Added 2.3.48

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en/2.4.17.md +5 −1
@@ -85,7 +85,7 @@
E = \frac{M v_{cm}^2}{2}
\]
−Now, we need to prove that the **increment of energy of the motion of the center of mass** is equal to the work done by the total external force, assuming the point of application is the center of mass.
+Now, we need to prove that the increment of energy of the motion of the center of mass is equal to the work done by the total external force, assuming the point of application is the center of mass.
</p><p>
Let $ {F}_{\text{ext}} $ be the total external force acting on the system.</p><p>
@@ -123,6 +123,10 @@
This proves that the increment of the energy of motion of the center of mass is equal to the work done by the total external force, with the point of application taken at the center of mass.
</p>
+ <p style="text-align: right; font-style: italic; font-size: 14;">
+ Almaskhan Arsen<br>
+ </p>
+
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