bn:un:tidal-force
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| bn:un:tidal-force [2025/08/11 04:24] – [4. জায়ান্ট গ্রহদের রিং] asad | bn:un:tidal-force [2025/08/11 04:25] (current) – [4. জায়ান্ট গ্রহদের রিং] asad | ||
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| - | ===== - জায়ান্ট গ্রহদের রিং ===== | ||
| - | $$ | ||
| - | \begin{aligned} | ||
| - | F_{\text{tidal}} &\simeq \frac{2 G M_p R_m}{r^3} \\[4pt] | ||
| - | \frac{G M_m}{R_m^{2}} &= \frac{2 G M_p R_m}{r^3} \\[4pt] | ||
| - | \Rightarrow\ \frac{M_m}{R_m^{2}} &= \frac{2 M_p R_m}{r^3} \\[4pt] | ||
| - | M_m &= \frac{4}{3}\pi R_m^{3}\rho_m, | ||
| - | \Rightarrow\ \frac{\frac{4}{3}\pi R_m^{3}\rho_m}{R_m^{2}} &= \frac{2\left(\frac{4}{3}\pi R_p^{3}\rho_p\right)R_m}{r^{3}} \\[4pt] | ||
| - | \Rightarrow\ \frac{4}{3}\pi R_m \rho_m &= \frac{8}{3}\pi \frac{R_p^{3}\rho_p R_m}{r^{3}} \\[4pt] | ||
| - | \Rightarrow\ \rho_m &= 2\, | ||
| - | \Rightarrow\ r^{3} &= 2\, | ||
| - | \therefore\quad r_{\text{crit}} &= 2^{1/ | ||
| - | r_{\text{crit}} & | ||
| - | \end{aligned} | ||
| - | $$ | ||
bn/un/tidal-force.1754907893.txt.gz · Last modified: by asad
