( g[above_115_km], t[above_115_km], dt_dz[above_115_km], M[s], ALPHA[s], ) return np.concatenate((fo1, fo2))
[docs] def thermal_diffusion_term_atomic_oxygen( z_grid: NDArray[np.float64], g: NDArray[np.float64], t: NDArray[np.float64], dt_dz: NDArray[np.float64], d: NDArray[np.float64], k: NDArray[np.float64], ) -> NDArray[np.float64]: """Compute oxygen thermal diffusion term in high-altitude region. Parameters ---------- z_grid: array Altitude grid [m]. g: array Gravity values on the altitude grid [m * s^-2]. t: array Temperature values on the altitude grid [K]. dt_dz: array Temperature values gradient on the altitude grid [K * m^-1]. d: array Thermal diffusion coefficient on the altitude grid [m^2 * s^-1]. k: array Eddy diffusion coefficient values on the altitude grid [m^2 * s^-1]. Returns ------- array Thermal diffusion term [-1]. """ mask1, mask2 = z_grid < 115e3, z_grid >= 115e3 x1 = f_below_115_km( g=g[mask1], t=t[mask1], dt_dz=dt_dz[mask1], m=M["N2"], mi=M["O"], alpha=ALPHA["O"], d=d, k=k, ) x2 = f_above_115_km( g=g[mask2], t=t[mask2], dt_dz=dt_dz[mask2], mi=M["O"], alpha=ALPHA["O"], ) return np.concatenate((x1, x2))
[docs] def velocity_term_hump( z: NDArray[np.float64], q1: float, q2: float, u1: float, u2: float, w1: float, w2: float, ) -> NDArray[np.float64]: r"""Compute transport term. Compute the transport term given by equation (37) in :cite:`NASA1976USStandardAtmosphere`. Parameters ---------- z: array Altitude [m]. q1: float Q constant [m^-3]. q2: float q constant [m^-3]. u1: float U constant [m]. u2: float u constant [m]. w1: float W constant [m^-3]. w2: float w constant [m^-3]. Returns ------- array: Transport term [m^-1]. Notes ----- Valid in the altitude region: 86 km :math:`\leq z \leq` 150 km. """ t = q1 * np.square(z - u1) * np.exp(-w1 * np.power(z - u1, 3.0)) + q2 * np.square( u2 - z ) * np.exp(-w2 * np.power(u2 - z, 3.0)) return np.array(t, dtype=np.float64)
[docs] def velocity_term_no_hump( z: NDArray[np.float64], q1: float, u1: float, w1: float ) -> NDArray[np.float64]: r"""Compute transport term. Compute the transport term given by equation (37) in :cite:`NASA1976USStandardAtmosphere` where the second term is zero. Parameters ---------- z: array Altitude. q1: float Q constant [m^-3]. u1: float U constant [m]. w1: float W constant [m^-3]. Returns ------- array Transport term [m^-1]. Notes ----- Valid in the altitude region :math:`86` km :math:`\leq z \leq 150` km. """ t = q1 * np.square(z - u1) * np.exp(-w1 * np.power(z - u1, 3.0)) # m^-1 return np.array(t, np.float64)
[docs] def velocity_term(s: str, z_grid: NDArray[np.float64]) -> NDArray[np.float64]: """Compute velocity term of a given species in high-altitude region. Parameters ---------- s: str Species. z_grid: array Altitude grid [m]. Returns ------- array Velocity term [m^-1]. Notes ----- Not valid for atomic oxygen. See :func:`velocity_term_atomic_oxygen`. """ x1 = velocity_term_no_hump( z=z_grid[z_grid <= 150e3], q1=Q1[s], u1=U1[s], w1=W1[s], ) # Above 150 km, the velocity term is neglected, as indicated at p. 14 in # :cite:`NASA1976USStandardAtmosphere` x2 = np.zeros(len(z_grid[z_grid > 150e3])) return np.concatenate((x1, x2))
[docs] def velocity_term_atomic_oxygen( grid: NDArray[np.float64], ) -> NDArray[np.float64]: """Compute velocity term of atomic oxygen in high-altitude region. Parameters ---------- grid: array Altitude grid [m]. Returns ------- array Velocity term [m^-1]. """ mask1, mask2 = grid <= 150e3, grid > 150e3 x1 = np.where( grid[mask1] <= 97e3, velocity_term_hump( z=grid[mask1], q1=Q1["O"], q2=Q2["O"], u1=U1["O"], u2=U2["O"], w1=W1["O"], w2=W2["O"], ), # m^-1 velocity_term_no_hump( z=grid[mask1], q1=Q1["O"], u1=U1["O"], w1=W1["O"], ), # m^-1 ) x2 = np.zeros(len(grid[mask2])) return np.concatenate((x1, x2))
[docs] def tau_function( z_grid: NDArray[np.float64], below_500: bool = True ) -> NDArray[np.float64]: r"""Compute :math:`\tau` function. Compute integral given by equation (40) in :cite:`NASA1976USStandardAtmosphere` at each point of an altitude grid. Parameters ---------- z_grid: array Altitude grid (values sorted by ascending order) to use for integration [m]. below_500: bool, default True ``True`` if altitudes in ``z_grid`` are lower than 500 km, False otherwise. Returns ------- array Integral evaluations [dimensionless]. Notes ----- Valid for 150 km :math:`\leq z \leq` 500 km. """ if below_500: z_grid = z_grid[::-1] y = ( M["H"] * compute_gravity(z=z_grid) / (R * compute_temperature_high_altitude(z=z_grid)) ) # m^-1 integral_values: NDArray[np.float64] = np.array( cumulative_trapezoid(y, z_grid, initial=0.0), dtype=np.float64 ) if below_500: values: NDArray[np.float64] = integral_values[::-1] return values else: return integral_values
[docs] def log_interp1d( x: NDArray[np.float64], y: NDArray[np.float64] ) -> Callable[[NDArray[np.float64]], NDArray[np.float64]]: """Compute linear interpolation of :math:`y(x)` in logarithmic space. Parameters ---------- x: array 1-D array of real values. y: array N-D array of real values. The length of y along the interpolation axis must be equal to the length of x. Returns ------- callable Interpolating function. """ logx = np.log10(x) logy = np.log10(y) lin_interp = interp1d(logx, logy, kind="linear") def log_interp(z: NDArray[np.float64]) -> NDArray[np.float64]: value = np.power(10.0, lin_interp(np.log10(z))) return np.array(value, dtype=np.float64) return log_interp
[docs] def compute_pressure_low_altitude( h: NDArray[np.float64], pb: NDArray[np.float64], tb: NDArray[np.float64], ) -> NDArray[np.float64]: """Compute pressure in low-altitude region. Parameters ---------- h: array Geopotential height [m]. pb: array Levels pressure [Pa]. tb: array Levels temperature [K]. Returns ------- array Pressure [Pa]. """ # we create a mask for each layer masks = [ ma.masked_inside(h, H[i - 1], H[i]).mask # type: ignore for i in range(1, len(H)) ] # for each layer, we evaluate the pressure based on whether the # temperature gradient is zero or non-zero p = np.empty(len(h)) for i, mask in enumerate(masks): if LK[i] == 0: p[mask] = compute_pressure_low_altitude_zero_gradient( h=h[mask], hb=H[i], pb=pb[i], tb=tb[i], ) else: p[mask] = compute_pressure_low_altitude_non_zero_gradient( h=h[mask], hb=H[i], pb=pb[i], tb=tb[i], lkb=LK[i], ) return p
[docs] def compute_pressure_low_altitude_zero_gradient( h: Union[float, NDArray[np.float64]], hb: float, pb: float, tb: float, ) -> NDArray[np.float64]: """Compute pressure in low-altitude zero temperature gradient region. Parameters ---------- h: array Geopotential height [m]. hb: float Geopotential height at the bottom of the layer [m]. pb: float Pressure at the bottom of the layer [Pa]. tb: float Temperature at the bottom of the layer [K]. Returns ------- array Pressure [Pa]. """ p = pb * np.exp(-G0 * M0 * (h - hb) / (R * tb)) return np.array(p, dtype=np.float64)
[docs] def compute_pressure_low_altitude_non_zero_gradient( h: Union[float, NDArray[np.float64]], hb: float, pb: float, tb: float, lkb: float, ) -> NDArray[np.float64]: """Compute pressure in low-altitude non-zero temperature gradient region. Parameters ---------- h: array Geopotential height [m]. hb: float Geopotential height at the bottom of the layer [m]. pb: float Pressure at the bottom of the layer [Pa]. tb: float Temperature at the bottom of the layer [K]. lkb: float Temperature gradient in the layer [K * m^-1]. Returns ------- array Pressure [Pa]. """ p = pb * np.power(tb / (tb + lkb * (h - hb)), G0 * M0 / (R * lkb)) return np.array(p, dtype=np.float64)
[docs] def compute_temperature_low_altitude( h: NDArray[np.float64], tb: NDArray[np.float64], ) -> NDArray[np.float64]: """Compute temperature in low-altitude region. Parameters ---------- h: array Geopotential height [m]. tb: array Levels temperature [K]. Returns ------- array Temperature [K]. """ # we create a mask for each layer masks = [ ma.masked_inside(h, H[i - 1], H[i]).mask # type: ignore for i in range(1, len(H)) ] # for each layer, we evaluate the pressure based on whether the # temperature gradient is zero or not t = np.empty(len(h)) for i, mask in enumerate(masks): if LK[i] == 0: t[mask] = tb[i] else: t[mask] = tb[i] + LK[i] * (h[mask] - H[i]) return t
[docs] def to_altitude(h: NDArray[np.float64]) -> NDArray[np.float64]: """Convert geopotential height to (geometric) altitude. Parameters ---------- h: array Geopotential altitude [m]. Returns ------- array Altitude [m]. """ return R0 * h / (R0 - h)
[docs] def to_geopotential_height(z: NDArray[np.float64]) -> NDArray[np.float64]: """Convert altitude to geopotential height. Parameters ---------- z: array Altitude [m]. Returns ------- array Geopotential height [m]. """ return R0 * z / (R0 + z)
[docs] def compute_gravity(z: NDArray[np.float64]) -> NDArray[np.float64]: """Compute gravity. Parameters ---------- z : array Altitude [m]. Returns ------- array Gravity [m * s^-2]. """ return np.array(G0 * np.power((R0 / (R0 + z)), 2.0), dtype=np.float64)