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QJEEM24Ph5fbe: JEE Main 2024 Physics - Class 12 JEEM24Ph5fbe Solution: A plane EM wave is propagating along direction. It has a…

A plane EM wave is propagating along xx direction. It has a wavelength of 4 mm4 \mathrm{~mm} . If electric field is in yy direction with the maximum magnitude of 60 Vm−160 \mathrm{~Vm}^{-1} , the equation for magnetic field is :

Multiple Choice Options

  • A Bz=2×10−7sin⁡[π2(x−3×108t)]k^T\mathrm{B}_z=2 \times 10^{-7} \sin \left[\frac{\pi}{2}\left(x-3 \times 10^8 \mathrm{t}\right)\right] \hat{\mathrm{k}} \mathrm{T}
  • B Bz=2×10−7sin⁡[π2×103(x−3×108t)]k^T\mathrm{B}_z=2 \times 10^{-7} \sin \left[\frac{\pi}{2} \times 10^3\left(x-3 \times 10^8 \mathrm{t}\right)\right] \hat{\mathrm{k}} \mathrm{T}
  • C Bz=60sin⁡[π2(x−3×108t)]k^T\mathrm{B}_z=60 \sin \left[\frac{\pi}{2}\left(x-3 \times 10^8 \mathrm{t}\right)\right] \hat{\mathrm{k}} \mathrm{T}
  • D Bx=60sin⁡[π2(x−3×108t)]i^T\mathrm{B}_x=60 \sin \left[\frac{\pi}{2}\left(x-3 \times 10^8 \mathrm{t}\right)\right] \hat{\mathrm{i}} \mathrm{T}

Step-by-Step Verified Solution

To find the correct equation for the magnetic field of the plane electromagnetic wave given its parameters, we can use a couple of known relationships from electromagnetism.

Firstly, the wavelength ( λ\lambda ) of the wave is given as 4 mm=4×10−3 m4 \mathrm{~mm} = 4 \times 10^{-3} \mathrm{~m} . The speed of light (and all electromagnetic waves in vacuum) is c=3×108 m/sc = 3 \times 10^8 \mathrm{~m/s} . Using these values, we can find the frequency ( ff ) of the wave using the relationship:

c=λfc = \lambda f

f=cλ=3×1084×10−3=75×109 Hzf = \frac{c}{\lambda} = \frac{3 \times 10^8}{4 \times 10^{-3}} = 75 \times 10^9 \mathrm{~Hz}

The angular frequency ( ω\omega ) which appears in wave equations is related to the frequency by ω=2πf\omega = 2\pi f . However, in this context, what we need is the wave vector ( kk ), which defines how the phase of the wave changes with space. The wave vector k=2πλk = \frac{2\pi}{\lambda} . So, for this wave, k=2π4×10−3=π2×103 m−1k = \frac{2\pi}{4 \times 10^{-3}} = \frac{\pi}{2} \times 10^3 \, \mathrm{m}^{-1} .

Knowing that the electric field ( E\mathbf{E} ) and magnetic field ( B\mathbf{B} ) are related as E=cBE = cB in a vacuum, where EE and BB are the magnitudes of the electric and magnetic fields, respectively, we can calculate the magnitude of the magnetic field using the provided maximum electric field magnitude ( E=60 Vm−1E = 60 \, \mathrm{Vm}^{-1} ).

B=Ec=603×108=2×10−7 TB = \frac{E}{c} = \frac{60}{3 \times 10^8} = 2 \times 10^{-7} \mathrm{~T}

Therefore, the wave equation for the magnetic field, considering it propagates in the xx -direction and oscillates in a direction perpendicular to both the xx -direction and the direction of the electric field (thus, in the zz -direction if E\mathbf{E} is in the yy -direction), is:

B=Bsin⁡(kx−ωt)k^\mathbf{B} = B \sin(kx - \omega t) \hat{\mathbf{k}}

B=2×10−7sin⁡(π2×103(x−3×108t))k^T\mathbf{B} = 2 \times 10^{-7} \sin \left(\frac{\pi}{2} \times 10^3(x - 3 \times 10^8t)\right) \hat{\mathbf{k}} \mathrm{T}

This is represented by Option B:

Bz=2×10−7sin⁡[π2×103(x−3×108t)]k^T\mathrm{B}_z=2 \times 10^{-7} \sin \left[\frac{\pi}{2} \times 10^3\left(x-3 \times 10^8 \mathrm{t}\right)\right] \hat{\mathrm{k}} \mathrm{T}

Therefore, the correct answer is Option B.

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