Alternating Current

JEE Physics · 99 questions · Page 9 of 10 · Click an option or "Show Solution" to reveal answer

Q81
The core of any transformer is laminated so as to
A reduce the energy loss due to eddy currents
B make it light weight
C make it robust and strong
D increase the secondary voltage
Correct Answer
Option A
Solution

Laminated core provide less area of cross-section for the current to flow.

Because of this, resistance of the core increases and current decreases thereby decreasing the eddy current losses.

Q82
An ac current is represented as i=52+10cos(650πt+π6)Ampi=5 \sqrt{2}+10 \cos \left(650 \pi t+\dfrac{\pi}{6}\right) A m p The r.m.s value of the current is
A 10 Amp
B 52 Amp5 \sqrt{2} \mathrm{~Amp}
C 100 Amp
D 50 Amp
Correct Answer
Option A
Solution

To find the root mean square (RMS) value of the given alternating current, follow these steps: The current is represented as: i=52+10cos(650πt+π6)Amp i = 5\sqrt{2} + 10 \cos \left(650\pi t + \dfrac{\pi}{6}\right) \, \text{Amp} Here, the time-independent DC component is 525\sqrt{2} and the AC component is 10cos(650πt+π6)10 \cos \left(650\pi t + \dfrac{\pi}{6}\right).

Calculate the square of the current, i2i^2: i2=(52)2+(10cos(650πt+π6))2+2×52×10cos(650πt+π6) i^2 = \left(5\sqrt{2}\right)^2 + \left(10 \cos \left(650\pi t + \dfrac{\pi}{6}\right)\right)^2 + 2 \times 5\sqrt{2} \times 10 \cos \left(650\pi t + \dfrac{\pi}{6}\right) Simplifying, we have: i2=50+100cos2(650πt+π6)+1002cos(650πt+π6) i^2 = 50 + 100 \cos^2 \left(650\pi t + \dfrac{\pi}{6}\right) + 100\sqrt{2} \cos \left(650\pi t + \dfrac{\pi}{6}\right) Find the average value i2\langle i^2 \rangle: The average value of cos\cos terms over a period is zero, simplifying our equation to: i2=50+1002+0 \langle i^2 \rangle = 50 + \dfrac{100}{2} + 0 This simplifies to: i2=50+50=100 \langle i^2 \rangle = 50 + 50 = 100 Calculate the RMS current: The RMS value is the square root of the mean of the squares of the current: i=100=10Amp \langle i \rangle = \sqrt{100} = 10 \, \text{Amp} Thus, the RMS value of the current is 10 Amps.

Q83
A transformer consisting of 300 turns in the primary and 150 turns in the secondary gives output power of 2.2 kW. If the current in the secondary coil is 10A, then the input voltage and current in the primary coil are :
A 220 V and 20 A
B 220 V and 10A
C 440 V and 5A
D 440 V and 20 A
Correct Answer
Option C
Solution

Given NP = 300, Ns = 150, P0 = 2200W Is = 10 A P0 = V0I0 \Rightarrow 2200 = V0 × 10 \Rightarrow V0 = 220 V \because

ViV0=NPNSVi=2×220=440V{{{V_i}} \over {{V_0}}} = {{{N_P}} \over {{N_S}}} \Rightarrow {V_i} = 2 \times 220 = 440\,V

Also, P0 = ViIi

Ii=2200440=5A\Rightarrow {I_i} = {{2200} \over {440}} = 5A
Q84
A 10 Ω\Omega resistance is connected across 220V - 50 Hz AC supply. The time taken by the current to change from its maximum value to the rms value is :
A 2.5 ms
B 1.5 ms
C 3.0 ms
D 4.5 ms
Correct Answer
Option A
Solution

\Rightarrow i = i0sinω\omegat when i = i0 i0 = i0sinω\omegat1 \Rightarrow ω\omegat1 =

π2{\pi \over 2}

..... (i) When i =

i12{{{i_1}} \over {\sqrt 2 }}
i12{{{i_1}} \over {\sqrt 2 }}

= i0sinω\omegat2 \Rightarrow ω\omegat2 =

π4{\pi \over 4}

...... (ii) Time taken by current from maximum value to rms value

(t1t2)=π2ωπ4ω=π4ω=π4×2πf\Rightarrow ({t_1} - {t_2}) = {\pi \over {2\omega }} - {\pi \over {4\omega }} = {\pi \over {4\omega }} = {\pi \over {4 \times 2\pi f}}
=18×50= {1 \over {8 \times 50}}
1400{1 \over {400}}

sec = 2.5 ms

Q85
For a series LCR circuit with R = 100 Ω\Omega, L = 0.5 mH and C = 0.1 pF connected across 220V-50 Hz AC supply, the phase angle between current and supplied voltage and the nature of the circuit is :
A 0^\circ, resistive circuit
B \approx 90^\circ, predominantly inductive circuit
C 0^\circ, resonance circuit
D \approx 90^\circ, predominantly capacitive circuit
Correct Answer
Option D
Solution

R = 100

Ω\Omega
XL=ωL=50π×103{X_L} = \omega L = 50\pi \times {10^{ - 3}}
XC=1ωC=1011100π{X_C} = {1 \over {\omega C}} = {{{{10}^{11}}} \over {100\pi }}
XC>>XL{X_C} > > {X_L}

&

XCXL>>R\left| {{X_C} - {X_L}} \right| > > R
Q86
A resistor R'R' and 2μF2\mu F capacitor in series is connected through a switch to 200200 VV direct supply. Across the capacitor is a neon bulb that lights up at 120120 V.V. Calculate the value of RR to make the bulb light up 55 ss after the switch has been closed. (log102.5=0.4)\left( {{{\log }_{10}}2.5 = 0.4} \right)
A 1.7×105Ω1.7 \times {10^5}\,\Omega
B 2.7×106Ω2.7 \times {10^6}\,\Omega
C 3.3×107Ω3.3 \times {10^7}\,\Omega
D 1.3×104Ω1.3 \times {10^4}\,\Omega
Correct Answer
Option B
Solution

We have,

V=V0(1et/RC)V = {V_0}\left( {1 - {e^{ - t/RC}}} \right)
120200(1et/RC)\Rightarrow 120 - 200\left( {1 - {e^{ - t/RC}}} \right)
t=RCin(2.5)\Rightarrow t = RC\,in\,\left( {2.5} \right)
R=2.71×106Ω\Rightarrow R = 2.71 \times {10^6}\Omega
Q87

Match with

List - IList - II
(a) ωL>1ωC\omega L > {1 \over {\omega C}} (i) Current is in phase with emf
(b) ωL=1ωC\omega L = {1 \over {\omega C}} (ii) Current lags behind the applied emf
(c) ωL<1ωC\omega L < {1 \over {\omega C}} (iii) Maximum current occurs
(d) Resonant frequency (iv) Current leads the emf
A a(ii), b(i), c(iv), d(iii)
B a(ii), b(i), c(iii), d(iv)
C a(iii), b(i), c(iv), d(ii)
D a(iv), b(iii), c(ii), d(i)
Correct Answer
Option A
Solution
ωL=1ωC,XL=XC\omega L = {1 \over {\omega C}},{X_L} = {X_C}

So current in phase with EMF At resonance, current have maximum value.

Q88
AC voltage V(t) = 20 sinω\omegat of frequency 50 Hz is applied to a parallel plate capacitor. The separation between the plates is 2 mm and the area is 1 m2. The amplitude of the oscillating displacement current for the applied AC voltage is _________. [Take ε\varepsilon 0 = 8.85 ×\times 10-12 F/m]
A 55.58 μ\muA
B 21.14 μ\muA
C 27.79 μ\muA
D 83.37 μ\muA
Correct Answer
Option C
Solution

Given, AC voltage, V(t) = 20 sin ω\omegat volt.

Frequency, f = 50Hz Separation between the plates, d = 2 mm = 2 ×\times 10-3 m Area, A = 1 m2 As,

C=ε0AdC = {{{\varepsilon _0}A} \over d}

where,

ε0{{\varepsilon _0}}

= absolute electrical permittivity of free space = 8.854 ×\times 10-12 N-1 kg2m-2

C=ε0×12×103C = {{{\varepsilon _0} \times 1} \over {2 \times {{10}^{ - 3}}}}

.... (i) Capacitive reactance

(XC)=1ωC({X_C}) = {1 \over {\omega C}}

.... (ii) From Eqs. (i) and (ii), we get

XC=2×1032×50π×ε0{X_C} = {{2 \times {{10}^{ - 3}}} \over {2 \times 50\pi \times {\varepsilon _0}}}

(\because ω\omega = 2π\pif)

=2×10325×4πε0= {{2 \times {{10}^{ - 3}}} \over {25 \times 4\pi {\varepsilon _0}}}
XC=2×10325×9×109\Rightarrow {X_C} = {{2 \times {{10}^{ - 3}}} \over {25}} \times 9 \times {10^9}
XC=1825×106Ω\Rightarrow {X_C} = {{18} \over {25}} \times {10^6}\,\Omega

By using Ohm's law, As,

I0=V0XC=20×2518×106=27.78×106{I_0} = {{{V_0}} \over {{X_C}}} = {{20 \times 25} \over {18}} \times {10^{ - 6}} = 27.78 \times {10^{ - 6}}

\Rightarrow I0 = 27.78μ\muA \therefore The amplitude of the oscillating displacement current for applied AC voltage will be approximately 27.79 μ\muA.

Q89
For an RLC circuit driven with voltage of amplitude vm and frequency ω0{\omega _0} = 1LC{1 \over {\sqrt {LC} }} the current exhibits resonance. The quality factor, Q is given by :
A CRω0{{CR} \over {{\omega _0}}}
B ω0LR{{{\omega _0}L} \over R}
C ω0RL{{{\omega _0}R} \over L}
D R(ω0C){R \over {\left( {{\omega _0}C} \right)}}
Correct Answer
Option B
Solution

Quality factor (Q) =

AngularResonanceBandwith{{Angular\,\,{\mathop{\rm Re}\nolimits} sonance} \over {Bandwith}}

=

1LCRL{{{1 \over {\sqrt {LC} }}} \over {{R \over L}}}

=

ω0RL{{{\omega _0}} \over {{R \over L}}}

=

ω0LR{{{\omega _0}L} \over R}
Q90
A series L.R circuit connected with an ac source E=(25sin1000t)VE=(25 \sin 1000 t) V has a power factor of 12\dfrac{1}{\sqrt{2}}. If the source of emf is changed to E=(20sin2000t)V\mathrm{E}=(20 \sin 2000 \mathrm{t}) \mathrm{V}, the new power factor of the circuit will be :
A 13\dfrac{1}{\sqrt{3}}
B 12\dfrac{1}{\sqrt{2}}
C 15\dfrac{1}{\sqrt{5}}
D 17\dfrac{1}{\sqrt{7}}
Correct Answer
Option C
Solution
E=25sin(1000t)cosθ=12\begin{aligned} & E=25 \sin (1000 t) \\\\ & \cos \theta=\frac{1}{\sqrt{2}} \end{aligned}

LR circuit

 Initially Rω1L=1tanθ=1tan45=1XL=ω1Lω2=2ω1, given tanθ=ω2LR=2ω1LRtanθ=2cosθ=15\begin{aligned} & \text{ Initially } \frac{R}{\omega_1 L}=\frac{1}{\tan \theta}=\frac{1}{\tan 45^{\circ}}=1 \\\\ & X_L=\omega_1 L \\\\ & \omega_2=2 \omega_1, \text{ given } \\\\ & \tan \theta^{\prime}=\frac{\omega_2 L}{R}=\frac{2 \omega_1 L}{R} \\\\ & \tan \theta^{\prime}=2 \\\\ & \cos \theta^{\prime}=\frac{1}{\sqrt{5}} \end{aligned}
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