Правка разделов «Solution», «Answer»

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правка #19472 предыдущая #19428 ← раньше
@@ -19,31 +19,31 @@Solution
$$E_K = \frac{(\upsilon_1 - \upsilon_2)^2}{2(\frac{1}{m_1}+\frac{1}{m_2})}$$
−Finite velocities in the case of $\frac{(\upsilon_1 - \upsilon_2)^2}{(\frac{1}{m_1}+\frac{1}{m_2})} < \frac{2B^2 l S^2(3s - 2S)}{\mu_0 (S - s)(2S - s)}$:
+Finite velocities in the case of $\frac{(\upsilon_1 - \upsilon_2)^2}{(\frac{1}{m_1}+\frac{1}{m_2})} < \frac{2B^2 l S s^2}{\mu_0 (S - s)(2S - s)}$:
They are obtained by changing the sign of the speeds in the CM system and adding its speed:
$${\upsilon_1}' = \frac{2m_2\upsilon_2 + (m_1 - m_2)\upsilon_1}{m_1 + m_2}$$
$${\upsilon_2}' = \frac{2m_1\upsilon_1 + (m_2 - m_1)\upsilon_2}{m_1 + m_2}$$
−For the case of $\frac{(\upsilon_1 - \upsilon_2)^2}{(\frac{1}{m_1}+\frac{1}{m_2})} > \frac{2B^2 l S^2(3s - 2S)}{\mu_0(S - s)(2S - s)}$ speeds will remain the same:
+For the case of $\frac{(\upsilon_1 - \upsilon_2)^2}{(\frac{1}{m_1}+\frac{1}{m_2})} > \frac{2B^2 l S s^2}{\mu_0(S - s)(2S - s)}$ speeds will remain the same:
$${\upsilon_1}' = \upsilon_1$$
$${\upsilon_2}' = \upsilon_2$$
#### Answer
For:
−$$\frac{(\upsilon_1 - \upsilon_2)^2}{(\frac{1}{m_1}+\frac{1}{m_2})} < \frac{2B^2 l S^2(3s - 2S)}{\mu_0 (S - s)(2S - s)}$$
+$$\frac{(\upsilon_1 - \upsilon_2)^2}{(\frac{1}{m_1}+\frac{1}{m_2})} < \frac{2B^2 l S s^2}{\mu_0 (S - s)(2S - s)}$$
$${\upsilon_1}' = \frac{2m_2\upsilon_2 + (m_1 - m_2)\upsilon_1}{m_1 + m_2}$$
$${\upsilon_2}' = \frac{2m_1\upsilon_1 + (m_2 - m_1)\upsilon_2}{m_1 + m_2}$$
−For the case of $\frac{(\upsilon_1 - \upsilon_2)^2}{(\frac{1}{m_1}+\frac{1}{m_2})} > \frac{2B^2 l S^2(3s - 2S)}{\mu_0(S - s)(2S - s)}$ speeds will remain the same:
+For the case of $\frac{(\upsilon_1 - \upsilon_2)^2}{(\frac{1}{m_1}+\frac{1}{m_2})} > \frac{2B^2 l S s^2}{\mu_0(S - s)(2S - s)}$ speeds will remain the same:
$${\upsilon_1}' = \upsilon_1$$
$${\upsilon_2}' = \upsilon_2$$