A plane electromagnetic wave of wavelength λ has an intensity I. It is propagating along the positive Y−direction. The allowed expressions for the electric and magnetic fields are given by
A
→E=√Iϵ0Ccos[2πλ(y−ct)]^i;→B=1cE^k
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B
→E=√Iϵ0Ccos[2πλ(y−ct)]^k;→B=−1cE^i
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C
→E=√2Iϵ0Ccos[2πλ(y−ct)]^k;→B=+1cE^i
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D
→E=√2Iϵ0Ccos[2πλ(y+ct)]^k;→B=1cE^i
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Solution
The correct option is C→E=√2Iϵ0Ccos[2πλ(y−ct)]^k;→B=+1cE^i E is the electric field vector, and B is the magnetic field vector of the EM wave. For electromagnetic waves E and B are always perpendicular to each other and perpendicular to the direction of propagation. The direction of propagation is the direction of E x B.
So, if the wave propagates in the +Y direction then the direction of E and B should be in +X and +Z or vice versa i.e +Z and +Xrespectively.
Case1.
Let us suppose →E is in ^i and →B is in ^k
Then →E×→B will be in −^j
Not Possible.
Case2.
Let us suppose →E is in ^k and →B is in ^i
Then →E×→B will be in ^j
This is satisfying option (3)
as the electric and magnetic field also propagate in positive y direction with time so (y−ct) should be there in wave equation.
Also I=cϵo2|Eo|2
|Eo|=√2Icϵo
From these, we can say that option (c) would be the best option.