- #1
eko_n2
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Homework Statement
The problem is #1 given here:
http://ocw.mit.edu/courses/physics/8-311-electromagnetic-theory-spring-2004/assignments/ps1.pdf
And there is a solution publicly available here:
http://ocw.mit.edu/courses/physics/8-311-electromagnetic-theory-spring-2004/assignments/solution1.pdf
In short, a conducting sphere is being charged through a straight wire with given current I. You are asked to find the displacement current, and finally the magnetic field.
My question pertains to finding the magnetic field - I don't understand how the displacement current was used to find the magnetic field.
Homework Equations
The displacement current was found to be:
j_d = \frac{I}{4 \pi r^2} \hat{r}
To find the magnetic field, use
\int B \cdot dl = \frac{4\pi}{c} \int j \cdot \hat{n} dA
where j is the current density and n is the unit vector normal to the surface.
The Attempt at a Solution
For the contour, we consider a loop about the axis of the wire (there is a figure in the solutions). The distance from the center of the sphere to the loop is r. The angle between the loop and the axis of the wire is θ.
On the left hand side, we thus have
\int B \cdot dl = 2 \pi r \sin{(\theta)} B
The surface we are using for the right hand side is a section of a sphere of radius r. So we need to integrate the displacement current (since there is no actual current through this surface, only displacement) over this region:
\frac{4\pi}{c} \int j \cdot \hat{n} dA = \frac{4\pi}{c} \int_0^{2\pi} d\phi \int_0^{\theta'} d\theta \sin{\theta} \frac{I}{4 \pi r^2} \hat{r} \cdot \hat{r}
= \frac{2\pi I}{c r^2} (1-\cos \theta)
Combine this with the left hand side from above:
2 \pi r \sin{(\theta)} B = \frac{2\pi I}{c r^2} (1-\cos \theta)
B = \frac{I}{c r^3 \sin{\theta}} (1-\cos \theta)
Finally, the question: why is the answer in the solutions given off by a factor r^2? Why does this factor from the displacement current disappear in the worked solutions?
Thanks for the help
Edit: the given solution is
B = \frac{(1-\cos \theta) I}{cr \sin \theta}