Electromagnetic Waves

JEE Physics · 127 questions · Page 1 of 13 · Click an option or "Show Solution" to reveal answer

Q1
For an electromagnetic wave travelling in free space, the relation between average energy densities due to electric (Ue) and magnetic (Um) fields is :
A Ue = Um
B Ue \ne Um
C Ue < Um
D Ue > Um
Correct Answer
Option A
Solution

In EMW, average energy density due to electric field (Ue) and magnetic field (Um) is same.

Q2
Electromagnetic waves are transverse in nature is evident by
A polarization
B interference
C reflection
D diffraction
Correct Answer
Option A
Solution

The phenomenon of polarisation is shown only by transverse waves.

Q3
Light is incident normally on a completely absorbing surface with an energy flux of 25 W cm–2. If the surface has an area of 25 cm2, the momentum transferred to the surface in 40 min time duration will be :
A 6.3 × 10–4 Ns
B 5.0 × 10–3 Ns
C 1.4 × 10–6 Ns
D 3.5 × 10–6 Ns
Correct Answer
Option B
Solution
P=ΔECP = {{\Delta E} \over C}
=(25×25)×40×603×108Ns= {{\left( {25 \times 25} \right) \times 40 \times 60} \over {3 \times {{10}^8}}}N - s
=5×102Ns= 5 \times {10^{ - 2}}N - s
Q4
Choose the correct option relating wave lengths of different parts of electromagnetic wave spectrum:
A λ\lambda radio waves > λ\lambda micro waves > λ\lambda visible > λ\lambda x-rays
B λ\lambda visible > λ\lambda x-rays > λ\lambda radio waves > λ\lambda micro waves
C λ\lambda visible < λ\lambda micro waves < λ\lambda radio waves < λ\lambda x-rays
D λ\lambda x-rays < λ\lambda micro waves < λ\lambda radio waves < λ\lambda visible
Correct Answer
Option A
Solution

Decreasing order of wavelength, Radio wave > Microwave > Infrared > ROYGBIV(Visiable Resion) > Ultraviolet > X rays > γ\gamma rays So the correct order - λ\lambdaradio waves > λ\lambdamicro waves > λ\lambdavisible > λ\lambdax-rays

Q5
A plane electromagnetic wave propagating along y-direction can have the following pair of electric field (E)\left( {\overrightarrow E } \right) and magnetic field (B)\left( {\overrightarrow B } \right) components.
A Ex, Bz or Ez, Bx
B Ex, By or Ey, Bx
C Ey, By or Ez, Bz
D Ey, Bx or Ex, By
Correct Answer
Option A
Solution

\because

E^×B^=C^\widehat E \times \widehat B = \widehat C

\therefore

E^×B^\widehat E \times \widehat B

should point in the direction of propagation of wave (y-direction here) \therefore possible combinations are (Ex, Bz) or (Ez, Bx)

Q6
In an electromagnetic wave the electric field vector and magnetic field vector are given as E=E0i^\overrightarrow E = {E_0}\widehat i and B=B0k^\overrightarrow B = {B_0}\widehat k respectively. The direction of propagation of electromagnetic wave is along :
A (k^)\left( {\widehat k} \right)
B j^\widehat j
C (k^)\left( { - \widehat k} \right)
D (j^)\left( { - \widehat j} \right)
Correct Answer
Option D
Solution

Direction of propagation =

E×B=i^×k^=j^\overrightarrow E \times \overrightarrow B = \widehat i \times \widehat k = - \widehat j
Q7
Sun light falls normally on a surface of area 36 cm236 \mathrm{~cm}^{2} and exerts an average force of 7.2×109 N7.2 \times 10^{-9} \mathrm{~N} within a time period of 20 minutes. Considering a case of complete absorption, the energy flux of incident light is
A 25.92×102 W/cm225.92 \times 10^{2} \mathrm{~W} / \mathrm{cm}^{2}
B 8.64×106 W/cm28.64 \times 10^{-6} \mathrm{~W} / \mathrm{cm}^{2}
C 6.0 W/cm26.0 \mathrm{~W} / \mathrm{cm}^{2}
D 0.06 W/cm20.06\mathrm{~W} / \mathrm{cm}^{2}
Correct Answer
Option D
Solution

Pressure

=lc= {l \over c}
FA=lc\Rightarrow {F \over A} = {l \over c}
l=7.2×109×3×10836×104\Rightarrow l = {{7.2 \times {{10}^{ - 9}} \times 3 \times {{10}^8}} \over {36 \times {{10}^{ - 4}}}}

W/m2

=600= 600

W/m2

l=0.06\Rightarrow l = 0.06

W/cm2

Q8
An electromagnetic wave is transporting energy in the negative zz direction. At a certain point and certain time the direction of electric field of the wave is along positive yy direction. What will be the direction of the magnetic field of the wave at that point and instant?
A Negative direction of yy
B Positive direction of zz
C Positive direction of xx
D Negative direction xx
Correct Answer
Option C
Solution

As, poynting vector

S=E×H\overrightarrow{\mathrm{S}}=\overrightarrow{\mathrm{E}} \times \overrightarrow{\mathrm{H}}

Given energy transport == negative z\mathrm{z} direction Electric field == positive y\mathrm{y} direction (k^)=(+j^)×[i^](-\hat{\mathrm{k}})=(+\hat{\mathrm{j}}) \times[\hat{\mathrm{i}}] Hence according to vector cross product magnetic field should be positive x\mathrm{x} direction.

Q9
A plane electromagnetic wave propagating in x\mathrm{x}-direction is described by Ey=(200Vm1)sin[1.5×107t0.05x]E_y=\left(200 \mathrm{Vm}^{-1}\right) \sin \left[1.5 \times 10^7 t-0.05 x\right] \text{; } The intensity of the wave is : (Use ϵ0=8.85×1012C2 N1 m2\epsilon_0=8.85 \times 10^{-12} \mathrm{C}^2 \mathrm{~N}^{-1} \mathrm{~m}^{-2})
A 35.4 Wm235.4 \mathrm{~Wm}^{-2}
B 53.1 Wm253.1 \mathrm{~Wm}^{-2}
C 26.6 Wm226.6 \mathrm{~Wm}^{-2}
D 106.2 Wm2106.2 \mathrm{~Wm}^{-2}
Correct Answer
Option B
Solution
I=12ε0E02×cI=12×8.85×1012×4×104×3×108I=53.1 W/m2\begin{aligned} & \mathrm{I}=\frac{1}{2} \varepsilon_0 \mathrm{E}_0^2 \times \mathrm{c} \\ & \mathrm{I}=\frac{1}{2} \times 8.85 \times 10^{-12} \times 4 \times 10^4 \times 3 \times 10^8 \\ & \mathrm{I}=53.1 \mathrm{~W} / \mathrm{m}^2 \end{aligned}
Q10
Electromagnetic waves travel in a medium with speed of 1.5×108 m s11.5 \times 10^8 \mathrm{~m} \mathrm{~s}^{-1}. The relative permeability of the medium is 2.0. The relative permittivity will be:
A 4
B 1
C 2
D 5
Correct Answer
Option C
Solution
v=1μ0μrε0εr1.5×108=3×1082εrεr=2\begin{aligned} & v=\frac{1}{\sqrt{\mu_0 \mu_r \varepsilon_0 \cdot \varepsilon_r}} \\ & \Rightarrow 1.5 \times 10^8=\frac{3 \times 10^8}{\sqrt{2 \cdot \varepsilon_r}} \Rightarrow \varepsilon_r=2 \end{aligned}
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