Students should be able to:
Reading: GVC § Independence of Path–Finding potential Functions
The gravitational field due to a spherical shell of mass is given by: %/* \[ \Vec g =\begin{cases}
0&r<b\\
-\frac{4}{3}\pi\rho\,G\left({r}-{b^3\over r^2}\right)\hat{r}&b<r<a\\ -\frac{4}{3}\pi\rho\, G\left({a^3-b^3\over r^2}\right)\hat{r}&a<r\\
\end{cases}
\]
where $b$ is the inside radius of the shell, $a$ is the outside radius of the shell, and $\rho$ is the constant mass density.
Using an explicit line integral, calculate the work required to bring the test mass along the same path, from infinity to the point $Q$ a distance $d$ (where $b<d<a$) from the center of the shell.
Using an explicit line integral, calculate the work required to bring the test mass along the same radial path from infinity all the way to the center of the shell.
(Throughout this problem, assume all of the constants-including invisible factors of 1-carry the necessary dimensions so that the fields in this problem are dimensionally correct.) Consider the vector field in rectangular coordinates: $$\vec{E} = \frac{q}{4 \pi \epsilon_{0}} [(2 x y^3z+z)\hat{x} + (3x^2 y^2 z) \hat{y}+(x^2 y^3+x)\hat{z}]$$
Using only the $x$-component of $\vec{E}$, find as much information as possible about the potential from which this electric field might have come.
Repeat this exercise for the $y$- and $z$-components of $\vec{E}$. Does this field come from a potential?
Consider the different vector field: $$\vec{E} = \frac{q}{4 \pi \epsilon_{0}} (-y \hat{x} + x \hat{y})$$ Does this field come from a potential?
Consider the different vector field: $$\vec{E}=\frac{q}{4 \pi \epsilon_{0}} \left(s \hat{\phi}\right)$$ Does this field come from a potential?