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bn:un:tidal-force [2025/08/11 04:09] asadbn:un:tidal-force [2025/08/11 04:25] (current) – [4. জায়ান্ট গ্রহদের রিং] asad
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 {{https://media.springernature.com/full/springer-static/image/art%3A10.1038%2Fs41598-022-14469-3/MediaObjects/41598_2022_14469_Fig1_HTML.png?nolink}}  {{https://media.springernature.com/full/springer-static/image/art%3A10.1038%2Fs41598-022-14469-3/MediaObjects/41598_2022_14469_Fig1_HTML.png?nolink}} 
  
-===== - এঙ্গুলার মোমেন্টাম ===== +===== - আর্থ-মুন এঙ্গুলার মোমেন্টাম =====
 $$ $$
 \begin{aligned} \begin{aligned}
-&= \frac{2}{5} M_e R_e^2 \,\omega_e + \mu_m d^2 \Omega_m \\ +\mu_m &= \frac{M_e M_m}{M_e + M_m} \\[4pt] 
-\Omega_m^2 &= \frac{G\,(M_e+M_m)}{d^3} \\ +I_e &= \frac{2}{5} M_e R_e^2 \\[4pt] 
-\Rightarrow\ \Omega_m &= \sqrt{\frac{G\,(M_e+M_m)}{d^3}} \\ +J &= I_e\,\omega_e + \mu_m d^2 \Omega_m \\[4pt] 
-\Rightarrow\ \mu_m d^2 \Omega_m &= \mu_m d^2 \sqrt{\frac{G\,(M_e+M_m)}{d^3}} \\ +P^2 &= \frac{4\pi^2 a^3}{G(M_e+M_m)} \\[2pt] 
-&= \mu_m \sqrt{\frac{d^4 G\,(M_e+M_m)}{d^3}} \\ +\Omega_m &= \frac{2\pi}{P} \\[2pt] 
-&= \mu_m \sqrt{\,d\, G\,(M_e+M_m)} \\+\Rightarrow\ \Omega_m^2 &= \frac{4\pi^2}{P^2} 
 +\frac{4\pi^2}{\dfrac{4\pi^2 a^3}{G(M_e+M_m)}} 
 +\frac{G(M_e+M_m)}{a^3} \\[2pt] 
 +a&=d \\[2pt] 
 +\Rightarrow\ \Omega_m^2 &= \frac{G(M_e+M_m)}{d^3} \\[4pt] 
 +\mu_m d^2 \Omega_m &= \mu_m d^2 \sqrt{\frac{G(M_e+M_m)}{d^3}} 
 += \mu_m \sqrt{\frac{d^4\,G(M_e+M_m)}{d^3}} 
 += \mu_m \sqrt{d\,G(M_e+M_m)} \\[4pt]
 \therefore\quad \therefore\quad
-J &= \frac{2}{5} M_e R_e^2 \,\omega_e + \mu_m \sqrt{\,d\, G\,(M_e+M_m)} \,.+J &= \frac{2}{5} M_e R_e^2\,\omega_e + \mu_m \sqrt{d\,G(M_e+M_m)} \,.
 \end{aligned} \end{aligned}
 $$ $$
 +
 +===== - মার্কারির স্পিন-অর্বিট রেজোনেন্স =====
 +৩ঃ২
 +
 +===== - জুপিটারের মুন =====
 +{{https://upload.wikimedia.org/wikipedia/commons/e/e5/Galilean_moon_Laplace_resonance_animation_2.gif?nolink}}
  
  
bn/un/tidal-force.1754906991.txt.gz · Last modified: by asad

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