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Electromagnetic Waves question

2016 · 10 Apr · Shift 1 · Q43
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Electromagnetic Waves question

2016 · 10 Apr · Shift 1 · Q43

JEE MainPhysicsElectromagnetic WavesMCQ+4 / −1
Consider an electromagnetic wave propagating in vacuum. Choose the correct statement :
  1. A
    For an electromagnetic wave propagating in +x direction the electric field is E⃗=12Eyz (x,t)(y^−z^)\vec E = {1 \over {\sqrt 2 }}{E_{yz}}{\mkern 1mu} \left( {x,t} \right)\left( {\hat y - \hat z} \right)E=2​1​Eyz​(x,t)(y^​−z^) and the magnetic field is B⃗=12Byz (x,t)(y^+z^)\vec B = {1 \over {\sqrt 2 }}{B_{yz}}{\mkern 1mu} \left( {x,t} \right)\left( {\hat y + \hat z} \right)B=2​1​Byz​(x,t)(y^​+z^)
  2. B
    For an electromagnetic wave propagating in +x direction the electric field is E⃗=12Eyz (y,z,t)(y^+z^)\vec E = {1 \over {\sqrt 2 }}{E_{yz{\mkern 1mu} }}\left( {y,z,t} \right)\left( {\hat y + \hat z} \right)E=2​1​Eyz​(y,z,t)(y^​+z^) and the magnetic field is B⃗=12Byz (y,z,t)(y^+z^)\vec B = {1 \over {\sqrt 2 }}{B_{yz{\mkern 1mu} }}\left( {y,z,t} \right)\left( {\hat y + \hat z} \right)B=2​1​Byz​(y,z,t)(y^​+z^)
  3. C
    For an electromagnetic wave propagating in + y direction the electric field is E→=12Eyz (x,t)y^\overrightarrow E = {1 \over {\sqrt 2 }}{E_{yz{\mkern 1mu} }}\left( {x,t} \right)\widehat yE=2​1​Eyz​(x,t)y​ and the magnetic field is B⃗=12Byz (x,t)z^\vec B = {1 \over {\sqrt 2 }}{B_{yz{\mkern 1mu} }}\left( {x,t} \right)\widehat zB=2​1​Byz​(x,t)z
  4. D
    For an electromagnetic wave propagating in + y direction the electric field is E→=12Eyz (x,t)z^\overrightarrow E = {1 \over {\sqrt 2 }}{E_{yz{\mkern 1mu} }}\left( {x,t} \right)\widehat zE=2​1​Eyz​(x,t)z and the magnetic field is B→=12Bz (x,t)y^\overrightarrow B = {1 \over {\sqrt 2 }}{B_{z{\mkern 1mu} }}\left( {x,t} \right)\widehat yB=2​1​Bz​(x,t)y​
View written solutionFree

Correct answer: A

  1. Conditions for an electromagnetic wave in vacuum

For an electromagnetic wave in vacuum:

  • E⃗⊥B⃗\vec E \perp \vec BE⊥B
  • Both E⃗\vec EE and B⃗\vec BB are perpendicular to the direction of propagation.
  • The direction of propagation is along E⃗×B⃗\vec E \times \vec BE×B.
  • Also, in vacuum, fields depend on the propagation coordinate and time, e.g. for propagation along +x+x+x, fields are functions of (x,t)(x,t)(x,t).

  1. Check option A

Given:

E⃗=12Eyz(x,t)(y^−z^),B⃗=12Byz(x,t)(y^+z^)\vec E = \frac{1}{\sqrt 2} E_{yz}(x,t)(\hat y - \hat z), \qquad \vec B = \frac{1}{\sqrt 2} B_{yz}(x,t)(\hat y + \hat z)E=2​1​Eyz​(x,t)(y^​−z^),B=2​1​Byz​(x,t)(y^​+z^)

(i) Are E⃗\vec EE and B⃗\vec BB perpendicular?

Compute dot product of direction vectors:

(y^−z^)⋅(y^+z^)=y^⋅y^+y^⋅z^−z^⋅y^−z^⋅z^(\hat y - \hat z) \cdot (\hat y + \hat z) = \hat y\cdot\hat y + \hat y\cdot\hat z - \hat z\cdot\hat y - \hat z\cdot\hat z(y^​−z^)⋅(y^​+z^)=y^​⋅y^​+y^​⋅z^−z^⋅y^​−z^⋅z^ =1+0−0−1=0= 1 + 0 - 0 - 1 = 0=1+0−0−1=0

So, E⃗⊥B⃗\vec E \perp \vec BE⊥B.

(ii) Direction of propagation

(y^−z^)×(y^+z^)(\hat y - \hat z) \times (\hat y + \hat z)(y^​−z^)×(y^​+z^)

Expand:

=y^×y^+y^×z^−z^×y^−z^×z^= \hat y\times\hat y + \hat y\times\hat z - \hat z\times\hat y - \hat z\times\hat z=y^​×y^​+y^​×z^−z^×y^​−z^×z^ =0+x^−(−x^)−0=2x^= 0 + \hat x - (-\hat x) - 0 = 2\hat x=0+x^−(−x^)−0=2x^

Thus,

E⃗×B⃗∥+x^\vec E \times \vec B \parallel +\hat xE×B∥+x^

So the wave propagates in +x+x+x direction, exactly as stated.

(iii) Functional dependence

Since propagation is along +x+x+x, dependence on (x,t)(x,t)(x,t) is correct.

So, Option A is correct.


  1. Check option B

Given:

E⃗=12Eyz(y,z,t)(y^+z^),B⃗=12Byz(y,z,t)(y^+z^)\vec E = \frac{1}{\sqrt 2} E_{yz}(y,z,t)(\hat y + \hat z), \qquad \vec B = \frac{1}{\sqrt 2} B_{yz}(y,z,t)(\hat y + \hat z)E=2​1​Eyz​(y,z,t)(y^​+z^),B=2​1​Byz​(y,z,t)(y^​+z^)

Here E⃗\vec EE and B⃗\vec BB are along the same direction (y^+z^)(\hat y+\hat z)(y^​+z^), so they are not perpendicular.

But in an electromagnetic wave, E⃗⊥B⃗\vec E \perp \vec BE⊥B.

Also, for propagation along +x+x+x, fields should depend on (x,t)(x,t)(x,t), not generally on (y,z,t)(y,z,t)(y,z,t).

So, Option B is incorrect.


  1. Check option C

Given for propagation in +y+y+y direction:

E⃗=12Eyz(x,t)y^,B⃗=12Byz(x,t)z^\vec E = \frac{1}{\sqrt 2} E_{yz}(x,t)\hat y, \qquad \vec B = \frac{1}{\sqrt 2} B_{yz}(x,t)\hat zE=2​1​Eyz​(x,t)y^​,B=2​1​Byz​(x,t)z^

For propagation along +y+y+y, both fields must be perpendicular to y^\hat yy^​.

But here E⃗\vec EE is along y^\hat yy^​, i.e. parallel to propagation direction, which is not allowed for a transverse electromagnetic wave.

So, Option C is incorrect.


  1. Check option D

Given for propagation in +y+y+y direction:

E⃗=12Eyz(x,t)z^,B⃗=12Bz(x,t)y^\vec E = \frac{1}{\sqrt 2} E_{yz}(x,t)\hat z, \qquad \vec B = \frac{1}{\sqrt 2} B_z(x,t)\hat yE=2​1​Eyz​(x,t)z^,B=2​1​Bz​(x,t)y^​

For propagation along +y+y+y, B⃗\vec BB must also be perpendicular to y^\hat yy^​.

But here B⃗\vec BB is along y^\hat yy^​, parallel to the propagation direction, which is impossible.

Also, direction of propagation is along E⃗×B⃗\vec E \times \vec BE×B:

z^×y^=−x^\hat z \times \hat y = -\hat xz^×y^​=−x^

which is not +y^+\hat y+y^​.

So, Option D is incorrect.


  1. Final conclusion

Only Option A satisfies all conditions for an electromagnetic wave in vacuum.

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