Thermonuclear Fusion in the Sun and Other Stars — Question 8

Section 43-6 · Physics pages 7266–7267

Question 8 An intermediate helium abundance adjusts to balance production and destruction In a uniform stellar region let 3He number density n obey ˙n = S −2Kn2, where two 3He nuclei are consumed per fusion event. Take S = 2.00 × 1010 m−3s−1 and K = 10−20 m3/s. n rates S 2Kn2 Schematic; labels, not drawing lengths, specify the data. (a) Find equilibrium abundance and the rate of final helium-producing events there. (b) Linearize about equilibrium to find the relaxation time and determine stability.
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Question 8 - Solution An intermediate helium abundance adjusts to balance production and destruction n rates S 2Kn2 (a) Method and calculation S −2Kn2 eq = 0 ⇒neq = √ S/(2K) = 1015 m−3 . Req = Kn2 eq = S/2 = 1010 m−3s−1 . (b) Interpretation and further calculation n = neq + δn ⇒˙δn ≃−4Kneqδn. τ = (4Kneq)−1 = 2.50 × 104 s, δn ∝e−t/τ . Physical check The negative linear coefficient makes equilibrium stable. The factor two in abundance removal is essential even though each event produces only one final helium nucleus.

Question 8

An intermediate helium abundance adjusts to balance production and destruction

In a uniform stellar region let 3^3He number density n obey ṅ=S−2Kn2\dot n=S-2Kn^2, where two 3^3He nuclei are consumed per fusion event. Take S=2.00×1010m−3s−1S=2.00\times10^{10}\,\mathrm{m^{-3}s^{-1}} and K=10−20m3/sK=10^{-20}\,\mathrm{m^3/s}.

Diagram shown in the original SVG worksheet.

  1. Find equilibrium abundance and the rate of final helium-producing events there.

  2. Linearize about equilibrium to find the relaxation time and determine stability.

Question 8 - Solution

An intermediate helium abundance adjusts to balance production and destruction

Diagram shown in the original SVG worksheet.

(a) Method and calculation

S−2Kneq2=0⇒neq=S/(2K)=1015m−3.S-2Kn_{\mathrm{eq}}^2=0\Rightarrow\boxed{n_{\mathrm{eq}}=\sqrt{S/(2K)}=10^{15}\,\mathrm{m^{-3}}}.Req=Kneq2=S/2=1010m−3s−1.\boxed{R_{\mathrm{eq}}=Kn_{\mathrm{eq}}^2=S/2=10^{10}\,\mathrm{m^{-3}s^{-1}}}.

(b) Interpretation and further calculation

n=neq+δn⇒δṅ≃−4Kneqδn.n=n_{\mathrm{eq}}+\delta n\Rightarrow\dot{\delta n}\simeq-4Kn_{\mathrm{eq}}\delta n.τ=(4Kneq)−1=2.50×104s,δn∝e−t/τ.\boxed{\tau=(4Kn_{\mathrm{eq}})^{-1}=2.50\times10^4\,\mathrm s,\quad\delta n\propto e^{-t/\tau}}.

Physical check

The negative linear coefficient makes equilibrium stable. The factor two in abundance removal is essential even though each event produces only one final helium nucleus.