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Induced electric field |
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| Dec11-12, 01:13 PM | #1 |
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Induced electric field
Can electric field be induced at a point near a time varying uniform magnetic field? "Near" means not the in the place where magnetic field exist. But at a point outside the field's presence.
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| Dec11-12, 05:03 PM | #2 |
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You can induce electric fields everywhere. Why do you expect that it would not be possible somewhere?
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| Dec12-12, 12:12 PM | #3 |
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Recognitions:
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A time varying magnetic field will have time varying vector potential [tex]\frac{\partial{\bf A}}{\partial t}[/tex] that can exist beyond the field, and induce an E field. This is like the 'Aharonov-Bohm' effect. |
| Dec12-12, 12:42 PM | #4 |
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Induced electric field
Yes. Say, for example, there's a long solenoid with a time-varying current I(t) running through it. The resulting magnetic field is nonzero only inside the solenoid. However, (assuming ∂B/∂t isn't zero) the electric field induced will also be nonzero outside of the solenoid.
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| Dec12-12, 02:04 PM | #5 |
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Mentor
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| Dec13-12, 01:08 AM | #6 |
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Take a circular area beyond the region of changing magnetic field,but it should include changing magnetic field area then
E.2∏R=-∏r2.∂B/∂t,E is induced in region beyond WHERE B changes. |
| Dec13-12, 03:53 PM | #7 |
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Recognitions:
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This gives an A outside the solenoid, where there is no B. |
| Dec13-12, 03:59 PM | #8 |
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I don't see how your quote and your post are related. You can get a non-zero A everywhere if you like - even in a perfect vacuum, as you have gauge freedom. But you do not get an electric field without a changing magnetic field or some charge distribution.
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| Dec13-12, 04:24 PM | #9 |
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| Dec13-12, 04:47 PM | #10 |
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Mentor
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$$curl(B)=\frac{1}{c}\frac{\partial E}{\partial t} + \frac{4\pi}{c} j$$ You do not want currents and no magnetic field? => electric field is time-invariant. You cannot switch it on or off. This means that a time-independent charge distribution (which might consist of moving charges) is the only relevant option for a source of an electric field. |
| Dec13-12, 05:56 PM | #11 |
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Evaluating the integral ∫E∙ds=-∂/∂t ∫B∙dA ⇔ E=-μ0na2 I'(t) / 2r Even though B=0 outside the solenoid, it still produces a nonzero E outside the solenoid. |
| Dec13-12, 06:30 PM | #12 |
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Sorry, I shouldn't be mean about it. It is a bit counter-intuitive. But yeah, if you take an infinitely-long solenoid, the magnetic field is ONLY present inside the solenoid. Yet you can wrap another solenoid around it, and induce a current on it by time-varying the current on the inner-solenoid. The B-field outside remains zero, but E-field is non-zero. This all has to do with curl of the electric field being governed by ∂B/∂t. Outside of the solenoid, both curl and divergence of E is zero, but it doesn't mean that the field itself is zero. Feel free to verify that circular E field with 1/R intensity satisfies conditions of both curl and divergence being zero. (In other words for [itex]E = E_0\frac{\hat{\phi}}{r}[/itex], [itex]\nabla \cdot E = 0[/itex] and [itex]\nabla \times E = 0[/itex] everywhere except r=0.) |
| Dec14-12, 02:06 AM | #13 |
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I have shown in post no.6 that even outside a solenoid if one take a circular area and if it encloses the region of changing magnetic field then electric field will be induced at far distances also.
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| Dec14-12, 07:50 AM | #14 |
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Ah ok, you are right. So we need a coil of infinite length, where B(t) changes linear in time. This gives a constant (in time), circular E(t) and no magnetic field outside.
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| Dec20-12, 09:35 AM | #15 |
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then..how will a time varying electric field induce magnetic field and where?
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| electro magnetism, faraday's law |
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