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Classical Angular Momentum
Prerequisites
Students should be able to:
In-class Content
- Add Angular Momentum SWBQs
- Introduction of Angular Momentum (Lecture, 25 minutes)
- Central Forces on an Air Table (Small Whiteboard Activity, 15 minutes)
- RESOURCE: Spherical coordinates handout showing unit vectors.
Homework for Central Forces
- (CentralForce) Determine whether several common forces in nature are central forces.
Which of the following forces can be central forces? which cannot?
The force on a test mass $m$ in a gravitational field $\Vec{g }$, i.e. $m\Vec g$
The force on a test charge $q$ in an electric field $\Vec E$, i.e. $q\Vec E$
The force on a test charge $q$ moving at velocity $\Vec{v }$ in a magnetic field $\Vec B$, i.e. $q\Vec v \times \Vec B$
- (FreeCentralForce) A simple check on your understanding of center-of-mass motion.
If a central force is the only force acting on a system of two masses (i.e. no external forces), what will the motion of the center of mass be?
- (PlanarOrbit) A simple check on your understanding of classical angular momentum.}
Show that the plane of the orbit is perpendicular to the angular momentum vector $\Vec L$.
- (CMLandT) Explicitly show how the kinetic energy and angular momentum of a two particle system is related to the energy and angular momentum of the center of mass and reduced mass system.
Consider a system of two particles.
Show that the total kinetic energy of the system is the same as that of two “fictitious” particles: one of mass $M=m_1+m_2$ moving with the speed of the CM (center of mass) and one of mass $\mu$ (the reduced mass) moving with the speed of the relative position $\vec{r}=\vec{r}_2-\vec{r}_1$.
Show that the total angular momentum of the system can be similarly decomposed into the angular momenta of these two fictitious particles.