Induced EMF on a moving rod next to a line of current.

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SUMMARY

The discussion focuses on calculating the induced electromotive force (emf) in a copper rod moving parallel to a long straight wire carrying a current. Given parameters include a velocity (v) of 5.0 m/s, a current (i) of 100 A, and distances a = 1 cm and b = 20 cm. The correct induced emf is calculated using the formula ε = -μ₀iv/(2π)(b-a)ln(b/a), leading to an answer of 3.0 x 10-4 V. Participants clarify the distinction between magnetic field and magnetic flux, emphasizing the importance of precise terminology in electromagnetic calculations.

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  • Understanding of electromagnetic theory, specifically induced emf
  • Familiarity with the Biot-Savart Law and magnetic fields
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grindfreak
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Homework Statement



I'm currently reviewing some of the old E&M material that I haven't seen in a while and have gotten stuck on this problem. I'm sure I'm just making a simple mistake but I can't seem to make any headway.

Here's the problem: Figure 35-32 shows a copper rod moving with velocity v parallel to a long straight wire carrying a current i. Calculate the induced emf in the rod, assuming v = 5.0m/s, i = 100A, a = 1cm and b = 20cm. Answer: 3.0X10-4V


The Attempt at a Solution



The magnetic field of the wire a distance y away is B = \frac{\mu _{0}i}{2\pi y}. Thus the total magnetic field across the length of the rod is B = \frac{\mu_{0}i}{2\pi}\int_{a}^{b}\frac{dy}{y} = \frac{\mu_{0}i}{2\pi}ln\frac{b}{a}. Now the induced emf is \varepsilon = -\frac{d\Phi _{B}}{dt}=-B\frac{dA}{dt}=-B(b-a)\frac{dx}{dt}=-B(b-a)v. Then the total equation is \varepsilon = \frac{-\mu_{0}iv}{2\pi}(b-a)ln\frac{b}{a}, the only problem being that this is apparently not the correct answer.

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hi grindfreak! :smile:
grindfreak said:
Now the induced emf is \varepsilon = -\frac{d\Phi _{B}}{dt}=-B\frac{dA}{dt}=-B(b-a)\frac{dx}{dt}=-B(b-a)v.

i don't understand this at all :confused:

yes, the area swept out in time t is A = (b-a)vt

but the magnetic flux through that area is ∫ab B(y)vt dy,

ie your previous integral times vt

how did you get that (b-a) factor?
Thus the total magnetic field across the length of the rod is B = \frac{\mu_{0}i}{2\pi}\int_{a}^{b}\frac{dy}{y} = \frac{\mu_{0}i}{2\pi}ln\frac{b}{a}.

whatever is "total magnetic field"?? :confused:

if you mean the flux, then say so, and don't call it "B" !

your strange nomenclature seems to have confused you
 
Yes I think your first integral is probably the right way to go with it, the b-a factor is the length of the rod, so that (b-a)*x is the area swept out by the rod in time t. As for total magnetic field, I really should have said magnetic field on the rod by the line of current (sorry if this sounds a bit poorly worded, I've been working all day).
 
sorry, but you're not making much sense

get some sleep :zzz:, and it'll be clearer in the morning :smile:
 
I checked my equation again and you're correct, I don't know why I used BA for the magnetic flux.
 

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