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===== Introduction to Angular Momentum Lecture ( minutes)=====

{{courses:lecture:cflec:central_forces_notes.pdf|Central Forces Notes}} Section 6

  * Small whiteboard question: Write down something about angular momentum. Students are much more likely to remember $L = I \omega$, the specific formula for simple rigid body rotation, than the general definition, $\Vec L = \Vec{r} \times \Vec{p}$.
  * Begin with the idea that angular momentum is defined about a specific point. Always say the angular momentum of $x$ about the point $y$.
  * Often it is useful to include a small whiteboard question about the cross product to refresh students memories about the meaning/interpretation of the cross product in the equation $$ \Vec{L} = \Vec{r} \times \Vec{p}$$.
  * It is often useful to discuss the angular momentum for a particle moving in a straight line around a point off that line.
  * Derivation of the expression $$ {d{\Vec{L}}\over{d{t}}} = \Vec{r} \times \Vec{f} = \Vec{\tau}$$
  * Given a central force, $\Vec{\tau} = 0$ and $ {d{\Vec{L}}\over{d{t}}}$ is conserved.
  * Since angular momentum is conserved, the motion is in a plane.

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