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ec.py
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ec.py
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# Transcibed from original Visual Basic scripts by Clayton Lewis and Lawrence Hipps
import pandas as pd
import scipy
import numpy as np
import dask as dd
#Public Module EC
import numba
# https://stackoverflow.com/questions/47594932/row-wise-interpolation-in-dataframe-using-interp1d
# https://krstn.eu/fast-linear-1D-interpolation-with-numba/
# https://scikit-learn.org/stable/modules/generated/sklearn.covariance.EmpiricalCovariance.html
# https://pythonawesome.com/maximum-covariance-analysis-in-python/
# https://pyxmca.readthedocs.io/en/latest/quickstart.html#maximum-covariance-analysis
# https://pandas.pydata.org/pandas-docs/stable/reference/api/pandas.DataFrame.cov.html
# https://pandas.pydata.org/pandas-docs/stable/user_guide/enhancingperf.html
# https://www.statsmodels.org/devel/generated/statsmodels.tsa.stattools.acovf.html
# https://www.statsmodels.org/devel/generated/statsmodels.tsa.stattools.ccovf.html
# https://python-advanced.quantecon.org/index_time_series_models.html
class CalcFluxWithKH20(object):
"""Determines H20 flux from input weather data, including a KH20 sensor, by the eddy covariance method.
:param df: dataframe Weather Parameters for the Eddy Covariance Method; must be time-indexed and include Ux, Uy, Uz, Pr, Ea, and LnKH
:return: Atmospheric Fluxes
:notes:
No High Pass Filtering or Trend Removal are Applied to the Data
Time Series Data Are Moved Forward and Backward to Find Maximum Covariance Values
Air Temperature and Sensible Heat Flux are Estimated From Sonic Temperature and Wind Data
Other Corrections Include Transducer Shadowing, Traditional Coordinate Rotation, High Frequency Correctioons, and WPL"""
def __init__(self, **kwargs):
self.Rv = 461.51 # 'Water Vapor Gas Constant', 'J/[kg*K]'
self.Ru = 8.314 # 'Universal Gas Constant', 'J/[kg*K]'
self.Cpd = 1005 # 'Specific Heat of Dry Air', 'J/[kg*K]'
self.Rd = 287.05 # 'Dry Air Gas Constant', 'J/[kg*K]'
self.Co = 0.21 # Molar Fraction of Oxygen in the Atmosphere
self.Mo = 0.032 # Molar Mass of Oxygen (gO2/mole)
self.XKH20 = 1.412 # 'Path Length of KH20', 'cm'
self.XKwC1 = -0.152214126 # First Order Coefficient in Vapor Density-KH20 Output Relationship, cm
self.XKwC2 = -0.001667836 # Second Order Coefficient in Vapor Density-KH20 Output Relationship, cm
self.directionKH20_U = 180
self.UHeight = 3 # Height of Sonic Anemometer above Ground Surface', 'm'
self.PathKH20_U = 0.1 # Separation Distance Between Sonic Anemometer and KH20', 'm', 0.1
self.lag = 10 # number of lags to consider
self.direction_bad_min = 0 # Clockwise Orientation from DirectionKH20_U
self.direction_bad_max = 360 # Clockwise Orientation from DirectionKH20_U
self.Kw = 1 # Extinction Coefficient of Water (m^3/[g*cm]) -instrument calibration
self.Ko = -0.0045 # Extinction Coefficient of Oxygen (m^3/[g*cm]) -derived experimentally
#Despiking Weather Parameters
self.despikefields = ['Ux', 'Uy', 'Uz', 'Ts', 'volt_KH20', 'Pr', 'Ta', 'Rh']
# Allow for update of input parameters
# https://stackoverflow.com/questions/60418497/how-do-i-use-kwargs-in-python-3-class-init-function
self.__dict__.update(kwargs)
self.parameters = {
'Ea': ['Actual Vapor Pressure', 'kPa'],
'LnKH': ['Natural Log of Krypton Hygrometer Output', 'mV'],
'Pr': ['Air Pressure', 'Pa'],
'Ta': ['Air Temperature', 'K'],
'Ts': ['Sonic Temperature', 'K'],
'Ux': ['X Component of Wind Speed', 'm/s'],
'Uy': ['Y Component of Wind Speed', 'm/s'],
'Uz': ['Z Component of Wind Speed', 'm/s'],
'E': ['Vapor Pressure', 'kPa'],
'Q': ['Specific Humidity', 'unitless'],
'pV': ['Water Vapor Density', 'kg/m^3'],
'Sd': ['Entropy of Dry Air', 'J/K'],
'Tsa': ['Absolute Air Temperature Derived from Sonic Temperature', 'K'],
}
def runall(self, df):
df = self.renamedf(df)
if 'Ea' in df.columns:
pass
else:
df['Ea'] = self.tetens(df['Ta'].to_numpy())
if 'LnKH' in df.columns:
pass
else:
df['LnKH'] = np.log(df['volt_KH20'].to_numpy())
for col in self.despikefields:
if col in df.columns:
df[col] = self.despike(df[col].to_numpy(), nstd=4.5)
df['Ts'] = self.convert_CtoK(df['Ts'].to_numpy())
df['Ux'],df['Uy'],df['Uz'] = self.fix_csat(df['Ux'].to_numpy(),
df['Uy'].to_numpy(),
df['Uz'].to_numpy())
# Calculate Sums and Means of Parameter Arrays
df = self.calculated_parameters(df)
# Calculate the Correct XKw Value for KH20
XKw = self.XKwC1 + 2 * self.XKwC2 * (df['pV'].mean() * 1000.)
self.Kw = XKw / self.XKH20
# Calculate Covariances (Maximum Furthest From Zero With Sign in Lag Period)
CovTs_Ts = df[['Ts', 'Ts']].cov().iloc[0,0] # location index needed because of same fields
CovUx_Uy = df[['Ux', 'Uy']].cov().loc['Ux', 'Uy'] # CalcCovariance(IWP.Ux, IWP.Uy)
CovUx_Uz = df[['Ux', 'Uz']].cov().loc['Ux', 'Uz'] # CalcCovariance(IWP.Ux, IWP.Uz)
CovUy_Uz = df[['Uy', 'Uz']].cov().loc['Uy', 'Uz'] # CalcCovariance(IWP.Uy, IWP.Uz)
CovTs_Q = self.calc_max_covariance(df, 'Ts', 'Q', self.lag)[0]
CovUx_LnKH = self.calc_max_covariance(df, 'Ux', 'LnKH', self.lag)[0]
CovUx_Q = self.calc_max_covariance(df, 'Ux', 'Q', self.lag)[0]
CovUx_Sd = self.calc_max_covariance(df, 'Ux', 'Sd', self.lag)[0]
CovUx_Ts = self.calc_max_covariance(df, 'Ux', 'Ts', self.lag)[0]
CovUy_LnKH = self.calc_max_covariance(df, 'Uy', 'LnKH', self.lag)[0]
CovUy_Q = self.calc_max_covariance(df, 'Uy', 'Q', self.lag)[0]
CovUy_Sd = self.calc_max_covariance(df, 'Uy', 'Sd', self.lag)[0]
CovUy_Ts = self.calc_max_covariance(df, 'Uy', 'Ts', self.lag)[0]
CovUz_LnKH = self.calc_max_covariance(df, 'Uz', 'LnKH', self.lag)[0]
CovUz_Q = self.calc_max_covariance(df, 'Uz', 'Q', self.lag)[0]
CovUz_Sd = self.calc_max_covariance(df, 'Uz', 'Sd', self.lag)[0]
CovUz_Ts = self.calc_max_covariance(df, 'Uz', 'Ts', self.lag)[0]
# Traditional Coordinate Rotation
cosν, sinν, sinTheta, cosTheta, Uxy, Uxyz = self.coord_rotation(df)
# Find the Mean Squared Error of Velocity Components and Humidity
UxMSE = self.calc_MSE(df['Ux'])
UyMSE = self.calc_MSE(df['Uy'])
UzMSE = self.calc_MSE(df['Uz'])
QMSE = self.calc_MSE(df['Q'])
# Correct Covariances for Coordinate Rotation
Uz_Ts = CovUz_Ts * cosTheta - CovUx_Ts * sinTheta * cosν - CovUy_Ts * sinTheta * sinν
if np.abs(Uz_Ts) >= np.abs(CovUz_Ts):
CovUz_Ts = Uz_Ts
Uz_LnKH = CovUz_LnKH * cosTheta - CovUx_LnKH * sinTheta * cosν - CovUy_LnKH * sinν * sinTheta
if np.abs(Uz_LnKH) >= np.abs(CovUz_LnKH):
CovUz_LnKH = Uz_LnKH
CovUx_Q = CovUx_Q * cosTheta * cosν + CovUy_Q * cosTheta * sinν + CovUz_Q * sinTheta
CovUy_Q = CovUy_Q * cosν - CovUx_Q * sinν
CovUz_Q = CovUz_Q * cosTheta - CovUx_Q * sinTheta * cosν - CovUy_Q * sinν * sinTheta
CovUx_Uz = CovUx_Uz * cosν * (cosTheta**2 - sinTheta**2) - 2 * CovUx_Uy * sinTheta * cosTheta * sinν * cosν + CovUy_Uz * sinν * (cosTheta**2 - sinTheta**2) - UxMSE * sinTheta * cosTheta * cosν**2 - UyMSE * sinTheta * cosTheta * sinν**2 + UzMSE * sinTheta * cosTheta
CovUy_Uz = CovUy_Uz * cosTheta * cosν - CovUx_Uz * cosTheta * sinν - CovUx_Uy * sinTheta * (cosν**2 - sinν**2) + UxMSE * sinTheta * sinν * cosν - UyMSE * sinTheta * sinν * cosν
CovUz_Sd = CovUz_Sd * cosTheta - CovUx_Sd * sinTheta * cosν - CovUy_Sd * sinν * sinTheta
Uxy_Uz = np.sqrt(CovUx_Uz**2 + CovUy_Uz**2)
Ustr = np.sqrt(Uxy_Uz)
# Find Average Air Temperature From Average Sonic Temperature
Tsa = self.calc_Tsa(df['Ts'].mean(), df['Pr'].mean(), df['pV'].mean())
# Calculate the Latent Heat of Vaporization
lamb = (2500800 - 2366.8 * (self.convert_KtoC(Tsa)))
# Determine Vertical Wind and Water Vapor Density Covariance
Uz_pV = (CovUz_LnKH / XKw) / 1000
# Calculate the Correct Average Values of Some Key Parameters
Cp = self.Cpd * (1 + 0.84 * df['Q'].mean())
pD = (df['Pr'].mean() - df['E'].mean()) / (self.Rd * Tsa)
p = pD + df['pV'].mean()
# Calculate Variance of Air Temperature From Variance of Sonic Temperature
StDevTa = np.sqrt(CovTs_Ts - 1.02 * df['Ts'].mean() * CovTs_Q - 0.2601 * QMSE * df['Ts'].mean()**2)
Uz_Ta = CovUz_Ts - 0.07 * lamb * Uz_pV / (p * Cp)
# Determine Saturation Vapor Pressure of the Air Using Highly Accurate Wexler's Equations Modified by Hardy
Td = self.calc_Td(df['E'].mean())
D = self.calc_Es(Tsa) - df['E'].mean()
S = (self.calc_Q(df['Pr'].mean(), self.calc_Es(Tsa + 1)) - self.calc_Q(df['Pr'].mean(), self.calc_Es(Tsa - 1))) / 2
# 'Determine Wind Direction
WindDirection = np.arctan(df['Uy'].mean() / df['Ux'].mean()) * 180 / np.pi
if df['Ux'].mean() < 0:
WindDirection += 180 * np.sign(df['Uy'].mean())
direction = self.directionKH20_U - WindDirection
if direction < 0:
direction += 360
# 'Calculate the Lateral Separation Distance Projected Into the Mean Wind Direction
pathlen = self.PathKH20_U * np.abs(np.sin((np.pi / 180) * direction))
#'Calculate the Average and Standard Deviations of the Rotated Velocity Components
StDevUz = df['Uz'].std()
UMean = df['Ux'].mean() * cosTheta * cosν + df['Uy'].mean() * cosTheta * sinν + df['Uz'].mean() * sinTheta
#'Frequency Response Corrections (Massman, 2000 & 2001)
tauB = (3600) / 2.8
tauEKH20 = np.sqrt((0.01 / (4 * UMean)) **2 + (pathlen / (1.1 * UMean))**2)
tauETs = np.sqrt((0.1 / (8.4 * UMean))**2)
tauEMomentum = np.sqrt((0.1 / (5.7 * UMean))**2 + (0.1 / (2.8 * UMean))**2)
#'Calculate ζ and Correct Values of Uᕽ and Uz_Ta
L = self.calc_L(Ustr, Tsa, Uz_Ta)
alpha, X = self.calc_AlphX(L)
fX = X * UMean / self.UHeight
B = 2 * np.pi * fX * tauB
momentum = 2 * np.pi * fX * tauEMomentum
_Ts = 2 * np.pi * fX * tauETs
_KH20 = 2 * np.pi * fX * tauEKH20
Ts = self.correct_spectral(B, alpha, _Ts)
Uxy_Uz /= self.correct_spectral(B, alpha, momentum)
Ustr = np.sqrt(Uxy_Uz)
#'Recalculate L With New Uᕽ and Uz_Ta, and Calculate High Frequency Corrections
L = self.calc_L(Ustr, Tsa, Uz_Ta / Ts)
alpha, X = self.calc_AlphX(L)
Ts = self.correct_spectral(B, alpha, _Ts)
KH20 = self.correct_spectral(B, alpha, _KH20)
#'Correct the Covariance Values
Uz_Ta /= Ts
Uz_pV /= KH20
Uxy_Uz /= self.correct_spectral(B, alpha, momentum)
Ustr = np.sqrt(Uxy_Uz)
CovUz_Sd /= KH20
exchange = ((p * Cp) / (S + Cp / lamb)) * CovUz_Sd
#'KH20 Oxygen Correction
Uz_pV += self.correct_KH20(Uz_Ta, df['Pr'].mean(), Tsa)
#'Calculate New H and LE Values
H = p * Cp * Uz_Ta
lambdaE = lamb * Uz_pV
#'Webb, Pearman and Leuning Correction
lambdaE = lamb * p * Cp * Tsa * (1.0 + (1.0 / 0.622) * (df['pV'].mean() / pD)) * (Uz_pV + (df['pV'].mean() / Tsa) * Uz_Ta) / (p * Cp * Tsa + lamb * (1.0 + (1 / 0.622) * (df['pV'].mean() / pD)) * df['pV'].mean() * 0.07)
#'Finish Output
Tsa = self.convert_KtoC(Tsa)
Td = self.convert_KtoC(Td)
zeta = self.UHeight / L
ET = lambdaE * self.get_Watts_to_H2O_conversion_factor(Tsa, (df.last_valid_index() - df.first_valid_index())/ pd.to_timedelta(1, unit='D'))
#'Out.Parameters = CWP
self.columns = ['Ta','Td','D', 'Ustr', 'zeta', 'H', 'StDevUz', 'StDevTa', 'direction', 'exchange', 'lambdaE', 'ET', 'Uxy']
self.out = [Tsa, Td, D, Ustr, zeta, H, StDevUz, StDevTa, direction, exchange, lambdaE, ET, Uxy]
return pd.Series(data=self.out,index=self.columns)
def calc_LnKh(self, mvolts):
return np.log(mvolts.to_numpy())
def renamedf(self, df):
return df.rename(columns={'T_SONIC':'Ts',
'TA_1_1_1':'Ta',
'amb_press':'Pr',
'RH_1_1_1':'Rh',
't_hmp':'Ta',
'e_hmp':'Ea',
'kh':'volt_KH20'
})
def despike(self, arr, nstd=4.5):
"""Removes spikes from parameter within a specified deviation from the mean.
"""
stdd = np.nanstd(arr) * nstd
avg = np.nanmean(arr)
avgdiff = stdd - np.abs(arr - avg)
y = np.where(avgdiff >= 0, arr, np.NaN)
nans, x = np.isnan(y), lambda z: z.nonzero()[0]
if len(x(~nans)) > 0:
y[nans] = np.interp(x(nans), x(~nans), y[~nans])
return y
def calc_Td(self, E):
c0 = 207.98233
c1 = -20.156028
c2 = 0.46778925
c3 = -0.0000092288067
d0 = 1
d1 = -0.13319669
d2 = 0.0056577518
d3 = -0.000075172865
lne = np.log(E)
return (c0 + c1 * lne + c2 * lne ** 2 + c3 * lne ** 3) / (d0 + d1 * lne + d2 * lne ** 2 + d3 * lne ** 3)
def calc_Q(self, P, E):
return (0.622 * E) / (P - 0.378 * E)
def calc_E(self, pV, T):
return pV * self.Rv * T
def calc_L(self, Ust, Tsa, Uz_Ta):
#removed negative sign
return -1*(Ust ** 3) * Tsa / (9.8 * 0.4 * Uz_Ta)
#@numba.njit#(forceobj=True)
def calc_Tsa(self, Ts, P, pV, Rv=461.51):
E = pV * self.Rv * Ts
return -0.01645278052 * (
-500 * P - 189 * E + np.sqrt(250000 * P ** 2 + 128220 * E * P + 35721 * E ** 2)) / pV / Rv
#@numba.jit(forceobj=True)
def calc_AlphX(self, L):
if (self.UHeight / L) <= 0:
alph = 0.925
X = 0.085
else:
alph = 1
X = 2 - 1.915 / (1 + 0.5 * self.UHeight / L)
return alph, X
#@numba.jit(forceobj=True)
def calc_Es(self,T):
g0 = -2836.5744
g1 = -6028.076559
g2 = 19.54263612
g3 = -0.02737830188
g4 = 0.000016261698
g5 = 0.00000000070229056
g6 = -0.00000000000018680009
g7 = 2.7150305
return np.exp(
g0 * T ** (-2) + g1 * T ** (-1) + g2 + g3 * T + g4 * T ** 2 + g5 * T ** 3 + g6 * T ** 4 + g7 * np.log(T))
def calc_cov(self, p1, p2):
# p1mean = np.mean(p1)
# p2mean = np.mean(p2)
sumproduct = 0
for i in range(len(p1)):
sumproduct += p1[i] * p2[i]
return (sumproduct - (np.sum(p1) * np.sum(p2)) / len(p1)) / (len(p1) - 1)
#@numba.njit#(forceobj=True)
def calc_MSE(self, y):
return np.mean((y - np.mean(y)) ** 2)
def convert_KtoC(self, T):
return T - 273.16
def convert_CtoK(self, T):
return T + 273.16
def correct_KH20(self, Uz_Ta, P, T):
"""Calculates an additive correction for the KH20 due to cross sensitivity between H20 and 02 molecules.
Uz_Ta = Covariance of Vertical Wind Component and Air Temperature (m*K/s)
P = Air Pressure (Pa)
T = Air Temperature (K)
Kw = Extinction Coefficient of Water (m^3/[g*cm]) -instrument calibration
Ko = Extinction Coefficient of Oxygen (m^3/[g*cm]) -derived experimentally
returns KH20 Oxygen Correction
"""
return ((self.Co * self.Mo * P) / (self.Ru * T ** 2)) * (self.Ko / self.Kw) * Uz_Ta
def correct_spectral(self, B, alpha, varib):
B_alpha = B ** alpha
V_alpha = varib ** alpha
return (B_alpha / (B_alpha + 1)) * (B_alpha / (B_alpha + V_alpha)) * (1 / (V_alpha + 1))
def get_Watts_to_H2O_conversion_factor(self, temperature, day_fraction):
to_inches = 25.4
return (self.calc_water_density(temperature) * 86.4 * day_fraction) / (
self.calc_latent_heat_of_vaporization(temperature) * to_inches)
def calc_water_density(self, temperature):
d1 = -3.983035 # °C
d2 = 301.797 # °C
d3 = 522528.9 # °C2
d4 = 69.34881 # °C
d5 = 999.97495 # kg/m3
return d5 * (1 - (temperature + d1) ** 2 * (temperature + d2) / (d3 * (temperature + d4))) # 'kg/m^3
def calc_latent_heat_of_vaporization(self, temperature):
l0 = 2500800
l1 = -2360
l2 = 1.6
l3 = -0.06
return l0 + l1 * temperature + l2 * temperature ** 2 + l3 * temperature ** 3 # 'J/kg
#@numba.njit#(forceobj=True)
def fix_csat(self, Ux, Uy, Uz):
CSAT3Inverse = [[-0.5, 0, 0.86602540378444],
[0.25, 0.4330127018922, 0.86602540378444],
[0.25, -0.4330127018922, 0.86602540378444]]
CSAT3Transform = [[-1.3333333333333, 0.66666666666666, 0.66666666666666],
[0, 1.1547005383792, -1.1547005383792],
[0.3849001794597, 0.3849001794597, 0.3849001794597]]
Ux_out = []
Uy_out = []
Uz_out = []
for i in range(len(Ux)):
u = {}
u[0] = CSAT3Inverse[0][0] * Ux[i] + CSAT3Inverse[0][1] * Uy[i] + CSAT3Inverse[0][2] * Uz[i]
u[1] = CSAT3Inverse[1][0] * Ux[i] + CSAT3Inverse[1][1] * Uy[i] + CSAT3Inverse[1][2] * Uz[i]
u[2] = CSAT3Inverse[2][0] * Ux[i] + CSAT3Inverse[2][1] * Uy[i] + CSAT3Inverse[2][2] * Uz[i]
scalar = (Ux[i] ** 2. + Uy[i] ** 2. + Uz[i] ** 2.) ** 0.5
u[0] = u[0] / (0.68 + 0.32 * np.sin(np.arccos(u[0] / scalar)))
u[1] = u[1] / (0.68 + 0.32 * np.sin(np.arccos(u[1] / scalar)))
u[2] = u[2] / (0.68 + 0.32 * np.sin(np.arccos(u[2] / scalar)))
Ux_out.append(CSAT3Transform[0][0] * u[0] + CSAT3Transform[0][1] * u[1] + CSAT3Transform[0][2] * u[2])
Uy_out.append(CSAT3Transform[1][0] * u[0] + CSAT3Transform[1][1] * u[1] + CSAT3Transform[1][2] * u[2])
Uz_out.append(CSAT3Transform[2][0] * u[0] + CSAT3Transform[2][1] * u[1] + CSAT3Transform[2][2] * u[2])
return Ux_out, Uy_out, Uz_out
# Calculated Weather Parameters
# @numba.jit
def calculated_parameters(self, df):
df['pV'] = self.calc_pV(df['Ea'],df['Ts'])
df['Tsa'] = self.calc_Tsa(df['Ts'], df['Pr'], df['pV'])
df['E'] = self.calc_E(df['pV'], df['Tsa'])
df['Q'] = self.calc_Q(df['Pr'], df['E'])
df['Sd'] = self.calc_Q(df['Pr'], self.calc_Es(df['Tsa'])) - df['Q']
return df
#@numba.njit#(forceobj=True)
def calc_pV(self, Ea, Ts):
return (Ea * 1000.0) / (self.Rv * Ts)
def calc_max_covariance(self, df, colx, coly, lags=10):
dfcov = []
for i in np.arange(-1 * lags, lags):
df[f"{coly}_{i}"] = df[coly].shift(i)
dfcov.append(df[[colx, f"{coly}_{i}"]].cov().loc[colx, f"{coly}_{i}"])
# print(i,df[[colx, f"{coly}_{i}"]].cov().loc[colx, f"{coly}_{i}"])
df = df.drop([f"{coly}_{i}"], axis=1)
abscov = np.abs(dfcov)
maxabscov = np.max(abscov)
try:
maxlagindex = np.where(abscov == maxabscov)[0][0]
lagno = maxlagindex - lags
maxcov = dfcov[maxlagindex]
except IndexError:
lagno = 0
maxcov = dfcov[10]
return maxcov, lagno
#@numba.njit#(forceobj=True)
def coord_rotation(self, df, Ux='Ux', Uy='Uy', Uz='Uz'):
"""Traditional Coordinate Rotation
"""
xmean = df[Ux].mean()
ymean = df[Uy].mean()
zmean = df[Uz].mean()
Uxy = np.sqrt(xmean ** 2 + ymean ** 2)
Uxyz = np.sqrt(xmean ** 2 + ymean ** 2 + zmean ** 2)
cosν = xmean / Uxy
sinν = ymean / Uxy
sinTheta = zmean / Uxyz
cosTheta = Uxy / Uxyz
return cosν, sinν, sinTheta, cosTheta, Uxy, Uxyz
def dayfrac(self, df):
return (df.last_valid_index() - df.first_valid_index()) / pd.to_timedelta(1, unit='D')
#@numba.njit#(forceobj=True)
def tetens(self, t, a=0.611, b=17.502, c=240.97):
"""Tetens formula for computing the
saturation vapor pressure of water from temperature; eq. 3.8
t = temperature (C)
a = constant (kPa)
b = constant (dimensionless)
c = constant (C)
returns saturation vapor pressure ()
"""
return a * np.exp((b * t) / (t + c))