INGENIA

AST-17

Saha ionisation snapshot

n_{i+1} n_e / n_i = (kT / λ_th³) exp(−χ / kT) (g-factor = 1 sketch).

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StarsSaha

Governing equation

ni+1neni=(2πmkTh2)3/2e−χ/kT\dfrac{n_{i+1}n_e}{n_i}=\left(\dfrac{2\pi m kT}{h^2}\right)^{3/2}e^{-\chi/kT}

T∈[3000,30000]T \in \left[3000, 30000\right]

where

T
Temperature (K)
\chi
Ionisation (eV)
n_e
Electron density (10¹⁸/m³)
n_{i+1}/n_i
Ion ratio (—)

The figure, part by part

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AST-17 · spectrum
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①

Governing law — red

ni+1neni=(2πmkTh2)3/2e−χ/kT\dfrac{n_{i+1}n_e}{n_i}=\left(\dfrac{2\pi m kT}{h^2}\right)^{3/2}e^{-\chi/kT}

T∈[3000,30000]T \in \left[3000, 30000\right]

T=3000T = 3000ni+1/ni=5.64×10−15n_{i+1}/n_i = 5.64\times 10^{-15}

②

Domain of the variable — blue

Tmin⁡=3000,Tmax⁡=30000T_{\min} = 3000,\quad T_{\max} = 30000

T∈[3000,30000]T \in \left[3000, 30000\right]

T=3000T = 3000T=3000T = 3000

③

Response curve — green

ni+1neni=(2πmkTh2)3/2e−χ/kT\dfrac{n_{i+1}n_e}{n_i}=\left(\dfrac{2\pi m kT}{h^2}\right)^{3/2}e^{-\chi/kT}

T∈[3000,30000]T \in \left[3000, 30000\right]

T=3000T = 3000ni+1/ni=5.64×10−15n_{i+1}/n_i = 5.64\times 10^{-15}

④

Rate of change — amber

dni+1/nidT\frac{\mathrm{d}n_{i+1}/n_i}{\mathrm{d}T}

T∈[3000,30000]T \in \left[3000, 30000\right]

T=3169.8T = 3169.8ni+1/ni′=4.09×10−15n_{i+1}/n_i^{\prime} = 4.09\times 10^{-15}

Lecture brief

Historical brief

Hubble expansion, Jeans collapse, Eddington luminosity, Bondi accretion and Stefan–Boltzmann stars are the first astrophysical budgets. The sheets scale a star, a cloud and a horizon. This sheet (AST-17 — Saha ionisation snapshot) is the form associated with Saha. Working symbols: TT, χ\chi, nen_e →\rightarrow ni+1/nin_{i+1}/n_i. Why Balmer lines peak around A0: hydrogen ionises, then the n=2 population falls.

Purpose

Purpose: compute ni+1/nin_{i+1}/n_i from TT, χ\chi, nen_e in Astrophysics via ni+1neni=(2πmkTh2)3/2e−χ/kT\dfrac{n_{i+1}n_e}{n_i}=\left(\dfrac{2\pi m kT}{h^2}\right)^{3/2}e^{-\chi/kT} n_{i+1} n_e / n_i = (kT / λ_th³) exp(−χ / kT) (g-factor = 1 sketch). Use it when a real astrophysics question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given T=10000.000 KT = 10000.000\,\mathrm{K}, χ=13.600 eV\chi = 13.600\,\mathrm{eV}, ne=1.000 1018/m3n_e = 1.000\,\mathrm{10¹⁸/m^{3}}, the governing relation ni+1neni=(2πmkTh2)3/2e−χ/kT\dfrac{n_{i+1}n_e}{n_i}=\left(\dfrac{2\pi m kT}{h^2}\right)^{3/2}e^{-\chi/kT} yields ni+1/ni=337.8795 —n_{i+1}/n_i = 337.8795\,\mathrm{—}. A star atmosphere, two ion stages, a ratio. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Ion ratio n_{i+1}/n_i337.8795 —
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AST-17 · spectrum
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Narration of this film

A star atmosphere, two ion stages, a ratio.

Why Balmer lines peak around A0: hydrogen ionises, then the n=2 population falls.

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