From d73ae558238c05a5364af5ff67cc156f3f07d800 Mon Sep 17 00:00:00 2001 From: Ben Ryan Date: Wed, 8 Jan 2025 10:43:52 -0700 Subject: [PATCH] oops --- README.md | 22 +++++++++++++--------- 1 file changed, 13 insertions(+), 9 deletions(-) diff --git a/README.md b/README.md index d2ae82a..561d26e 100644 --- a/README.md +++ b/README.md @@ -15,19 +15,20 @@ For frequency-dependent absorption opacities, the following functions are provid | --------------------- | ---------- | --------------------- | ------- | | AbsorptionCoefficient | $n \sigma$ | Absorption coefficient | ${\rm cm}^{-1}$ | | AngleAveragedAbsorptionCoefficient | $\frac{1}{4 \pi}\int n \sigma d\Omega$ | Absorption coefficient averaged over solid angle | ${\rm cm}^{-1}$ | -| EmissivityPerNuOmega | $j_{\nu} = \frac{dE}{d^3x dt d\Omega d\nu}$ | Frequency- and angle-dependent emissivity | ${\rm erg~cm}^{-3}~{\rm s}^{-1}~{\rm Sr}^{-1}~{\rm Hz}^{-1}$ | -| EmissivityPerNu | $\int j_{\nu} d\Omega$ | Frequency-dependent emissivity | ${\rm erg~cm}^{-3}~{\rm s}^{-1}~{\rm Hz}^{-1}$ | -| Emissivity | $\int j_{\nu} d\nu d\Omega$ | Total emissivity | ${\rm erg~cm}^{-3}~{\rm s}^{-1}$ | +| EmissivityPerNuOmega | $j_{\nu} = \frac{dE}{d^3x dt d\Omega d\nu}$ | Frequency- and angle-dependent emissivity | ${\rm erg}~{\rm cm}^{-3}~{\rm s}^{-1}~{\rm Sr}^{-1}~{\rm Hz}^{-1}$ | +| EmissivityPerNu | $\int j_{\nu} d\Omega$ | Frequency-dependent emissivity | ${\rm erg}~{\rm cm}^{-3}~{\rm s}^{-1}~{\rm Hz}^{-1}$ | +| Emissivity | $\int j_{\nu} d\nu d\Omega$ | Total emissivity | ${\rm erg}~{\rm cm}^{-3}~{\rm s}^{-1}$ | | NumberEmissivity | $\int \frac{1}{h \nu} j_{\nu} d\Omega d\nu$ | Total number emissivity | ${\rm cm}^{-3}~{\rm s}^{-1}$ | -| ThermalDistributionOfTNu | $B_{\nu} = \frac{dE}{dA dt d\Omega d\nu}$ | Specific intensity of thermal distribution | ${\rm erg~cm}^{-2}~{\rm s}^{-1}~{\rm Sr}^{-1}~{\rm Hz}^{-1}$ | -| DThermalDistributionOfTNuDT | $dB_{\nu}/dT$ | Temperature derivative of specific intensity of thermal distribution | ${\rm erg~cm}^{-2}~{\rm s}^{-1}~{\rm Sr}^{-1}~{\rm Hz}^{-1}~{\rm K}^{-1}$ | -| ThermalDistributionOfT | $B = \int B_{\nu} d\Omega d\nu$ | Frequency- and angle-integrated intensity of thermal distribution | ${\rm erg~cm}^{-2}~{\rm s}^{-1}$ | -| ThermalNumberDistributionOfT | $B = \int \frac{1}{h \nu} B_{\nu} d\Omega d\nu$ | Frequency- and angle-integrated intensity of thermal distribution | ${\rm erg~cm}^{-2}~{\rm s}^{-1}$ | -| EnergyDensityFromTemperature | $E_{\rm R}$ | Radiation energy density | ${\rm erg~cm}^{-3}$ | +| ThermalDistributionOfTNu | $B_{\nu} = \frac{dE}{dA dt d\Omega d\nu}$ | Specific intensity of thermal distribution | ${\rm erg}~{\rm cm}^{-2}~{\rm s}^{-1}~{\rm Sr}^{-1}~{\rm Hz}^{-1}$ | +| DThermalDistributionOfTNuDT | $dB_{\nu}/dT$ | Temperature derivative of specific intensity of thermal distribution | ${\rm erg}~{\rm cm}^{-2}~{\rm s}^{-1}~{\rm Sr}^{-1}~{\rm Hz}^{-1}~{\rm K}^{-1}$ | +| ThermalDistributionOfT | $B = \int B_{\nu} d\Omega d\nu$ | Frequency- and angle-integrated intensity of thermal distribution | ${\rm erg}~{\rm cm}^{-2}~{\rm s}^{-1}$ | +| ThermalNumberDistributionOfT | $B = \int \frac{1}{h \nu} B_{\nu} d\Omega d\nu$ | Frequency- and angle-integrated intensity of thermal distribution | ${\rm erg}~{\rm cm}^{-2}~{\rm s}^{-1}$ | +| EnergyDensityFromTemperature | $E_{\rm R}$ | Radiation energy density | ${\rm erg}~{\rm cm}^{-3}$ | | TemperatureFromEnergyDensity | $T_{\rm R}$ | Radiation temperature | ${\rm K}$ | | NumberDensityFromTemperature | $n_{\rm R}$ | Radiation number density | ${\rm cm}^{-3}$ | with the following function signatures: + AbsorptionCoefficient(density, temperature, frequency) AngleAveragedAbsorptionCoefficient(density, temperature, frequency) EmissivityPerNuOmega(density, temperature, frequency) @@ -48,9 +49,10 @@ For mean absorption opacities, the following functions are provided: | PlankMeanAbsorptionCoefficient | $n \sigma$ | Absorption coefficient | ${\rm cm}^{-1}$ | | RosselandMeanAbsorptionCoefficient | $n \sigma$ | Absorption coefficient | ${\rm cm}^{-1}$ | | AbsorptionCoefficient | $n \sigma$ | Absorption coefficient | ${\rm cm}^{-1}$ | -| Emissivity | $\int j_{\nu} d\nu d\Omega$ | Total emissivity | ${\rm erg~cm}^{-3}~{\rm s}^{-1}$ | +| Emissivity | $\int j_{\nu} d\nu d\Omega$ | Total emissivity | ${\rm erg}~{\rm cm}^{-3}~{\rm s}^{-1}$ | with the following function signatures: + PlanckMeanAbsorptionCoefficient(density, temperature) RosselandMeanAbsorptionCoefficient(density, temperature) AbsorptionCoefficient(density, temperature, gmode [Planck, Rosseland]) @@ -64,6 +66,7 @@ For frequency-dependent scattering opacities, the following functions are provid | TotalScatteringCoefficient | $ n \sigma $ | Scattering coefficient | ${\rm cm}^{-1}$ | with the following function signatures: + TotalCrossSection(density, temperature, frequency) DifferentialCrossSection(density, temperature, frequency, cos(theta)) TotalScatteringCoefficient(density, temperature, frequency) @@ -75,6 +78,7 @@ For mean scattering opacities, the following functions are provided: | RosselandMeanScatteringCoefficient | $n \sigma$ | Rosseland mean scattering coefficient | ${\rm cm}^{-1}$ | with the following function signatures: + PlanckMeanScatteringCoefficient(density, temperature) RosselandMeanScatteringCoefficient(density, temperature)