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Home/Astronomy & The Sky/Chandrasekhar limit (Lane–Emden toy)

Chandrasekhar limit (Lane–Emden toy)

White-dwarf M–R track for n = 3/2 cold degenerate electrons; UR n = 3 marks the ~1.44 M☉ scale (μ_e dependent).

Equation of state (toy)

2

μ_e = 2 for C/O (typical WD), μ_e = 1 for pure H (unphysical as a WD but shows how M_Ch scales).

Central density sweep

6.8
10.4
9.1

Shortcuts

  • •Drag sliders — μ_e, log₁₀ ρ_c range, marker
  • •R — reset to defaults

Measured values

M_Ch (UR n = 3, Newtonian)1.456M☉
M at marker0.557M☉
R at marker1.694R⊕
ρ_c at marker1.259e+9kg m⁻³

About this model

This page uses the textbook Newtonian Lane–Emden model for a spherically symmetric star supported by a cold, completely degenerate electron gas. In the non-relativistic limit the pressure scales as P ∝ ρ^(5/3), corresponding to a polytrope of index n = 3/2. Homologous scaling along that sequence gives M ∝ ρ_c^(1/2) and R ∝ ρ_c^(−1/6) in Newtonian gravity. In the ultra-relativistic limit P ∝ ρ^(4/3) (n = 3), the Lane–Emden mass becomes independent of central density in Newtonian theory and sets the Chandrasekhar mass scale M_Ch ∝ (ħc/G)^(3/2)/(μ_e m_u)^2. General relativity, finite temperature, Coulomb corrections, and composition gradients change the numerical maximum to about 1.4 M☉ for carbon/oxygen white dwarfs; the plotted UR line is the Newtonian schematic (~1.45 M☉ at μ_e = 2).

Who it's for: Upper-level undergraduate astrophysics after degenerate matter and polytropes; pairs with neutron-star TOV and HR diagram pages.

Key terms

  • Chandrasekhar mass
  • white dwarf
  • Lane–Emden equation
  • polytrope
  • degenerate electrons
  • mean molecular weight per electron

How it works

A cold, spherically symmetric white dwarf is modeled as a Newtonian self-gravitating polytrope with P ∝ ρ^(5/3) from a non-relativistic T = 0 degenerate electron gas (Lane–Emden index n = 3/2). Along this sequence M ∝ ρ_c^(1/2) and R ∝ ρ_c^(−1/6), so more compact cores carry more mass in this toy EOS. The ultra-relativistic P ∝ ρ^(4/3) limit (n = 3) yields a mass plateau in Newtonian theory — the Chandrasekhar scale M_Ch ∝ μ_e^(−2) (here ~1.45 M☉ for μ_e = 2). General relativity and finite-temperature / composition effects move the physical maximum to ≈ 1.4 M☉; this page is schematic only.

Frequently asked questions

Why can the n = 3/2 track exceed the gold Chandrasekhar line?
The cyan curve is the Newtonian non-relativistic EOS only; it has no upper mass bound. Real stars need the relativistic crossover and GR, which cap the stable mass near ~1.4 M☉.
What is μ_e?
Electrons per baryon in the ionized bulk: μ_e = 2 for equal carbon and oxygen (one electron per two nucleons on average), lower for hydrogen-rich compositions in the same counting convention.