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NEET • PHYSICS • ELECTROMAGNETIC WAVES

Electromagnetic waves practice · Easy

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1 Easy
Understanding +4 | -1
An electromagnetic wave is propagating along the +z+\mathrm{z}-axis. Direction of electric and the magnetic field of this wave can be represented by
View answer and explanation
Correct option: A
E⃗=E0i^,B⃗=B0j^\vec{E}=E_0 \hat{i}, \vec{B}=B_0 \hat{j}
Option A (E⃗=E0i^,B⃗=B0j^\vec{E}=E_0 \hat{i}, \vec{B}=B_0 \hat{j}) is correct because the electric and magnetic fields are perpendicular to each other and to the direction of propagation, which is the z-axis.
Solution approach
  1. Correct Answer + Core Reason: E⃗=E0i^,B⃗=B0j^\vec{E}=E_0 \hat{i}, \vec{B}=B_0 \hat{j}. E and B fields are perpendicular to each other and the direction of propagation.

    Step-by-Step Solution:

    Step 1: Recall the properties of electromagnetic waves.

    Step 2: In an electromagnetic wave, the electric field (E⃗\vec{E}), magnetic field (B⃗\vec{B}), and the direction of propagation (k⃗\vec{k}) are mutually perpendicular. Since the wave is propagating along the +z-axis, k⃗=k^\vec{k} = \hat{k}.

    Step 3: If E⃗\vec{E} is along the x-axis (i^\hat{i}), then B⃗\vec{B} must be along the y-axis (j^\hat{j}) to satisfy the condition E⃗×B⃗∝k⃗\vec{E} \times \vec{B} \propto \vec{k}.

    Step 4: Final Answer: E⃗=E0i^,B⃗=B0j^\vec{E}=E_0 \hat{i}, \vec{B}=B_0 \hat{j}

    Why other options are wrong:
    - Option B: E⃗=E0k^,B⃗=B0i^\vec{E}=E_0 \hat{k}, \vec{B}=B_0 \hat{i} is incorrect because the electric field is along the z-axis, which is the direction of propagation, violating the perpendicularity condition.
    - Option C: E⃗=E0j^,B⃗=B0i^\vec{E}=E_0 \hat{j}, \vec{B}=B_0 \hat{i} is incorrect because E⃗×B⃗\vec{E} \times \vec{B} would be in the -z direction, not the +z direction.
    - Option D: E⃗=E0j^,B⃗=B0k^\vec{E}=E_0 \hat{j}, \vec{B}=B_0 \hat{k} is incorrect because the magnetic field is along the z-axis, which is the direction of propagation, violating the perpendicularity condition.

    Key Concepts:
    - Electromagnetic waves
    - Direction of propagation
    - Perpendicularity of E, B, and k

    Memory Aids:
    - Remember that E, B, and the direction of propagation are mutually perpendicular.

    Quick Tips:
    - Use the right-hand rule to determine the direction of propagation: E⃗×B⃗\vec{E} \times \vec{B} gives the direction of propagation.
2 Easy
Application +4 | -1
Calculate the momentum transferred to a surface when a radiation of energy E falls normally on it. Assume that the reflectivity of the surface is unity.
View answer and explanation
Correct option: B
2Ec\frac{2 E}{c}
Option B (2Ec\frac{2 E}{c}) is correct because the momentum transferred to a surface with reflectivity of unity is twice the energy divided by the speed of light.
Solution approach
  1. Correct Answer + Core Reason: 2Ec\frac{2 E}{c}. Momentum transferred for total reflection is twice the energy divided by c.

    Step-by-Step Solution:

    Step 1: Recall the relationship between energy and momentum of radiation.

    Step 2: The momentum of radiation with energy E is given by p=Ecp = \frac{E}{c}.

    Step 3: For a surface with reflectivity of unity (total reflection), the momentum transferred is twice the initial momentum.

    Step 4: Therefore, the momentum transferred is 2p=2Ec2p = \frac{2E}{c}.

    Why other options are wrong:
    - Option A: Ec\frac{E}{c} is incorrect because it represents the momentum transferred for total absorption, not reflection.
    - Option C: EcE c is incorrect because it multiplies energy by the speed of light, which is not the correct relationship for momentum.
    - Option D: Ec2\frac{E}{c^2} is incorrect because it divides energy by the square of the speed of light, which is not the correct relationship for momentum.

    Key Concepts:
    - Momentum of radiation
    - Reflection of radiation

    Memory Aids:
    - Remember that reflection doubles the momentum transfer.

    Quick Tips:
    - For total reflection, the momentum transferred is 2E/c2E/c.
3 Easy
Application +4 | -1
Radiations of intensity 0.5 Wm−2W{m^{ - 2}}are striking a metal plate. The pressure on the plate is
View answer and explanation
Correct option: A
0.166×10−8  Nm−20.166 \times {10^{ - 8}}\;\mathrm{N}{\mathrm{m}^{ - 2}}
Option A (0.166×10−8  Nm−20.166 \times {10^{ - 8}}\;\mathrm{N}{\mathrm{m}^{ - 2}}) is correct because the pressure is calculated as intensity divided by the speed of light when the radiation is fully absorbed.
Solution approach
  1. Correct Answer + Core Reason: 0.166×10−8  Nm−20.166 \times {10^{ - 8}}\;\mathrm{N}{\mathrm{m}^{ - 2}}. The pressure is calculated by dividing the intensity by the speed of light.

    Step-by-Step Solution:

    Step 1: Identify the given information: Intensity, I=0.5  W/m2I = 0.5 \;W/m^2.

    Step 2: Recall the formula for radiation pressure when the radiation is fully absorbed: P=IcP = \frac{I}{c}, where PP is the pressure, II is the intensity, and cc is the speed of light.

    Step 3: Substitute the given values: P=0.5  W/m23×108  m/sP = \frac{0.5 \;W/m^2}{3 \times 10^8 \;m/s}

    Step 4: Calculate the pressure: P=0.166×10−8  N/m2P = 0.166 \times 10^{-8} \;N/m^2

    Step 5: Final Answer: P=0.166×10−8  Nm−2P = 0.166 \times {10^{ - 8}}\;\mathrm{N}{\mathrm{m}^{ - 2}}

    Why other options are wrong:
    - Option B: This value is incorrect. It might be obtained by multiplying the correct answer by 2, possibly confusing the case of full reflection with full absorption.
    - Option C: This value is incorrect. It might be obtained by using an incorrect formula or making a calculation error.
    - Option D: This value is incorrect. It might be obtained by dividing the intensity by a value other than the speed of light or making a calculation error.

    Key Concepts:
    - Radiation pressure
    - Intensity of electromagnetic waves
    - Speed of light

    Memory Aids:
    - Pressure = Intensity / Speed of Light (P = I/c) for full absorption

    Quick Tips:
    - Remember the formula for radiation pressure. Ensure you use the correct formula based on whether the radiation is absorbed or reflected.
4 Easy
Remembering +4 | -1
Part of electromagnetic spectrum that has largest penetrating power is
View answer and explanation
Correct option: A
γ\gamma-rays
Option A is correct because gamma rays have the largest penetrating power due to their high energy and short wavelength in the electromagnetic spectrum.
Solution approach
  1. Correct Answer + Core Reason: γ\gamma-rays. Gamma rays have the highest penetrating power due to their high energy.

    Step-by-Step Solution:

    Step 1: Recall the relationship between energy, frequency, and wavelength of electromagnetic radiation: E=hf=hcλE = hf = \frac{hc}{\lambda}, where E is energy, f is frequency, λ is wavelength, h is Planck's constant, and c is the speed of light.

    Step 2: Higher energy electromagnetic radiation has greater penetrating power.

    Step 3: Among the given options, gamma rays have the highest energy and shortest wavelength, therefore the largest penetrating power.

    Why other options are wrong:
    - Option B: X-rays. X-rays have less penetrating power than gamma rays.
    - Option C: radio-waves. Radio waves have much lower energy and penetrating power than gamma rays.
    - Option D: Infrared rays. Infrared rays have much lower energy and penetrating power than gamma rays.

    Key Concepts:
    - Electromagnetic Spectrum
    - Energy of Electromagnetic Radiation
    - Penetrating Power

    Memory Aids:
    - Remember that higher energy radiation has greater penetrating power.

    Quick Tips:
    - Know the relationship between energy, frequency, and wavelength.
5 Easy
Application +4 | -1
If frequency of electromagnetic wave is 60 MHz60 \mathrm{~MHz} and it travels in air along zz direction then the corresponding electric and magnetic field vectors will be mutually perpendicular to each other and the wavelength of the wave (in m\mathrm{m}) is
View answer and explanation
Correct option: D
5
Option D (5) is correct because the wavelength is calculated using the formula λ=c/f\lambda = c/f, where cc is the speed of light and ff is the frequency.
Solution approach
  1. Correct Answer + Core Reason: 5. The wavelength is calculated using λ=c/f\lambda = c/f.

    Step-by-Step Solution:

    Step 1: Formula: The wavelength of an electromagnetic wave is given by λ=cf\lambda = \frac{c}{f}, where cc is the speed of light in air (approximately 3×108 m/s3 \times 10^8 \text{ m/s}) and ff is the frequency.

    Step 2: Substitution: Given f=60 MHz=60×106 Hzf = 60 \text{ MHz} = 60 \times 10^6 \text{ Hz}, we have λ=3×10860×106\lambda = \frac{3 \times 10^8}{60 \times 10^6}.

    Step 3: Calculation: λ=30060=5 m\lambda = \frac{300}{60} = 5 \text{ m}.

    Step 4: Final Answer: 5

    Why other options are wrong:
    - Option A: This is incorrect. The correct calculation yields 5 m.
    - Option B: This is incorrect. The correct calculation yields 5 m.
    - Option C: This is incorrect. The correct calculation yields 5 m.

    Key Concepts:
    - Wavelength of electromagnetic waves
    - Frequency
    - Speed of light

    Memory Aids:
    - λ=c/f\lambda = c/f (Lambda equals c over f).

    Quick Tips:
    - Always convert frequency to Hz before calculating wavelength.
6 Easy
Application +4 | -1
nn photons of wavelength λ\lambda are absorbed by a black body of mass 'mm'. The momentum gained by the body is
View answer and explanation
Correct option: A
nhλ\frac{nh}{\lambda}
Option A (nhλ\frac{nh}{\lambda}) is correct because the momentum gained by the body is the sum of the momenta of the absorbed photons.
Solution approach
  1. Correct Answer + Core Reason: nhλ\frac{nh}{\lambda}. The momentum gained is the sum of the momenta of the absorbed photons.

    Step-by-Step Solution:

    Step 1: Recall the momentum of a photon.

    Step 2: The momentum of a single photon is given by p=hλp = \frac{h}{\lambda}, where h is Planck's constant and λ\lambda is the wavelength.

    Step 3: Calculate the total momentum gained by the black body.

    Step 4: Since n photons are absorbed, the total momentum gained is P=n×p=nhλP = n \times p = n \frac{h}{\lambda}.

    Why other options are wrong:
    - Option B: nhmλ\frac{nh}{m \lambda} is incorrect because it divides the momentum by the mass of the black body, which is not relevant to the momentum gained.
    - Option C: mnhλ\frac{mnh}{\lambda} is incorrect because it multiplies the momentum by the mass of the black body, which is not relevant to the momentum gained.
    - Option D: hmλ\frac{h}{m \lambda} is incorrect because it considers only one photon and divides by the mass of the black body, which is not relevant to the momentum gained.

    Key Concepts:
    - Momentum of a photon
    - Absorption of photons

    Memory Aids:
    - Remember that the momentum of a photon is inversely proportional to its wavelength.

    Quick Tips:
    - The total momentum gained is the sum of individual photon momenta.
7 Easy
Understanding +4 | -1
During the porpagation of electromagnetic waves in a medium,
View answer and explanation
Correct option: C
electric energy density is equal to the magnetic energy density
Option C (electric energy density is equal to the magnetic energy density) is correct because in an electromagnetic wave, the electric and magnetic energy densities are equal on average.
Solution approach
  1. Correct Answer + Core Reason: electric energy density is equal to the magnetic energy density. In an EM wave, energy is equally distributed between electric and magnetic fields.

    Step-by-Step Solution:

    Step 1: Recall the energy densities of electric and magnetic fields.

    Step 2: The energy density of the electric field is given by uE=12ε0E2u_E = \frac{1}{2} \varepsilon_0 E^2, and the energy density of the magnetic field is given by uB=12B2μ0u_B = \frac{1}{2} \frac{B^2}{\mu_0}.

    Step 3: In an electromagnetic wave, E=cBE = cB, and c=1ε0μ0c = \frac{1}{\sqrt{\varepsilon_0 \mu_0}}. Substituting these relationships, we find that uE=uBu_E = u_B.

    Step 4: Final Answer: uE=uBu_E = u_B

    Why other options are wrong:
    - Option A: electric energy density is double of the magnetic energy density is incorrect because the energy densities are equal, not doubled.
    - Option B: electric energy density is half of the magnetic energy density is incorrect because the energy densities are equal, not halved.
    - Option D: Both electric and magnetic energy densities are zero is incorrect because electromagnetic waves carry energy, so the energy densities are non-zero.

    Key Concepts:
    - Electromagnetic waves
    - Electric and magnetic energy densities

    Memory Aids:
    - Remember that energy is equally distributed in EM waves.

    Quick Tips:
    - In EM waves, the electric and magnetic fields contribute equally to the energy density.
8 Easy
Application +4 | -1
In an electromagnetic wave, at any instant the electric field was found to oscillate with an amplitude of 18 v/m18\, \mathrm{v} / \mathrm{m}. The magnitude of oscillating magnetic field will be -
View answer and explanation
Correct option: B
6×10−8 T6 \times 10^{-8} \mathrm{~T}
Option B (6×10−8 T6 \times 10^{-8} \mathrm{~T}) is correct because the magnitude of the oscillating magnetic field is calculated using the formula B0=E0cB_0 = \frac{E_0}{c}, where c is the speed of light.
Solution approach
  1. Correct Answer + Core Reason: 6×10−8 T6 \times 10^{-8} \mathrm{~T}. The magnitude of the oscillating magnetic field is calculated using the formula B0=E0cB_0 = \frac{E_0}{c}.

    Step-by-Step Solution:

    Step 1: Identify the given value: Amplitude of the electric field E0=18 V/mE_0 = 18 \text{ V/m}.

    Step 2: Recall the relationship between the amplitudes of the electric and magnetic fields in an electromagnetic wave: E0=cB0E_0 = cB_0, where cc is the speed of light in vacuum (c=3×108 m/sc = 3 \times 10^8 \text{ m/s}).

    Step 3: Solve for the amplitude of the magnetic field: B0=E0c=18 V/m3×108 m/sB_0 = \frac{E_0}{c} = \frac{18 \text{ V/m}}{3 \times 10^8 \text{ m/s}}.

    Step 4: Calculate the amplitude of the magnetic field: B0=6×10−8 TB_0 = 6 \times 10^{-8} \text{ T}.

    Why other options are wrong:
    - Option A: 4×10−6 T4 \times 10^{-6} \mathrm{~T} is incorrect because it does not follow from the correct calculation.
    - Option C: 9×10−9 T9 \times 10^{-9} \mathrm{~T} is incorrect because it does not follow from the correct calculation.
    - Option D: 11×10−11 T11 \times 10^{-11} \mathrm{~T} is incorrect because it does not follow from the correct calculation.

    Key Concepts:
    - Electromagnetic waves
    - Relationship between electric and magnetic field amplitudes
    - Speed of light

    Memory Aids:
    - Remember the relationship E0=cB0E_0 = cB_0.

    Quick Tips:
    - Always remember the relationship between E and B fields in EM waves: E = cB.
9 Easy
Application +4 | -1
The sun delivers 103 W/m2{10^3}\,W/{m^2} of electromagnetic flux to the earth’s surface. Find the total power that is incident on a roof of dimensions 8 m×20 m8\,m \times 20\,m and the radiation force on the roof is given by 5.33×10−4N5.33 \times {10^{ - 4}}N
View answer and explanation
Correct option: C
1.6×105watt1.6 \times {10^5}\mathrm{ watt}
Option C (1.6×105watt1.6 \times {10^5}\mathrm{ watt}) is correct because the total power is the product of the intensity and the area of the roof.
Solution approach
  1. Correct Answer + Core Reason: 1.6×105watt1.6 \times {10^5}\mathrm{ watt}. Total power is intensity times area.

    Step-by-Step Solution:

    Step 1: Calculate the area of the roof.

    Step 2: Area = length x width = 8 m x 20 m = 160 m2^2.

    Step 3: Calculate the total power incident on the roof.

    Step 4: Power = Intensity x Area = 103^3 W/m2^2 x 160 m2^2 = 1.6 x 105^5 W.

    Why other options are wrong:
    - Option A: 20 watt is incorrect. This value is much smaller than the actual power.
    - Option B: 40 watt is incorrect. This value is much smaller than the actual power.
    - Option D: Zero is incorrect because the sun delivers electromagnetic flux to the earth's surface, hence there is power incident on the roof.

    Key Concepts:
    - Intensity of electromagnetic waves
    - Power calculation

    Memory Aids:
    - Remember that Power = Intensity x Area.

    Quick Tips:
    - Always ensure consistent units when calculating power.
10 Easy
Application +4 | -1
If equation of wave is given by y=0.05sin⁡(2x−4t)y=0.05 \sin (2 x-4 t). Find velocity of wave?
View answer and explanation
Correct option: A
2
Option A (2) is correct because the velocity of the wave is the coefficient of t divided by the coefficient of x.
Solution approach
  1. Correct Answer + Core Reason: 2. The velocity of the wave is calculated as the ratio of the coefficient of t to the coefficient of x.

    Step-by-Step Solution:

    Step 1: Recall the general form of a wave equation: y=Asin⁡(kx−ωt)y = A \sin(kx - \omega t), where A is the amplitude, k is the wave number, and ω\omega is the angular frequency.

    Step 2: Given the wave equation y=0.05sin⁡(2x−4t)y = 0.05 \sin(2x - 4t).

    Step 3: Identify the values of k and ω\omega: k=2k = 2 and ω=4\omega = 4.

    Step 4: Calculate the velocity of the wave (v) using the formula v=ωkv = \frac{\omega}{k}.

    Step 5: Substitute the values of ω\omega and k into the equation: v=42=2v = \frac{4}{2} = 2.

    Why other options are wrong:
    - Option B: 0 is incorrect because it is not the correct calculation of the velocity of the wave.
    - Option C: 0 is incorrect because it is not the correct calculation of the velocity of the wave.
    - Option D: 0 is incorrect because it is not the correct calculation of the velocity of the wave.

    Key Concepts:
    - Wave equation
    - Wave number
    - Angular frequency
    - Velocity of wave

    Memory Aids:
    - Remember the relationship v=ωkv = \frac{\omega}{k}.

    Quick Tips:
    - Understand the general form of a wave equation and how to extract the values of k and ω\omega.
11 Easy
Understanding +4 | -1
A plane electromagnetic wave propagating along z-direction can be generated by
View answer and explanation
Correct option: A
Ex,ByE_x, B_y
Option A (Ex,ByE_x, B_y) is correct because in an electromagnetic wave propagating along the z-direction, the electric field and magnetic field are perpendicular to each other and to the direction of propagation.
Solution approach
  1. Correct Answer + Core Reason: Ex,ByE_x, B_y. The electric and magnetic fields must be perpendicular to each other and the direction of propagation.

    Step-by-Step Solution:

    Step 1: Recall that electromagnetic waves are transverse waves, meaning that the electric field (E) and magnetic field (B) are perpendicular to each other and to the direction of propagation.

    Step 2: Given that the wave is propagating along the z-direction, the electric and magnetic fields must be in the x-y plane.

    Step 3: Therefore, if the electric field is in the x-direction (ExE_x), the magnetic field must be in the y-direction (ByB_y), and vice versa.

    Why other options are wrong:
    - Option B: Ex,BxE_x, B_x is incorrect because the electric and magnetic fields must be perpendicular to each other.
    - Option C: Ex,BzE_x, B_z is incorrect because the magnetic field must be perpendicular to the direction of propagation (z-direction).
    - Option D: Ey,BzE_y, B_z is incorrect because the magnetic field must be perpendicular to the direction of propagation (z-direction).

    Key Concepts:
    - Electromagnetic waves
    - Transverse waves
    - Direction of propagation

    Memory Aids:
    - Remember that the electric field, magnetic field, and direction of propagation are mutually perpendicular.

    Quick Tips:
    - Use the right-hand rule to determine the direction of the electric and magnetic fields.
12 Easy
Application +4 | -1
A plane electromagnetic wave of frequency 35MHz35 {MHz} travels in free space along the XX-direction. At a particular point (in space and time) E⃗=9.6j^ V/m\vec{E}=9.6 \hat{j} {~V} / {m}. The value of magnetic field at this point is :
View answer and explanation
Correct option: D
3.2×10−8k^ T3.2 \times 10^{-8} \hat{k}\, T
Option D (3.2×10−8k^ T3.2 \times 10^{-8} \hat{k}\, T) is correct because the magnetic field is calculated using B=EcB = \frac{E}{c} and the direction is determined by the right-hand rule, resulting in the k direction.
Solution approach
  1. Correct Answer + Core Reason: 3.2×10−8k^ T3.2 \times 10^{-8} \hat{k}\, T. The magnetic field is calculated using B=EcB = \frac{E}{c} and the direction is determined by the right-hand rule.

    Step-by-Step Solution:

    Step 1: Identify the given values: Frequency f=35 MHz=35×106 Hzf = 35 \text{ MHz} = 35 \times 10^6 \text{ Hz} and electric field E⃗=9.6j^ V/m\vec{E} = 9.6 \hat{j} \text{ V/m}. The wave travels along the X-direction.

    Step 2: Recall the relationship between the amplitudes of the electric and magnetic fields in an electromagnetic wave: E=cBE = cB, where cc is the speed of light in vacuum (c=3×108 m/sc = 3 \times 10^8 \text{ m/s}).

    Step 3: Solve for the magnitude of the magnetic field: B=Ec=9.6 V/m3×108 m/s=3.2×10−8 TB = \frac{E}{c} = \frac{9.6 \text{ V/m}}{3 \times 10^8 \text{ m/s}} = 3.2 \times 10^{-8} \text{ T}.

    Step 4: Determine the direction of the magnetic field. Since the wave travels along the X-direction and the electric field is along the Y-direction (j^\hat{j}), the magnetic field must be along the Z-direction (k^\hat{k}) to satisfy the condition that the direction of propagation is given by E⃗×B⃗\vec{E} \times \vec{B}.

    Step 5: Therefore, the magnetic field is B⃗=3.2×10−8k^ T\vec{B} = 3.2 \times 10^{-8} \hat{k} \text{ T}.

    Why other options are wrong:
    - Option A: 9.6j^T9.6 \hat{j} T is incorrect because it has the wrong magnitude and direction.
    - Option B: 9.6×10−8k^ T9.6 \times 10^{-8} \hat{k}\, T is incorrect because it has the wrong magnitude.
    - Option C: 3.2×10−8i^ T3.2 \times 10^{-8} \hat{i} {~T} is incorrect because it has the wrong direction.

    Key Concepts:
    - Electromagnetic waves
    - Relationship between electric and magnetic field amplitudes
    - Speed of light
    - Direction of propagation

    Memory Aids:
    - Remember the relationship E=cBE = cB and the right-hand rule for the direction of propagation.

    Quick Tips:
    - Always remember to consider the direction of the fields in addition to their magnitudes.
13 Easy
Understanding +4 | -1
A plane electromagnetic wave propagating along z-direction can be generated by
View answer and explanation
Correct option: B
Ey,BxE_y, B_x
Option B, Ey,BxE_y, B_x, is correct because for a wave propagating along the z-direction, the electric and magnetic fields must be perpendicular to each other and to the direction of propagation.
Solution approach
  1. Correct Answer + Core Reason: Ey,BxE_y, B_x. For a wave propagating in the z-direction, the electric and magnetic fields must be perpendicular to each other and to the direction of propagation.

    Step-by-Step Solution:

    Step 1: Recall the properties of electromagnetic waves.

    Step 2: Electromagnetic waves are transverse waves, meaning that the electric field (E→\overrightarrow E) and the magnetic field (B→\overrightarrow B) are perpendicular to each other and to the direction of propagation (k→\overrightarrow k).

    Step 3: If the wave is propagating along the z-direction, then k→\overrightarrow k is along the z-axis. Therefore, E→\overrightarrow E and B→\overrightarrow B must be in the x-y plane. If E→\overrightarrow E is along the y-axis (EyE_y), then B→\overrightarrow B must be along the x-axis (BxB_x) to satisfy the condition that E→\overrightarrow E, B→\overrightarrow B, and k→\overrightarrow k are mutually perpendicular and E→×B→\overrightarrow E \times \overrightarrow B is in the direction of k→\overrightarrow k.

    Why other options are wrong:
    - Option A: Ey,ByE_y, B_y is incorrect because the electric and magnetic fields are parallel to each other, which is not possible for an electromagnetic wave.
    - Option C: Ex,BzE_x, B_z is incorrect because the magnetic field is along the direction of propagation, which is not possible for an electromagnetic wave.
    - Option D: Ey,BzE_y, B_z is incorrect because the magnetic field is along the direction of propagation, which is not possible for an electromagnetic wave.

    Key Concepts:
    - Properties of electromagnetic waves
    - Transverse waves
    - Direction of propagation

    Memory Aids:
    - Remember that the electric and magnetic fields are perpendicular to each other and to the direction of propagation.

    Quick Tips:
    - Always remember the properties of electromagnetic waves.
14 Easy
Remembering +4 | -1
Part of electromagnetic spectrum that corresponds to wavelength of 10−1010^{-10} m is
View answer and explanation
Correct option: D
X-rays
Option D is correct because X-rays correspond to a wavelength of approximately 10-10 m in the electromagnetic spectrum.
Solution approach
  1. Correct Answer + Core Reason: X-rays. X-rays have wavelengths around 10−1010^{-10} m.

    Step-by-Step Solution:

    Step 1: Recall the approximate wavelengths of different parts of the electromagnetic spectrum:
    - Radio waves: > 1 m
    - Microwaves: 10−310^{-3} m to 1 m
    - Infrared: 10−610^{-6} m to 10−310^{-3} m
    - Visible light: 4×10−74 \times 10^{-7} m to 7×10−77 \times 10^{-7} m
    - Ultraviolet: 10−810^{-8} m to 4×10−74 \times 10^{-7} m
    - X-rays: 10−810^{-8} m to 10−1210^{-12} m
    - Gamma rays: < 10−1210^{-12} m

    Step 2: Compare the given wavelength (10−1010^{-10} m) with the approximate wavelengths of the options.

    Step 3: 10−1010^{-10} m falls within the range of X-rays.

    Why other options are wrong:
    - Option A: Microwaves. Microwaves have much longer wavelengths than 10−1010^{-10} m.
    - Option B: Ultraviolet rays. Ultraviolet rays have longer wavelengths than 10−1010^{-10} m.
    - Option C: Infrared rays. Infrared rays have much longer wavelengths than 10−1010^{-10} m.

    Key Concepts:
    - Electromagnetic Spectrum
    - Wavelength

    Memory Aids:
    - Remember the approximate wavelengths of different parts of the electromagnetic spectrum.

    Quick Tips:
    - Know the typical wavelengths for different types of electromagnetic radiation.
15 Easy
Application +4 | -1
In a plane EM wave, the electric field oscillates sinusoidally at a frequency of 5×1010 Hz5 \times 10^{10} \mathrm{~Hz} and an amplitude of 50Vm−150 \mathrm{Vm}^{-1}. The total average energy density of the electromagnetic field of the wave is : [Use ε0=8.85×10−12C2/Nm2\varepsilon_0=8.85 \times 10^{-12} \mathrm{C}^2 / \mathrm{Nm}^2 ]
View answer and explanation
Correct option: C
1.106×10−8Jm−31.106 \times 10^{-8} \mathrm{Jm}^{-3}
Option C (1.106×10−8Jm−31.106 \times 10^{-8} \mathrm{Jm}^{-3}) is correct because it is the total average energy density calculated using the formula u=ε0E02/2u = \varepsilon_0 E_0^2 / 2.
Solution approach
  1. Correct Answer + Core Reason: 1.106×10−8Jm−31.106 \times 10^{-8} \mathrm{Jm}^{-3}. The total average energy density is calculated using the electric field amplitude and permittivity of free space.

    Step-by-Step Solution:

    Step 1: Identify the given information:\nFrequency, f=5×1010Hzf = 5 \times 10^{10} \mathrm{Hz}\nAmplitude of electric field, E0=50Vm−1E_0 = 50 \mathrm{Vm}^{-1}\nPermittivity of free space, ε0=8.85×10−12C2/Nm2\varepsilon_0 = 8.85 \times 10^{-12} \mathrm{C}^2 / \mathrm{Nm}^2

    Step 2: Recall the formula for the total average energy density of an electromagnetic wave:
    u=12ε0E02u = \frac{1}{2} \varepsilon_0 E_0^2

    Step 3: Substitute the given values into the formula:
    u=12×(8.85×10−12C2/Nm2)×(50Vm−1)2u = \frac{1}{2} \times (8.85 \times 10^{-12} \mathrm{C}^2 / \mathrm{Nm}^2) \times (50 \mathrm{Vm}^{-1})^2

    Step 4: Calculate the energy density:
    u=12×8.85×10−12×2500Jm−3u = \frac{1}{2} \times 8.85 \times 10^{-12} \times 2500 \mathrm{Jm}^{-3}
    u=4.425×10−12×2500Jm−3u = 4.425 \times 10^{-12} \times 2500 \mathrm{Jm}^{-3}
    u=11.0625×10−9Jm−3u = 11.0625 \times 10^{-9} \mathrm{Jm}^{-3}
    u=1.10625×10−8Jm−3u = 1.10625 \times 10^{-8} \mathrm{Jm}^{-3}

    Step 5: Round to three significant figures:
    u≈1.106×10−8Jm−3u \approx 1.106 \times 10^{-8} \mathrm{Jm}^{-3}

    Final Answer: 1.106×10−8Jm−31.106 \times 10^{-8} \mathrm{Jm}^{-3}

    Why other options are wrong:
    - Option A: 4.425×10−8Jm−34.425 \times 10^{-8} \mathrm{Jm}^{-3}: This is incorrect because it seems to have missed the factor of 1/2 in the energy density formula.
    - Option B: 2.212×10−8Jm−32.212 \times 10^{-8} \mathrm{Jm}^{-3}: This is incorrect, likely from a calculation error or using the wrong formula.
    - Option D: 2.212×10−10Jm−32.212 \times 10^{-10} \mathrm{Jm}^{-3}: This is incorrect because it seems to have used the wrong power of 10, possibly due to a unit conversion error.

    Key Concepts:
    - Electromagnetic waves
    - Energy density of electromagnetic waves
    - Permittivity of free space

    Memory Aids:
    - Remember the formula for energy density: u=12ε0E02u = \frac{1}{2} \varepsilon_0 E_0^2

    Quick Tips:
    - Ensure correct units are used in the calculation.
    - Double-check the formula before substituting values.
16 Easy
Application +4 | -1
In an electromagnetic wave the amplitude of magnetic field is 3×10−8 T3 \times 10^{-8} \mathrm{~T}. If the frequency of wave is 1012 Hz10^{12} \mathrm{~Hz}, then find the amplitude of associated electric field in S.I. unit.
View answer and explanation
Correct option: A
9
Option A (9) is correct because the amplitude of the electric field is calculated using the relation E0=cB0E_0 = cB_0, where c is the speed of light.
Solution approach
  1. Correct Answer + Core Reason: 9. The amplitude of the electric field is calculated using the relation E0=cB0E_0 = cB_0.

    Step-by-Step Solution:

    Step 1: Identify the given values: Amplitude of magnetic field B0=3×10−8 TB_0 = 3 \times 10^{-8} \text{ T}, and frequency f=1012 Hzf = 10^{12} \text{ Hz}.

    Step 2: Recall the relationship between the amplitudes of the electric and magnetic fields in an electromagnetic wave: E0=cB0E_0 = cB_0, where cc is the speed of light in vacuum (c=3×108 m/sc = 3 \times 10^8 \text{ m/s}).

    Step 3: Substitute the given values into the equation: E0=(3×108 m/s)×(3×10−8 T)E_0 = (3 \times 10^8 \text{ m/s}) \times (3 \times 10^{-8} \text{ T}).

    Step 4: Calculate the amplitude of the electric field: E0=9 V/mE_0 = 9 \text{ V/m}.

    Why other options are wrong:
    - Option B: 0 is incorrect because it does not follow from the correct calculation.
    - Option C: 0 is incorrect because it does not follow from the correct calculation.
    - Option D: 0 is incorrect because it does not follow from the correct calculation.

    Key Concepts:
    - Electromagnetic waves
    - Relationship between electric and magnetic field amplitudes
    - Speed of light

    Memory Aids:
    - Remember the relationship E0=cB0E_0 = cB_0.

    Quick Tips:
    - Always remember the relationship between E and B fields in EM waves: E = cB.
17 Easy
Understanding +4 | -1
Given below are two statements:
Statement I: Electromagnetic waves carry energy
as they travel through space and this energy is
equally shared by the electric and magnetic fields
Statement II: When electromagnetic waves strike
a surface, a pressure is exerted on the surface
In the light of the above statements, choose the
most appropriate answer from the options given
below
View answer and explanation
Correct option: A
Both Statement I and Statement II are correct
Option A (Both Statement I and Statement II are correct) is correct because electromagnetic waves carry energy and exert pressure when they strike a surface.
Solution approach
  1. Correct Answer + Core Reason: Both Statement I and Statement II are correct. Electromagnetic waves carry energy and exert pressure.

    Step-by-Step Solution:

    Step 1: Statement I: Electromagnetic waves carry energy. This is a fundamental property of electromagnetic waves. The energy is indeed shared by the electric and magnetic fields.

    Step 2: Statement II: Electromagnetic waves exert pressure. This is also true. When electromagnetic waves strike a surface, they transfer momentum, resulting in radiation pressure.

    Step 3: Final Answer: Both statements are correct.

    Why other options are wrong:
    - Option B: This is incorrect because Statement II is also correct.
    - Option C: This is incorrect because Statement I is also correct.
    - Option D: This is incorrect because both statements are correct.

    Key Concepts:
    - Energy of electromagnetic waves
    - Radiation pressure

    Memory Aids:
    - Electromagnetic waves are like tiny bullets carrying energy and momentum.

    Quick Tips:
    - Remember that electromagnetic waves can transfer both energy and momentum.
18 Easy
Application +4 | -1
An electromagnetic wave has electric field given by E⃗=(9.6j^)sin⁡[2π{30×106t−110x}],x\vec{E}=(9.6 \hat{j}) \sin \left[2 \pi\left\{30 \times 10^6 t-\frac{1}{10} x\right\}\right], x and tt are in SI units. The maximum magnetic field is
View answer and explanation
Correct option: A
3.2×10−93.2 \times 10^{-9}
Option A (3.2×10−93.2 \times 10^{-9}) is correct because the maximum magnetic field is calculated using the relation B0=E0cB_0 = \frac{E_0}{c}, where c is the speed of light.
Solution approach
  1. Correct Answer + Core Reason: 3.2×10−93.2 \times 10^{-9}. The maximum magnetic field is calculated using the relation B0=E0cB_0 = \frac{E_0}{c}.

    Step-by-Step Solution:

    Step 1: Identify the given value: Amplitude of the electric field E0=9.6 V/mE_0 = 9.6 \text{ V/m}.

    Step 2: Recall the relationship between the amplitudes of the electric and magnetic fields in an electromagnetic wave: E0=cB0E_0 = cB_0, where cc is the speed of light in vacuum (c=3×108 m/sc = 3 \times 10^8 \text{ m/s}).

    Step 3: Solve for the amplitude of the magnetic field: B0=E0c=9.6 V/m3×108 m/sB_0 = \frac{E_0}{c} = \frac{9.6 \text{ V/m}}{3 \times 10^8 \text{ m/s}}.

    Step 4: Calculate the amplitude of the magnetic field: B0=3.2×10−8 TB_0 = 3.2 \times 10^{-8} \text{ T}.

    Why other options are wrong:
    - Option B: 9.6×10−89.6 \times 10^{-8} is incorrect because it does not follow from the correct calculation.
    - Option C: 1.7×10−91.7 \times 10^{-9} is incorrect because it does not follow from the correct calculation.
    - Option D: 10−710^{-7} is incorrect because it does not follow from the correct calculation.

    Key Concepts:
    - Electromagnetic waves
    - Relationship between electric and magnetic field amplitudes
    - Speed of light

    Memory Aids:
    - Remember the relationship E0=cB0E_0 = cB_0.

    Quick Tips:
    - Always remember the relationship between E and B fields in EM waves: E = cB.
19 Easy
Application +4 | -1
In a place e.m. wave, the electric field oscillates sinusoidally at a frequency of 2.5×1010 Hz2.5 \times 10^{10} {~Hz} and amplitude 480 V/m480 {~V} / {m}. The amplitude of oscillating magnetic field will be :-
View answer and explanation
Correct option: C
1.6×10−6 Wb/m21.6 \times 10^{-6} {~Wb} / {m}^2
Option C (1.6×10−6 Wb/m21.6 \times 10^{-6} {~Wb} / {m}^2) is correct because the amplitude of the oscillating magnetic field is calculated using the formula B0=E0cB_0 = \frac{E_0}{c}, where c is the speed of light.
Solution approach
  1. Correct Answer + Core Reason: 1.6×10−6 Wb/m21.6 \times 10^{-6} {~Wb} / {m}^2. The amplitude of the oscillating magnetic field is calculated using the formula B0=E0cB_0 = \frac{E_0}{c}.

    Step-by-Step Solution:

    Step 1: Identify the given values: Frequency f=2.5×1010 Hzf = 2.5 \times 10^{10} \text{ Hz} and amplitude of the electric field E0=480 V/mE_0 = 480 \text{ V/m}.

    Step 2: Recall the relationship between the amplitudes of the electric and magnetic fields in an electromagnetic wave: E0=cB0E_0 = cB_0, where cc is the speed of light in vacuum (c=3×108 m/sc = 3 \times 10^8 \text{ m/s}).

    Step 3: Solve for the amplitude of the magnetic field: B0=E0c=480 V/m3×108 m/sB_0 = \frac{E_0}{c} = \frac{480 \text{ V/m}}{3 \times 10^8 \text{ m/s}}.

    Step 4: Calculate the amplitude of the magnetic field: B0=1.6×10−6 T=1.6×10−6 Wb/m2B_0 = 1.6 \times 10^{-6} \text{ T} = 1.6 \times 10^{-6} \text{ Wb/m}^2.

    Why other options are wrong:
    - Option A: 1.52×10−8 Wb/m21.52 \times 10^{-8} {~Wb} / {m}^2 is incorrect because it does not follow from the correct calculation.
    - Option B: 1.52×10−7 Wb/m21.52 \times 10^{-7} {~Wb} / {m}^2 is incorrect because it does not follow from the correct calculation.
    - Option D: 1.6×10−7 Wb/m21.6 \times 10^{-7} {~Wb} / {m}^2 is incorrect because it does not follow from the correct calculation.

    Key Concepts:
    - Electromagnetic waves
    - Relationship between electric and magnetic field amplitudes
    - Speed of light

    Memory Aids:
    - Remember the relationship E0=cB0E_0 = cB_0.

    Quick Tips:
    - Always remember the relationship between E and B fields in EM waves: E = cB.
20 Easy
Remembering +4 | -1
Rays in electromagnetic spectrum that has shortest wavelength are
View answer and explanation
Correct option: D
X-rays
Option D is correct because X-rays have the shortest wavelength among the given options in the electromagnetic spectrum.
Solution approach
  1. Correct Answer + Core Reason: X-rays. X-rays have the shortest wavelength among the given options.

    Step-by-Step Solution:

    Step 1: Recall the order of the electromagnetic spectrum from longest to shortest wavelength: Radio waves, Microwaves, Infrared, Visible light, Ultraviolet, X-rays, Gamma rays.

    Step 2: Compare the wavelengths of the given options:
    - Microwaves have longer wavelengths than infrared, visible light, ultraviolet, X-rays, and gamma rays.
    - Ultraviolet rays have shorter wavelengths than microwaves, infrared, and visible light, but longer than X-rays and gamma rays.
    - Infrared rays have longer wavelengths than visible light, ultraviolet, X-rays, and gamma rays.
    - X-rays have shorter wavelengths than microwaves, infrared, visible light, and ultraviolet rays, but longer than gamma rays.

    Step 3: From the given options, X-rays have the shortest wavelength.

    Why other options are wrong:
    - Option A: Microwaves. Microwaves have longer wavelengths than X-rays.
    - Option B: Ultraviolet rays. Ultraviolet rays have longer wavelengths than X-rays.
    - Option C: Infrared rays. Infrared rays have longer wavelengths than X-rays.

    Key Concepts:
    - Electromagnetic Spectrum
    - Wavelength

    Memory Aids:
    - Remember the order of the electromagnetic spectrum.

    Quick Tips:
    - Know the relative positions of different types of electromagnetic radiation in the spectrum.
21 Easy
Remembering +4 | -1
Displacement Current is:
View answer and explanation
Correct option: D
Due to time Varying Electric field
Option D is correct because displacement current arises from a time-varying electric field, as described by Maxwell's equations.
Solution approach
  1. Correct Answer + Core Reason: Due to time Varying Electric field. Displacement current is caused by a changing electric field.

    Step-by-Step Solution:

    Step 1: Recall Maxwell's modification to Ampere's Law: Maxwell added the displacement current term to Ampere's Law to account for changing electric fields. The displacement current is given by ID=ϵ0dΦEdt=ϵ0d(EA)dt=ϵ0AdEdtI_D = \epsilon_0 \frac{d\Phi_E}{dt} = \epsilon_0 \frac{d(EA)}{dt} = \epsilon_0 A \frac{dE}{dt}, where ΦE\Phi_E is the electric flux.

    Step 2: Analyze the options: The displacement current is directly proportional to the rate of change of the electric field.

    Why other options are wrong:
    - Option A: Flow of free electrons constitutes conduction current, not displacement current.
    - Option B: Flow of positive ions constitutes conduction current, not displacement current.
    - Option C: Flow of both positive and negative ions constitutes conduction current, not displacement current.

    Key Concepts:
    - Displacement current
    - Maxwell's equations
    - Time-varying electric fields

    Memory Aids:
    - Remember that displacement current is related to the *change* in electric field.

    Quick Tips:
    - Displacement current exists even in the absence of free charges.
22 Easy
Remembering +4 | -1
The S.I. unit of displacement current is:
View answer and explanation
Correct option: C
Ampere
Option C (Ampere) is correct because displacement current, like regular current, is measured in Amperes.
Solution approach
  1. Correct Answer + Core Reason: Ampere. Displacement current is a current, so it has the same unit as current.

    Step-by-Step Solution:

    Step 1: Recall the definition of displacement current: ID=ϵ0dΦEdtI_D = \epsilon_0 \frac{d\Phi_E}{dt}.

    Step 2: Analyze the units: The units of displacement current are the same as the units of regular current, which is Ampere.

    Why other options are wrong:
    - Option A: Henry is the unit of inductance.
    - Option B: Coulomb is the unit of electric charge.
    - Option D: Faraday is a (non-SI) unit of electric charge, and also a unit of capacitance.

    Key Concepts:
    - Displacement current
    - Units of current

    Memory Aids:
    - Displacement current is a *current*, so its unit must be Ampere.

    Quick Tips:
    - Always remember the units of physical quantities.
23 Easy
Understanding +4 | -1
Let the velocities of light in vacuum and glass are represented by vv and vgv_{\mathrm{g}}. When electrons move through glass with a velocity vev_e, there emitted a visible radiation in glass if
View answer and explanation
Correct option: A
ve>vgv_e > v_g
Option A (ve>vgv_e > v_g) is correct because Cherenkov radiation is emitted when a charged particle moves through a dielectric medium faster than the speed of light in that medium.
Solution approach
  1. Correct Answer + Core Reason: ve>vgv_e > v_g. Cherenkov radiation is emitted when a charged particle moves faster than the speed of light in that medium.

    Step-by-Step Solution:

    Step 1: Understand Cherenkov Radiation: This phenomenon occurs when a charged particle travels through a dielectric medium at a speed greater than the phase velocity of light in that medium.

    Step 2: Define variables: vev_e is the velocity of the electron in the glass, and vgv_g is the velocity of light in the glass.

    Step 3: Condition for Cherenkov Radiation: For visible radiation to be emitted, the electron's velocity must be greater than the speed of light in the glass: ve>vgv_e > v_g.

    Step 4: Final Answer: ve>vgv_e > v_g

    Why other options are wrong:
    - Option B: This is incorrect because if ve<vgv_e < v_g, the electron is moving slower than light in the glass, and Cherenkov radiation will not occur.
    - Option C: This is incorrect because the speed of light in vacuum (vv) is always greater than the speed of light in a medium (vgv_g). The condition depends on the speed of light in the glass, not in vacuum.
    - Option D: This is incorrect because it introduces an unnecessary ratio of speeds and doesn't represent the condition for Cherenkov radiation.

    Key Concepts:
    - Cherenkov Radiation
    - Speed of light in a medium

    Memory Aids:
    - Remember that Cherenkov radiation is the optical equivalent of a sonic boom.

    Quick Tips:
    - Cherenkov radiation occurs when a particle's speed exceeds the phase velocity of light in the medium.
24 Easy
Analyzing +4 | -1
A proton moving with a constant velocity passes through a region of space without any change in its velocity. If E⃗\vec{E} and B⃗\vec{B} represent the electric and magnetic fields respectively, then the region of space may have:

(A) E=0,B=0E=0, B=0

(B) E=0,B≠0E=0, B \neq 0

(C) E≠0,B=0E \neq 0, B=0

(D) E≠0,B≠0E \neq 0, B \neq 0

Choose the most appropriate answer from the options given below:
View answer and explanation
Correct option: C
(A), (B) and (D) only
Option C ((A), (B) and (D) only) is correct because a proton can move with constant velocity if there are no fields, only a magnetic field (velocity parallel to B), or both electric and magnetic fields such that their forces cancel out.
Solution approach
  1. Correct Answer + Core Reason: (A), (B) and (D) only. A proton can move with constant velocity if the net force on it is zero.

    Step-by-Step Solution:

    Step 1: Analyze each case:
    - (A) E=0,B=0E=0, B=0: If both electric and magnetic fields are zero, the net force on the proton is zero, and it will move with constant velocity. This is possible.
    - (B) E=0,B≠0E=0, B \neq 0: If the electric field is zero and there is only a magnetic field, the force on the proton is given by the Lorentz force F⃗=q(v⃗×B⃗)\vec{F} = q(\vec{v} \times \vec{B}). If the velocity v⃗\vec{v} is parallel to the magnetic field B⃗\vec{B}, then v⃗×B⃗=0\vec{v} \times \vec{B} = 0, and the force is zero. This is possible.
    - (C) E≠0,B=0E \neq 0, B=0: If there is an electric field but no magnetic field, the force on the proton is given by F⃗=qE⃗\vec{F} = q\vec{E}. Since E≠0E \neq 0, the force is non-zero, and the proton will accelerate. This is not possible.
    - (D) E≠0,B≠0E \neq 0, B \neq 0: If both electric and magnetic fields are present, the net force on the proton is given by F⃗=q(E⃗+v⃗×B⃗)\vec{F} = q(\vec{E} + \vec{v} \times \vec{B}). It is possible for the electric and magnetic forces to cancel each other out, resulting in zero net force and constant velocity. This is possible.

    Step 2: Based on the analysis, cases (A), (B), and (D) are possible.

    Final Answer: (A), (B) and (D) only

    Why other options are wrong:
    - Option A ((A), (C) and (D) only): Option (C) is incorrect because a non-zero electric field without a magnetic field will cause the proton to accelerate.
    - Option B ((A), (B) and (C) only): Option (C) is incorrect because a non-zero electric field without a magnetic field will cause the proton to accelerate.
    - Option D ((B), (C) and (D) only): Option (C) is incorrect because a non-zero electric field without a magnetic field will cause the proton to accelerate, and option (A) is possible.

    Key Concepts:
    - Lorentz force
    - Electric force
    - Magnetic force
    - Constant velocity

    Memory Aids:
    - F⃗=q(E⃗+v⃗×B⃗)\vec{F} = q(\vec{E} + \vec{v} \times \vec{B}) (Lorentz force equation)
    - If v⃗\vec{v} is parallel to B⃗\vec{B}, then v⃗×B⃗=0\vec{v} \times \vec{B} = 0.

    Quick Tips:
    - Remember that the net force on the particle must be zero for it to move with constant velocity.
    - Consider the direction of the velocity relative to the magnetic field.
25 Easy
Understanding +4 | -1
If E→  and  B→\overrightarrow E \,\,\mathrm{and}\,\,\overrightarrow B are the electric and magnetic field vectors of E.M waves then the direction of propagation of E.M wave is along the direction of
View answer and explanation
Correct option: C
E→×B→\overrightarrow E \times \overrightarrow B
Option C, E→×B→\overrightarrow E \times \overrightarrow B, is correct because the direction of propagation of an electromagnetic wave is given by the Poynting vector, which is proportional to the cross product of the electric and magnetic field vectors.
Solution approach
  1. Correct Answer + Core Reason: E→×B→\overrightarrow E \times \overrightarrow B. The direction of propagation is given by the Poynting vector, which is proportional to the cross product of the electric and magnetic fields.

    Step-by-Step Solution:

    Step 1: Recall the definition of the Poynting vector.

    Step 2: The Poynting vector (S→\overrightarrow S) is given by: S→=1μ0(E→×B→)\overrightarrow S = \frac{1}{\mu_0} (\overrightarrow E \times \overrightarrow B)

    Step 3: The Poynting vector represents the direction of energy flow, which is also the direction of propagation of the electromagnetic wave. Therefore, the direction of propagation is along the direction of E→×B→\overrightarrow E \times \overrightarrow B.

    Why other options are wrong:
    - Option A: E→\overrightarrow E is incorrect because the direction of propagation is not solely determined by the electric field vector.
    - Option B: B→\overrightarrow B is incorrect because the direction of propagation is not solely determined by the magnetic field vector.
    - Option D: None of these is incorrect because the direction of propagation is given by E→×B→\overrightarrow E \times \overrightarrow B.

    Key Concepts:
    - Poynting vector
    - Direction of propagation of electromagnetic waves

    Memory Aids:
    - Remember that the direction of propagation is given by the cross product of the electric and magnetic fields.

    Quick Tips:
    - Always remember the definition of the Poynting vector.
26 Easy
Application +4 | -1
A plane electromagnetic wave travels in a medium of relative permittivity 2 and relative permeability 8.0.8.0. If the magnitude of magnetic intensity is 6π×10−2 A/m\frac{6}{\pi} \times 10^{-2} \mathrm{~A} / \mathrm{m} at a point, then the electric field at that point in ___ V/m\mathrm{V} / \mathrm{m}.
View answer and explanation
Correct option: A
1.801.80
Option A (1.80) is correct because the electric field is calculated using the formula E=vBE = vB, where v=cμrϵrv = \frac{c}{\sqrt{\mu_r \epsilon_r}} is the speed of light in the medium.
Solution approach
  1. Correct Answer + Core Reason: 1.801.80. The electric field is calculated using the formula E=vBE = vB, where vv is the speed of light in the medium.

    Step-by-Step Solution:

    Step 1: Identify the given values: Relative permittivity ϵr=2\epsilon_r = 2, relative permeability μr=8.0\mu_r = 8.0, and magnetic intensity H=6π×10−2 A/mH = \frac{6}{\pi} \times 10^{-2} \text{ A/m}.

    Step 2: Calculate the magnetic field BB using the relation B=μH=μ0μrHB = \mu H = \mu_0 \mu_r H, where μ0=4π×10−7 H/m\mu_0 = 4\pi \times 10^{-7} \text{ H/m}.
    B=(4π×10−7 H/m)×8.0×(6π×10−2 A/m)=192×10−9 TB = (4\pi \times 10^{-7} \text{ H/m}) \times 8.0 \times (\frac{6}{\pi} \times 10^{-2} \text{ A/m}) = 192 \times 10^{-9} \text{ T}

    Step 3: Calculate the speed of light in the medium: v=cϵrμr=3×108 m/s2×8=3×1084=0.75×108 m/sv = \frac{c}{\sqrt{\epsilon_r \mu_r}} = \frac{3 \times 10^8 \text{ m/s}}{\sqrt{2 \times 8}} = \frac{3 \times 10^8}{4} = 0.75 \times 10^8 \text{ m/s}.

    Step 4: Calculate the electric field EE using the relation E=vB=(0.75×108 m/s)×(192×10−9 T)=1.8 V/mE = vB = (0.75 \times 10^8 \text{ m/s}) \times (192 \times 10^{-9} \text{ T}) = 1.8 \text{ V/m}.

    Why other options are wrong:
    - Option B: 1.791.79 is close but incorrect due to rounding errors.
    - Option C: 1.51.5 is incorrect because it doesn't follow from the correct calculation.
    - Option D: 1 is incorrect because it doesn't follow from the correct calculation.

    Key Concepts:
    - Electromagnetic waves
    - Relative permittivity and permeability
    - Speed of light in a medium
    - Relationship between electric and magnetic fields

    Memory Aids:
    - Remember the relation E=vBE = vB and v=cϵrμrv = \frac{c}{\sqrt{\epsilon_r \mu_r}}.

    Quick Tips:
    - Always remember to account for the relative permittivity and permeability when calculating the speed of light in a medium.
27 Easy
Application +4 | -1
The wave function [in S.I unit] for an electromagnetic wave is given as ψ(x,t)=103sin⁡π[3×106x−9×1014t]\psi \left( {x,t} \right) = {10^3}\sin \pi \left[ {3 \times {{10}^6}x - 9 \times {{10}^{14}}t} \right] The speed of the wave is [in m/s]
View answer and explanation
Correct option: B
3×1083 \times {10^8}
Option B (3×1083 \times {10^8}) is correct because the speed of the wave can be found by dividing the coefficient of t by the coefficient of x.
Solution approach
  1. Correct Answer + Core Reason: 3×1083 \times {10^8}. The speed of the wave is found by dividing the coefficient of t by the coefficient of x.

    Step-by-Step Solution:

    Step 1: Identify the general form of a wave function: ψ(x,t)=Asin⁡(kx−ωt)\psi(x, t) = A \sin(kx - \omega t), where A is the amplitude, k is the wave number, and ω\omega is the angular frequency.

    Step 2: Given the wave function ψ(x,t)=103sin⁡π[3×106x−9×1014t]\psi(x, t) = {10^3}\sin \pi [3 \times {10^6}x - 9 \times {10^{14}}t].

    Step 3: Identify the values of k and ω\omega: k=3×106πk = 3 \times {10^6}\pi and ω=9×1014π\omega = 9 \times {10^{14}}\pi.

    Step 4: Calculate the speed of the wave (v) using the formula v=ωkv = \frac{\omega}{k}.

    Step 5: Substitute the values of ω\omega and k into the equation: v=9×1014π3×106π=3×108 m/sv = \frac{9 \times {10^{14}}\pi}{3 \times {10^6}\pi} = 3 \times {10^8} \text{{ m/s}}.

    Why other options are wrong:
    - Option A: 9×10149 \times {10^{14}} is incorrect because it is the angular frequency, not the speed of the wave.
    - Option C: 3×1063 \times {10^6} is incorrect because it is related to the wave number, not the speed of the wave.
    - Option D: 3×1073 \times {10^7} is incorrect because it is not the correct calculation of the speed of the wave.

    Key Concepts:
    - Wave function
    - Wave number
    - Angular frequency
    - Speed of wave

    Memory Aids:
    - Remember the relationship v=ωkv = \frac{\omega}{k}.

    Quick Tips:
    - Understand the general form of a wave function and how to extract the values of k and ω\omega.
28 Easy
Remembering +4 | -1
Rays in electromagnetic spectrum that has lowest frequency are
View answer and explanation
Correct option: A
Microwaves
Option A is correct because Microwaves have the lowest frequency among the given options in the electromagnetic spectrum.
Solution approach
  1. Correct Answer + Core Reason: Microwaves. Microwaves have the lowest frequency among the given options.

    Step-by-Step Solution:

    Step 1: Recall the order of the electromagnetic spectrum from lowest to highest frequency: Radio waves, Microwaves, Infrared, Visible light, Ultraviolet, X-rays, Gamma rays.

    Step 2: Compare the frequencies of the given options:
    - Microwaves have lower frequencies than infrared, visible light, ultraviolet, and X-rays.
    - Ultraviolet rays have higher frequencies than microwaves, infrared, and visible light.
    - Infrared rays have higher frequencies than microwaves.
    - X-rays have higher frequencies than microwaves, infrared, and ultraviolet rays.

    Step 3: From the given options, microwaves have the lowest frequency.

    Why other options are wrong:
    - Option B: Ultraviolet rays. Ultraviolet rays have higher frequencies than microwaves.
    - Option C: Infrared rays. Infrared rays have higher frequencies than microwaves.
    - Option D: X-rays. X-rays have higher frequencies than microwaves.

    Key Concepts:
    - Electromagnetic Spectrum
    - Frequency

    Memory Aids:
    - Remember the order of the electromagnetic spectrum.

    Quick Tips:
    - Know the relative positions of different types of electromagnetic radiation in the spectrum.
29 Easy
Understanding +4 | -1
In the case of a photon :-
View answer and explanation
Correct option: D
Its speed can change but cannot become equal to zero.
Option D (Its speed can change but cannot become equal to zero) is correct because a photon always travels at the speed of light in a given medium, and it cannot be stopped.
Solution approach
  1. Correct Answer + Core Reason: Its speed can change but cannot become equal to zero. A photon always travels at the speed of light in a given medium.

    Step-by-Step Solution:

    Step 1: Recall properties of a photon: A photon is a massless particle that always travels at the speed of light in vacuum (cc).

    Step 2: Photon speed in a medium: When a photon enters a medium, its speed changes to v=c/nv = c/n, where nn is the refractive index of the medium. However, it never becomes zero.

    Step 3: Final Answer: Its speed can change but cannot become equal to zero.

    Why other options are wrong:
    - Option A: This is incorrect because the energy of a photon is proportional to its frequency (E=hfE = hf) and not the square of its velocity (which is constant in a given medium).
    - Option B: This is incorrect because a photon's energy remains constant unless it interacts with matter. It doesn't lose energy simply by entering a denser medium.
    - Option C: This is incorrect because photons can interact, although photon-photon scattering is a rare event.

    Key Concepts:
    - Properties of a photon
    - Speed of light in a medium
    - Energy of a photon

    Memory Aids:
    - Photons are always moving!

    Quick Tips:
    - Remember that photons are massless and always travel at the speed of light (in a vacuum).
30 Easy
Application +4 | -1
The velocity of electromagnetic waves in a dielectric medium of constant 4 is
View answer and explanation
Correct option: A
1.5×108ms−11.5 \times {10^8}\mathrm{m}{\mathrm{s}^{ - 1}}
Option A (1.5×108  ms−11.5 \times {10^8}\mathrm{\;m}{\mathrm{s}^{ - 1}}) is correct because the velocity of electromagnetic waves in a dielectric medium is given by v=c/ϵrv = c / \sqrt{\epsilon_r}, where ϵr\epsilon_r is the dielectric constant.
Solution approach
  1. Correct Answer + Core Reason: 1.5×108  ms−11.5 \times {10^8}\mathrm{\;m}{\mathrm{s}^{ - 1}}. The velocity of EM waves in a dielectric is reduced by a factor of ϵr\sqrt{\epsilon_r}.

    Step-by-Step Solution:

    Step 1: Formula: The velocity of electromagnetic waves in a dielectric medium is given by v=cϵrv = \frac{c}{\sqrt{\epsilon_r}}, where cc is the speed of light in vacuum and ϵr\epsilon_r is the dielectric constant.

    Step 2: Substitution: Given ϵr=4\epsilon_r = 4 and c=3×108 m/sc = 3 \times 10^8 \text{ m/s}, we have v=3×1084v = \frac{3 \times 10^8}{\sqrt{4}}.

    Step 3: Calculation: v=3×1082=1.5×108 m/sv = \frac{3 \times 10^8}{2} = 1.5 \times 10^8 \text{ m/s}.

    Step 4: Final Answer: 1.5×108  ms−11.5 \times {10^8}\mathrm{\;m}{\mathrm{s}^{ - 1}}

    Why other options are wrong:
    - Option B: This is the speed of light in vacuum, not in a dielectric medium with a dielectric constant of 4.
    - Option C: This is incorrect. The velocity is reduced, not doubled.
    - Option D: This is incorrect. The velocity is reduced, not quadrupled.

    Key Concepts:
    - Velocity of electromagnetic waves in a dielectric medium
    - Dielectric constant

    Memory Aids:
    - Dielectric slows down EM waves.

    Quick Tips:
    - Remember the formula v=cϵrv = \frac{c}{\sqrt{\epsilon_r}}.
Revision notes and key takeaways

Review ELECTROMAGNETIC WAVES in your textbook or class notes, then use this set to check your understanding.

Key Takeaways

  • ✓ This set contains 35 single-correct-answer MCQs on ELECTROMAGNETIC WAVES.
  • ✓ Try each question before opening its answer. Read the explanation where one is available.
  • ✓ Sign in to save submitted answers. Revisit incorrect answers alongside your textbook or class notes.
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