Question:

The electric field associated with an electromagnetic wave propagating in a dielectric medium is given by Eβƒ—\vec{E}=30(2π‘₯Μ‚ + 𝑦̂)sin [2πœ‹ (5Γ—1014𝑑 βˆ’1073z\frac{10^7}{3}z)] Vmβˆ’1. Which of the following option(s) is(are) correct? [Given: The speed of light in vacuum, 𝑐 = 3 Γ— 108 msβˆ’1]

Updated On: May 19, 2024
  • 𝐡π‘₯ = βˆ’2 Γ— 10βˆ’7 sin [2πœ‹(5Γ—1014π‘‘βˆ’1073z\frac{10^7}{3}z)]Wbβˆ’2
  • 𝐡y=2Γ—10βˆ’7 sin[2πœ‹(5Γ—1014π‘‘βˆ’1073z\frac{10^7}{3}z)]Wbβˆ’2
  • The wave is polarized in the π‘₯𝑦-plane with a polarization angle 30Β° with respect to the π‘₯-axis.
  • The refractive index of the medium is 2
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The Correct Option is A, D

Approach Solution - 1

the speed of light in a medium is V=wk\frac{w}{k}
v=3Γ—5Γ—1014107v=\frac{3\times5\times10^{14}}{10^7}
v=1.5Γ—108v=1.5\times10^8
refractive index = ΞΌ\mu = CV=3Γ—1081.5Γ—108=2\frac{C}{V}=\frac{3\times10^8}{1.5\times10^8}=2
ΞΌ=2\mu=2
given, Eβƒ—=30(2x^+y^) sin(2Ο€(5Γ—1014βˆ’1073))1m\vec{E}=30(2\hat{x}+\hat{y})\,sin(2\pi(5\times10^{14}-\frac{10^7}{3}))^\frac{1}{m}
The electric field associated with an electromagnetic wave propagating in a dielectric medium
B0=E0V=3051.5Γ—108B_0=\frac{E_0}{V}=\frac{30\sqrt{5}}{1.5\times10^8}
Direction of B0βƒ—\vec{B_0} is (Vβƒ—Γ—Eβƒ—\vec{V}\times\vec{E})
V⃗×E⃗=k^×2i^+j^5\vec{V}\times\vec{E}=\hat{k}\times\frac{2\hat{i}+\hat{j}}{\sqrt5}
(βˆ’i^+2j^5)(\frac{-\hat{i}+2\hat{j}}{\sqrt5}) put value B0βƒ—\vec{B_0} = 3051.5Γ—108Γ—(βˆ’i^+2j^5)\frac{30\sqrt5}{1.5\times10^8}\times(\frac{-\hat{i}+2\hat{j}}{\sqrt5})
Bx=βˆ’2Γ—107B_x=-2\times10^7
 
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Approach Solution -2

 Explanation:
- The speed of light V V in a medium is given by Ο‰k \frac{\omega}{k} .
- Using the provided frequency and wave number, v=3Γ—5Γ—1014107 v = \frac{3 \times 5 \times 10^{14}}{10^7} .
- This calculates to v=1.5Γ—108 v = 1.5 \times 10^8 m/s.
- The refractive index ΞΌ \mu is calculated as CV=3Γ—1081.5Γ—108=2 \frac{C}{V} = \frac{3 \times 10^8}{1.5 \times 10^8} = 2 .
- Given the electric field Eβƒ—=30(2x^+y^)sin⁑[2Ο€(5Γ—1014tβˆ’z3Γ—107)] Vmβˆ’1 \vec{E} = 30(2\hat{x}+\hat{y})\sin\left[2\pi\left(5\times10^{14}t-\frac{z}{3\times10^7}\right)\right] \, \text{Vm}^{-1} .
- The magnetic field amplitude B0=E0V=3051.5Γ—108 B_0 = \frac{E_0}{V} = \frac{30\sqrt{5}}{1.5\times10^8} .
- The direction of B0⃗ \vec{B_0} is given by V⃗×E⃗ \vec{V} \times \vec{E} .
- Calculating Vβƒ—Γ—Eβƒ—=k^Γ—2i^+j^5=βˆ’i^+2j^5 \vec{V} \times \vec{E} = \hat{k} \times \frac{2\hat{i} + \hat{j}}{\sqrt{5}} = \frac{-\hat{i} + 2\hat{j}}{\sqrt{5}} .
- Therefore, B0βƒ—=3051.5Γ—108Γ—βˆ’i^+2j^5 \vec{B_0} = \frac{30\sqrt{5}}{1.5\times10^8} \times \frac{-\hat{i}+2\hat{j}}{\sqrt{5}} .
- Finally, Bx=βˆ’2Γ—10βˆ’7 B_x = -2 \times 10^{-7} .
Further:
- The speed of light V V in the medium is derived using V=Ο‰k V = \frac{\omega}{k} .
- Calculating with the given values, V=1.5Γ—108 m/s V = 1.5 \times 10^8 \, \text{m/s} .
- The refractive index ΞΌ \mu is found to be 2 using ΞΌ=CV \mu = \frac{C}{V} .
- Given the electric field expression, the magnetic field B0 B_0 and its direction are determined by V⃗×E⃗ \vec{V} \times \vec{E} .
- The correct options are A and D.

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The waves that are produced when an electric field comes into contact with a magnetic field are known as Electromagnetic Waves or EM waves. The constitution of an oscillating magnetic field and electric fields gives rise to electromagnetic waves.

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Electromagnetic waves can be grouped according to the direction of disturbance in them and according to the range of their frequency. Recall that a wave transfers energy from one point to another point in space. That means there are two things going on: the disturbance that defines a wave, and the propagation of wave. In this context the waves are grouped into the following two categories:

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  • Transverse waves: A wave is called a transverse wave when the disturbances in the wave are perpendicular (at right angles) to the direction of propagation of the wave.