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Electromagnetic Field Theory

Electromagnetic Field Theory
The frequency of the power wave associated with an electromagnetic wave having field as E = e-z/δ cos(ω - zδ) is given by

 ω.
 ω / π.
 ω/4π.
 ω/2π.

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Electromagnetic Field Theory
A plane wave magnetic field is represented by Bx = cos(y – ct). The electric and magnetic fields will be zero in the direction

 Ex = Ey = 0, Bx = By = 0.
 None of these.
 Ex = Ey = 0, By = Bz = 0.
 Ey = Ez = 0, By = Bz = 0.

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Electromagnetic Field Theory
For an inductor, current is proportional to

 none of them.
 magnetic field.
 both (A) and (B).
 voltage across the inductor.

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Electromagnetic Field Theory
XEROX machine is working on

 magnetic effect.
 peltier effect.
 heating effect of current.
 electrostatic effect.

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Electromagnetic Field Theory
In case of surface waves the field strength at a point is directly proportional to

Antenna height
Distance of the point from the antenna
Wave frequency
Current of the antenna

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Electromagnetic Field Theory
An electric dipole of moment P is placed in front of a ground sphere. The change induced on the surface of the sphere is (Assume radius of sphere = R and distance from dipole to centre of sphere = d)

 PR/d.
 Zero.
 PR/d2.
 PR 2/d3.

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