Updated en 2.2.37, 2.2.44, 2.2.36, 2.2.39

astrosander правка от
правка #2512 предыдущая #2506 GitHub f9d1737 ← раньше позже →
@@ -49,50 +49,53 @@
<h3>Solution</h3>
<p>
+ Expression for the potential energy
$$
−u = \frac{kqQ}{r}
+U = \frac{kqQ}{r}
$$
$$
−u' = \frac{kqQ}{r} - \frac{kqQ}{R}
+U' = \frac{kqQ}{r} - \frac{kqQ}{R}
$$
+By statement, $R$ is a constant distance
$$
R = \text{const}
$$
−
+Derivatives for potential energy of expressions
$$
−(u_x)' = p
+(U_x)' = p
$$
$$
−(u)' = - \frac{kqQ}{r^2} \, dr
+(U)' = - \frac{kqQ}{r^2} \, dr
$$
$$
−(u')' = - \frac{kqQ}{r^2} \, dr
+(U')' = - \frac{kqQ}{r^2} \, dr
$$
+The derivative of the constant is zero
$$
(\text{const})' = 0 \Rightarrow (R)' = 0
$$
$$
−(u)' = (u')'!
+(U)' = (U')'!
$$
−
+Thus, the speeds remain unchanged and the motion of the particles is not affected
$$
−u = u'!
+V = V'!
$$
−$$
−\text{No, it won't!}
−$$
+
</p>
<h4>Answer</h4>
<p>
− No.
+ $
+\text{No, it won't!}
+$
</p>
<p style="text-align: right; font-style: italic; font-size: 14;">
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