Dark Matter — Question 2

Section 44-12 · Physics pages 7514–7515

Question 2 Differentiating a flat-curve mass profile yields an inverse-square density For an ideal spherical halo with constant circular speed v0, use M(< r) = v2 0r/G and dM/dr = 4πr2ρ(r). r ρ Schematic; labels, not drawing lengths, specify the data. (a) Derive the density profile. (b) Find the density ratio at radii 10 and 30 kpc and explain why the model needs inner and outer limits.
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Question 2 - Solution Differentiating a flat-curve mass profile yields an inverse-square density r ρ (a) Method and calculation 4πr2ρ(r) = d(v2 0r/G)/dr = v2 0/G. ρ(r) = v2 0/(4πGr2) . (b) Interpretation and further calculation ρ(30)/ρ(10) = (10/30)2 = 1/9 . ρ →∞(r →0), M(< r) →∞(r →∞). Physical check The ideal profile is a local description over the observed flat part, not a globally physical halo with finite total mass.

Question 2

Differentiating a flat-curve mass profile yields an inverse-square density

For an ideal spherical halo with constant circular speed v0, use M(<r)=v02r/GM(<r)=v_0^2r/G and dM/dr=4πr2ρ(r)dM/dr=4\pi r^2\rho(r).

Diagram shown in the original SVG worksheet.

  1. Derive the density profile.

  2. Find the density ratio at radii 10 and 30 kpc and explain why the model needs inner and outer limits.

Question 2 - Solution

Differentiating a flat-curve mass profile yields an inverse-square density

Diagram shown in the original SVG worksheet.

(a) Method and calculation

4πr2ρ(r)=d(v02r/G)/dr=v02/G.4\pi r^2\rho(r)=d(v_0^2r/G)/dr=v_0^2/G.ρ(r)=v02/(4πGr2).\boxed{\rho(r)=v_0^2/(4\pi Gr^2)}.

(b) Interpretation and further calculation

ρ(30)/ρ(10)=(10/30)2=1/9.\boxed{\rho(30)/\rho(10)=(10/30)^2=1/9}.ρ→∞(r→0),M(<r)→∞(r→∞).\rho\to\infty\ (r\to0),\quad M(<r)\to\infty\ (r\to\infty).

Physical check

The ideal profile is a local description over the observed flat part, not a globally physical halo with finite total mass.