Consider a charged capacitor placed in a uniform B field in the $+y$ direction. $z$ points along the capacitor axis, so that $x$ points upward.

Which way does the stored field momentum in this system point?

1. $\pm \hat{x}$
2. $\pm \hat{y}$
3. $\pm \hat{z}$
4. Zero!

Now "short out" this capacitor with a small wire. As the current flows, (while the capacitor is discharging)...

which way does the magnetic force push the wire (and thus, the system)?

1. $\pm \hat{x}$
2. $\pm \hat{y}$
3. $\pm \hat{z}$
4. Zero!

Feynman’s Paradox: Two charged balls are attached to a horizontal ring that can rotate about a vertical axis without friction. A solenoid with current I is on the axis. Initially, everything is at rest.

The current in the solenoid is turned off. What is the direction of the induced $\mathbf{E}$ when viewed from the top?

1. 0
2. CW.
3. CCW.

Feynman’s Paradox: Two charged balls are attached to a horizontal ring that can rotate about a vertical axis without friction. A solenoid with current I is on the axis. Initially, everything is at rest.

The current in the solenoid is turned off. What happens to the charges?

1. They remain at rest
2. They rotate CW.
3. They rotate CCW.

Does the Feynman device violate Conservation of Angular Momentum?

1. Yes
2. No
3. Neither, Cons of Ang Mom does not apply in this case.

A function, $f(x,t)$, satisfies this PDE:

$$\dfrac{\partial^2 f}{\partial x^2} = \dfrac{1}{c^2}\dfrac{\partial^2 f}{\partial t^2}$$

Invent two different functions $f(x,t)$ that solve this equation. Try to make one of them "boring" and the other "interesting" in some way.

A function, $f(x,t)$, satisfies this PDE:

$$\dfrac{\partial^2 f}{\partial x^2} = \dfrac{1}{c^2}\dfrac{\partial^2 f}{\partial t^2}$$

Which of the following functions work?

1. $\sin( k(x – vt))$
2. $exp( k(-x – vt ))$
3. $a( x + vt )^3$
4. All of these.
5. None of these.