Electromagnetic Waves
$\overrightarrow B $ = 8.0 $\times$ 10$-$8 $\widehat z$T. The value of electric field at this point is :
(speed of light = 3 $\times$ 108 ms$-$1)
$\widehat x$, $\widehat y$, $\widehat z$ are unit vectors along x, y and z directions.
| List I | List II | ||
|---|---|---|---|
| (a) | Source of microwave frequency | (i) | Radioactive decay of nucleus |
| (b) | Source of infrared frequency | (ii) | Magnetron |
| (c) | Source of Gamma Rays | (iii) | Inner shell electrons |
| (d) | Source of X-rays | (iv) | Vibration of atoms and molecules |
| (v) | LASER | ||
| (vi) | RC circuit |
Choose the correct answer from the options given below :
The energy contained in a cylinder of volume V is 5.5 $\times$ 10$-$12 J. The value of V is _____________ cm3. (given $\in$0 = 8.8 $\times$ 10$-$12C2N$-$1m$-$2)
Explanation:
Energy density = ${1 \over 2}{ \in _0}E_0^2$
Energy of volume $V = {1 \over 2}{ \in _0}E_0^2.\,V = 5.5 \times {10^{ - 12}}$
${1 \over 2}8.8 \times {10^{ - 12}} \times 2500V = 5.5 \times {10^{ - 12}}$
$V = {{5.5 \times 2} \over {2500 \times 8.8}} = .0005{m^3}$
= .0005 $\times$ 106 (c.m)3
= 500 (c.m)3
Explanation:
= 2 $\times$ 10$-$8 T
$\therefore$ x = 2
$\overrightarrow E = 200\cos \left[ {\left( {{{0.5 \times {{10}^3}} \over m}} \right)x - \left( {1.5 \times {{10}^{11}}{{rad} \over s} \times t} \right)} \right]{V \over m}\widehat j$. If this wave falls normally on a perfectly reflecting surface having an area of 100 cm2. If the radiation pressure exerted by the E.M. wave on the surface during a 10 minute exposure is ${x \over {{{10}^9}}}{N \over {{m^2}}}$. Find the value of x .
Explanation:
$I = {1 \over 2}{\varepsilon _0}E_0^2.C$
Radiation pressure
$P = {{2I} \over C}$
$ = \left( {{2 \over C}} \right)\left( {{1 \over 2}{\varepsilon _0}E_0^2C} \right)$
$ = {\varepsilon _0}E_0^2$
$ = 8.85 \times {10^{ - 12}} \times {200^2}$
$ = 8.85 \times {10^{ - 8}} \times 4$
$ = {{354} \over {{{10}^9}}}$
Explanation:
${E^2} \propto I$
$I = {{Power} \over {Area}}$
${E^2} \propto {P \over A}$
$E \propto \sqrt P $
${{E'} \over E} = \sqrt {{{60} \over {100}}} $
$E' = \sqrt {{3 \over 5}} E$
So the value of x = 3
Explanation:
Given f = 9 $\times$ 102 Hz
$ \in $ = $ \in $0$ \in $r
$ \in $ = 80 $ \in $0
So $ \in $r = 80
$\rho $ = 0.25 $\Omega$m
V(t) = V0 sin (2$\pi$ft)
${I_d} = {{dq} \over {dt}} = {{cdv} \over {dt}}$
${I_d} = {{{ \in _0}{ \in _r}A} \over d}{d \over {dt}}({v_0}\sin (2\pi ft))$
${I_d} = {{{ \in _0}{ \in _r}A} \over d}{V_0}(2\pi f)\cos (2\pi ft)$ .......... (1)
& ${I_c} = {V \over R}$
${I_c} = {{{V_0}\sin (2\pi ft)} \over {\rho {d \over A}}} = {{A{v_0}\sin (2\pi ft)} \over {\rho d}}$ ....... (2)
divide equation (1) and (2)
${{{I_d}} \over {{I_c}}} = { \in _0}{ \in _r}2\pi f(\rho )\cot (2\pi ft)$
${{{I_d}} \over {{I_c}}} = {1 \over {4\pi \times 9 \times {{10}^9}}} \times 80 \times 2\pi \times 9 \times {10^2} \times (0.25) \times \cot (2\pi \times 9 \times {10^2} \times {1 \over {800}})$
$ = {{{{10}^3}} \over {{{10}^9}}}\left( {\cot \left( {{{9\pi } \over 4}} \right)} \right)$
$ = {{{{10}^3}} \over {{{10}^9}}}$
${{{I_d}} \over {{I_c}}} = {1 \over {{{10}^6}}}$
${I_c} = {10^6}{I_d}$
So x = 6
(Assume complete absorption and normal incidence conditions are there)
Explanation:
I = P $\times$ C
I = ${{2.5 \times {{10}^{ - 6}}} \over {30c{m^2}}}$ N $\times$ 3 $\times$ 108 m/s
I = 25 W/cm2
Explanation:
$I = {1 \over 2}c{\varepsilon _0}E_0^2 = {P \over {4\pi {r^2}}}$
${1 \over 2}4\pi {\varepsilon _0} \times c \times E_0^2 = {P \over {{r^2}}}$
${1 \over 2} \times {{3 \times {{10}^5} \times E_0^2} \over {9 \times {{10}^9}}} = {{1000 \times 1.25} \over {{{(2)}^2}}} \times {1 \over {100}}$
$E_0^2 = {{60 \times 1000 \times 1.25} \over {4 \times 100}} = {{125 \times 3} \over 2}$
$E_0^2 = {{375} \over 2} = 187.5$
${E_0} = 13.69$
${E_0} \approx 137 \times {10^{ - 1}}$ v/m
Explanation:
$I = \frac{P}{4\pi r^2} \tag{1}$ ........(1)
This intensity can also be related to the electric field (E) in an electromagnetic wave using the equation :
$I = \frac{1}{2} c \varepsilon_0 E^2 \tag{2}$ .........(2)
where $c=\frac{1}{\sqrt{\mu_0 \varepsilon_0}}=$ speed of light in vacuum and $\varepsilon_0$ is the permittivity of free space.
From equations (1) and (2), we can solve for E and square root it to find the peak value of the electric field $E_{\text{peak}}$ :
$E_{\text{peak}} = \sqrt{\frac{2P}{c \varepsilon_0 4\pi r^2}} = \sqrt{\frac{2P \mu_0 c}{4\pi r^2}}$
Since $ \varepsilon_0=\frac{1}{\mu_0 c^2} $
Given the efficiency of the bulb is 10%, the actual power radiated is $0.10 \times 8\, \text{W} = 0.8\, \text{W}$.
So, substituting $P = 0.8\, \text{W}$, $r = 10\, \text{m}$, $c = 3 \times 10^8\, \text{m/s}$, and $\mu_0 = 4\pi \times 10^{-7}\, \text{T m/A}$, we have :
$E_{\text{peak}} = \sqrt{\frac{2 \times 0.8 \times 4\pi \times 10^{-7} \times 3 \times 10^8}{4\pi \times 100}} = \frac{x}{10} \sqrt{\frac{\mu_0 c}{\pi}}$
Comparing with the expression in the question, we find that $x = 2$.
Therefore, the answer is $x = 2$.
Explanation:
$ \because $ E = ${{hc} \over \lambda } = m{c^2}$
$ \Rightarrow $ m = ${h \over {c\lambda }}$
The mass of a fictitious particle having the same energy as that of the x-ray photons = ${x \over 3}$h kg
$ \therefore $ ${x \over 3}h = {h \over {c\lambda }}$
$x = {3 \over {c\lambda }}$
$ = {3 \over {3 \times {{10}^8} \times 10 \times {{10}^{ - 10}}}}$
x = 10
Explanation:
Relative permittivity, $\varepsilon $r = 2.25
Since, f = C/$\lambda$
$ \Rightarrow \lambda = {c \over f} = {{3 \times {{10}^8}} \over {3 \times {{10}^9}}} = 0.1$ m
$\because$ $\lambda$m (wavelength of wave in a medium) = $\lambda$/$\mu$ and we know that, $\mu = \sqrt {{\mu _r}{\varepsilon _r}} $
As, dielectric is non-magnetic, $\mu$r = 1
$ \Rightarrow \mu = \sqrt {2.25} = 1.5$
$ \Rightarrow {\lambda _m} = {{0.1} \over {1.5}} = {1 \over {15}} = 0.0667$ m
= 6.67 cm = 667 $\times$ 10$-$2 cm
Explanation:
where, $\mu$r is relative permeability, $\varepsilon $r is relative permittivity.
Speed of electromagnetic wave v is given by
$v = {c \over n}$
where, n = refractive index = $\sqrt {{\mu _r}{\varepsilon _r}} = \sqrt 4 = 2$
$ \Rightarrow v = {{3 \times {{10}^8}} \over 2}$ = 15 $\times$ 107 m/s
$\because$ x $\times$ 107 = 15 $\times$ 107
$\Rightarrow$ x = 15
The electric and the magnetic fields associated with an electromagnetic wave propagating along the $z$-axis, can be represented by
The magnetic field of a plane electromagnetic wave is given by $B=(400 \propto \mathrm{T})\sin \left[\left(4.0 \times 10^{15} \mathrm{~s}^{-1}\right)\left(t-\frac{x}{c}\right)\right]$. Average energy density corresponding to the electric field is
In an amplitude modulated signal, the maximum amplitude is $15 \mathrm{~V}$ and minimum amplitude is $5 \mathrm{~V}$. The amplitude of modulating wave will be
$\overrightarrow B \left( {x,t} \right)$ = $\left[ {1.2 \times {{10}^{ - 7}}\sin \left( {0.5 \times {{10}^3}x + 1.5 \times {{10}^{11}}t} \right)\widehat k} \right]$ T
The instantaneous electric field $\overrightarrow E $ corresponding to $\overrightarrow B $ is :
(speed of light c = 3 × 108 ms–1)
| I | II |
|---|---|
| Radiation | Wavelength |
| (a) Microwave | (i) 100 m |
| (b) Gamma rays | (ii) 10–15 m |
| (c) A.M. radio waves | (iii) 10–10 m |
| (d) X-rays | (iv) 10–3 m |
$\overrightarrow E = 30\widehat j\sin \left( {1.5 \times {{10}^7}t - 5 \times {{10}^{ - 2}}x} \right)$ V/m.
The maximum magnetic force experienced by the electron will be :
(given c = 3 $ \times $ 108 ms–1 and electron charge = 1.6 $ \times $ 10–19 C)
$\overrightarrow E = {E_0}\left( {\widehat x + \widehat y} \right)\sin \left( {kz - \omega t} \right)$
Its magnetic field will be given by :
$\overrightarrow E = {E_0}\widehat j\cos \left( {\omega t - kx} \right)$.
The magnetic field $\overrightarrow B $ , at the moment t = 0 is :
$\overrightarrow B = 3 \times {10^{ - 8}}\sin \left[ {200\pi \left( {y + ct} \right)} \right]\widehat i$ T
where c = 3 $ \times $ 108 ms–1 is the speed of light. The corresponding electric field is :
frequency of 2.0 $ \times $ 1010 Hz and its energy density is 1.02 $ \times $ 10–8 J/m3 in vacuum. The amplitude of the magnetic field of the wave is close to
( ${1 \over {4\pi {\varepsilon _0}}} = 9 \times {10^9}{{N{m^2}} \over {{C^2}}}$ and speed of light
= 3 $ \times $ 108 ms–1)
$\overrightarrow {{E_1}} = {E_0}\widehat j\cos \left( {\omega t - kx} \right)$ and
$\overrightarrow {{E_2}} = {E_0}\widehat k\cos \left( {\omega t - ky} \right)$
At t = 0, a particle of charge q is at origin with
a velocity $\overrightarrow v = 0.8c\widehat j$ (c is the speed of light in vacuum). The instantaneous force experienced by the particle is :
$\overrightarrow E = {E_0}{{\widehat i + \widehat j} \over {\sqrt 2 }}\cos \left( {kz + \omega t} \right)$
At t = 0, a positively charged particle is at the point (x, y, z) = $\left( {0,0,{\pi \over k}} \right)$.
If its instantaneous velocity at (t = 0) is ${v_0}\widehat k$ , the force acting on it due to the wave is :
$\overrightarrow B $ = 3 $ \times $ 10-8 sin(1.6 $ \times $ 103x + 48 $ \times $ 1010t)$\widehat j$ T, then what will be expression for electric field ?
The rms electric field, in units of V/m associated with this source is close to the nearest integer is __________.
$ \in $0 = 8.86 × 10–12 C2 Nm–2; c = 3 × 108 ms–1)
Explanation:
$ \Rightarrow $ E0 = $\sqrt {{{2I} \over {{\varepsilon _0}c}}} $
$ \therefore $ Erms = ${{{E_0}} \over {\sqrt 2 }}$ = $\sqrt {{I \over {{\varepsilon _0}c}}} $
= $\sqrt {{{{{315} \over \pi }} \over {8.86 \times {{10}^{ - 12}} \times 3 \times {{10}^8}}}} $
= 194
The typical wavelength of X-ray is
$10^{-10} \mathrm{~m}$
$10^{-15} \mathrm{~m}$
$10^{-6} \mathrm{~m}$
$10^6 \mathrm{~m}$
The radiation energy emitted per second by a point source is 100 W . If the efficiency of the source is $4 \%$, then the rms value of the electric field at distance of 2 m is [use $\frac{1}{4 \pi \varepsilon_0}=9 \times 10^9$ in SI unit]
$\sqrt{60} \mathrm{~V} / \mathrm{m}$
$\sqrt{30} \mathrm{~V} / \mathrm{m}$
$\sqrt{50} \mathrm{~V} / \mathrm{m}$
$\sqrt{40} \mathrm{~V} / \mathrm{m}$
A parallel-plate capacitor with circular plates is being discharged. The radius of the circular plate is 10 cm . A circular loop of radius 20 cm is concentric with the capacitor and located halfway between the plates. If the electric field between the plates is charging at the rate $3.6 \times 10^{12} \mathrm{~V} /(\mathrm{ms})$, then the displacement current through the loop is
$ \text { (Assume } \frac{1}{4 \pi \varepsilon_0}=9 \times 10^9 \mathrm{Nm}^2 / \mathrm{C}^2 \text { ) } $
1 A
2 A
3 A
4 A
What is the amplitude of the electric field in a parallel beam of light intensity $\left(\frac{15}{\pi}\right) \frac{\mathrm{W}}{\mathrm{m}^2}$ ?
$ \left[\text { Assume }, \frac{1}{4 \pi \varepsilon_0}=9 \times 10^9 \frac{\mathrm{Nm}^2}{\mathrm{C}^2}\right] $
$60 \mathrm{~N} / \mathrm{C}$
$50 \mathrm{~N} / \mathrm{C}$
$40 \mathrm{~N} / \mathrm{C}$
$30 \mathrm{~N} / \mathrm{C}$
$\overrightarrow E = {E_0}\widehat i\cos (kz)cos(\omega t)$
The corresponding magnetic field $\overrightarrow B $ is then given by
$$\overline B = {B_0}\widehat i\left[ {\cos (kz - \omega t)} \right] + {B_i}\widehat j\cos (kz + \omega t)$$ B0 = 3 × 10–5 T and B1 = 2 × 10–6 T.
The rms value of the force experienced by a stationary charge Q = 10–4 C at z = 0 is closest to :
$\mathop B\limits^ \to = 1.6 \times {10^{ - 6}}\cos \left( {2 \times {{10}^7}z + 6 \times {{10}^{15}}t} \right)\left( {2\mathop i\limits^ \wedge + \mathop j\limits^ \wedge } \right){{Wb} \over {{m^2}}}$
The associated electric field will be :-
[Given permittivity of space $ \in $0 = 9 $ \times $ 10–12 SI units, Speed of light c = 3 $ \times $ 108 m/s]
