Постоянная роста массы

Last modified by Alexey Popov on 2022/03/15 20:13

$\mathbf a = \frac{4}{3}\pi G\rho_u \mathbf R = \mathbf R H_0^2$

$\mathbf a = -G \frac{M}{R^2}+ \frac{4}{3}\pi G\rho_u \mathbf R$

$\varphi = \frac{4}{3}\pi G\rho_u R^2$

$\mathbf v = \mathbf R\sqrt{\frac{4}{3}\pi G\rho_u}$

$H_0 = \sqrt{\frac{4}{3}\pi G\rho_u}$

$\mathbf v = \mathbf R\sqrt{\frac{4}{3}\pi G\rho_u} = \mathbf R H_0$

$H_0 = \sqrt{\frac{4}{3}\pi \frac{G}{H_n}\rho_u H_n} = \sqrt{\frac{4}{3}\pi \frac{\omega_n}{\rho_n}\rho_u H_n}$

$H_0^2 = \frac{4}{3}\pi \frac{\omega_n}{\rho_n}\rho_u H_n$

$\mathbf v = \frac{4}{3}\pi \frac{\omega_n}{\rho_n}\rho_u \mathbf R$

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Created by Alexey Popov on 2022/01/18 13:07

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