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Posted

Fig. 21.16, on page 893, of Carroll & Ostlie's Intro. to Mod. Astrophys. [1st ed.], shows that (1) for stars more massive than [math]2 M_{\odot}[/math] (A5), Specific Angular Momentum (L/M) increases as M2/3; and, that (2) for stars less massive than said same value, the star's S.A.M. increases as M5 (with the deficit probably borne by planets, according to the caption). We seek an order-of-magnitude calculation, which can indicate some sort of suggestion, as to the origin of this [math]2 M_{\odot}[/math] threshold.

 

 

 

S.A.M. for massive stars

 

Please ponder an idealized Giant Molecular Cloud core, of constant density, from which a spherical fragment begins to collapse. The initial Angular Momentum of said spherical cloud at onset of collapse is:

 

[math]L = \frac{2}{5} M R^{2} \omega_{g} = \frac{2}{5} M \left(\frac{M}{\frac{4 \pi \rho}{3}}\right)^{2/3} \omega_{g}[/math]

 

And so:

 

[math]\frac{L}{M} = \frac{2}{5} \left(\frac{M}{\frac{4 \pi \rho}{3}}\right)^{2/3} \omega_{g} \propto M^{2/3}[/math]

 

Thus, it is completely consistent, w/ Carroll & Ostlie (ibid.), to consider the collapse of cloud cores as occurring in a constant density, and w/ a constant initial angular velocity (being [math]\omega_{g}[/math], the local galactic angular velocity, of rotation around the galactic center). More massive stars have higher S.A.M. merely b/c they "reach out farther" across the (quasi-)constant density cloud core, accumulating amounts of matter (dM) having higher & higher S.A.M. (dL ~ dM x R2).

 

Note that, at the threshold mass ([math]2 M_{\odot}[/math]), the S.A.M. is 1017.3 cm2 s-1, from which we can calculate the (effective) cloud core density, as:

 

[math]\rho = \left( \frac{2 \omega_{g}}{5 \frac{L}{M} } \right)^{3/2} M \frac{3}{4 \pi} \approx 7.3 \times 10^{-17} g \; cm^{-3}[/math]

 

Reassuringly, this value favorably compares w/ Carroll & Ostlie's figures for dense cloud cores (~10-16).

 

But, below the threshold mass value of [math]2 M_{\odot}[/math], more and more of that S.A.M. is missing from the central star (& seemingly deposited into a disk of protoplanets). Why would this be?


Merged post follows:

Consecutive posts merged

This author's investigation of Extra-solar Planetary Disks:

 

  • 2 weeks later...
Posted

From their figure 21.16, Specific Angular Momentum is the ratio of Angular Momentum to Mass, L / M. Since (ignoring coefficients) L = I w, and I = M R2, SAM has the units of R2 w (as you said).

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