Magnetic Force on Moving Parallel Plate Capacitor

AI Thread Summary
A parallel plate capacitor is moving at 31 m/s through a 4.0 T magnetic field, with an electric field of 170 N/C and plate area of 7.5 x 10^-4 m^2. To find the magnetic force on the positive plate, the charge must first be calculated using the relationship between electric field, charge density, and area. Applying Gauss's Law reveals that the electric field inside the capacitor is E = σ/ε₀, allowing for the determination of charge as q = 2.25 x 10^-12 C. Substituting this value into the magnetic force equation yields F = 2.79 x 10^-10 N, which was initially incorrect due to a misunderstanding of the electric field's contribution from both plates. Correcting the electric field calculation resolved the issue, confirming that the fields between the plates indeed add together.
jason.maran
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Homework Statement


The drawing shows a parallel plate capacitor that is moving with a speed of 31 m/s through a 4.0 T magnetic field. The velocity v is perpendicular to the magnetic field. The electric field within the capacitor has a value of 170 N/C and each plate has an area of 7.5 multiplied by 10 x 10^-4 m^2. What is the magnetic force (magnitude and direction) exerted on the positive plate of the capacitor?

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Homework Equations


F = Bqvsin(theta) --- sin() isn't important in this case because it's perpendicular

Then there's also E = F/q and C = KEoA/d, but I can't for the life of me figure out how to use it in this case.

The Attempt at a Solution


Well, I've established that I'm going to need to find the charge somehow from the electric field and the area of the plates, since all the other info for F = Bvq is given. I'm at a loss to figure out how to get the charge though... thanks in advance for any help/advice.
 

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You're completely correct. As it turns out, if you draw a Guassian cylinder or cube that extends halfway into one of the (conducting) capacitor plates and apply Gauss's Law, you'll find that the electric field from one plate is always \sigma/2\epsilon_0, where \sigma is the charge density of the plate (charge over area). If you add to this value the field from the other plate, you'll find that inside a parallel plate capacitor, the electric field always has a value of \sigma/\epsilon_0. So given your value for the electric field and the areas of the plates, you can now calculate the charge on the positive plate.
 
Thanks for your help, swuster. I'm still having a bit of trouble though.

I've done the following now:

E = (q/A)/2Eo
170 = (q/7.5e-4)/(2 * 8.85e-12)
q = 2.25e-12 C

Then I substitute in and solve for F:
F = qvB = (2.25e-12)(31)(4) = 2.79e-10 N, which is wrong, unfortunately.

I feel like I missed a step when following your instructions, and I didn't quite follow this bit:
If you add to this value the field from the other plate, you'll find that inside a parallel plate capacitor, the electric field always has a value of LaTeX Code: \\sigma/\\epsilon_0 .
Thanks again for the help, I appreciate it greatly! :)
 
jason.maran said:
E = (q/A)/2Eo

Should be:

E = (q/A)/Eo

^_^
 
Ah, OK, thanks a bunch! Worked like a charm after that!
 
Yep - between the capacitor plates, the electric field adds!
 
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