Electromagnetic Induction

JEE Physics · 59 questions · Page 6 of 6 · Click an option or "Show Solution" to reveal answer

Q51

Match with \cdot \overrightarrow{d l}=\mu_o i_c+\mu_o \varepsilon_o \frac{d \phi_E}{d t}$$

List - IList - II
(B) Edl=dϕBdt\oint \vec{E} \cdot \overrightarrow{d l}=\dfrac{d \phi_B}{d t} (I) Gauss' law for electricity
(C) EdA=Qεo\oint \vec{E} \cdot \overrightarrow{d A}=\dfrac{Q}{\varepsilon_o} (II) Gauss' law for magnetism
(D) BdA=0\oint \vec{B} \cdot \overrightarrow{d A}=0 (III) Faraday law
() (IV) Ampere - Maxwell law
A A-IV, B-III, C-I, D-II
B A-I, B-II, C-III, D-IV
C A-IV, B-I, C-III, D-II
D A-II, B-III, C-I, D-IV
Correct Answer
Option A
Solution

Ampere-Maxwell law

Bdl=μ0ic+μ0ε0dϕEdt\rightarrow \oint \overrightarrow{\mathrm{B}} \cdot \overrightarrow{\mathrm{dl}}=\mu_0 \mathrm{i}_{\mathrm{c}}+\mu_0 \varepsilon_0 \frac{\mathrm{d} \phi_{\mathrm{E}}}{\mathrm{dt}}

Faraday law

Edl=dϕBdt\rightarrow \oint \vec{E} \cdot \overrightarrow{d l}=\frac{d \phi_{\mathrm{B}}}{d t}

Gauss' law for electricity

EdA=Qε0\rightarrow \oint \overrightarrow{\mathrm{E}} \cdot \overrightarrow{\mathrm{dA}}=\frac{\mathrm{Q}}{\varepsilon_0}

Gauss ' law for magnetism

BdA=0\rightarrow \oint \vec{B} \cdot \overrightarrow{d A}=0
Q52
A coil having nn turns and resistance RΩR\Omega is connected with a galvanometer of resistance 4RΩ.4R\Omega . This combination is moved in time tt seconds from a magnetic field W1{W_1} weber to W2{W_2} weber. The induced current in the circuit is
A (W2W1)Rnt{{\left( {{W_2} - {W_1}} \right)} \over {Rnt}}
B n(W2W1)5Rt - {{n\left( {{W_2} - {W_1}} \right)} \over {5\,\,Rt}}
C (W2W1)5Rnt - {{\left( {{W_2} - {W_1}} \right)} \over {5\,\,Rnt}}
D n(W2W1)Rt - {{n\left( {{W_2} - {W_1}} \right)} \over {Rt}}
Correct Answer
Option B
Solution
ΔϕΔt=(W2W1)t{{\Delta \phi } \over {\Delta t}} = {{\left( {{W_2} - {W_1}} \right)} \over t}
Rtot=(R+4R)Ω=5RΩ{R_{tot}} = \left( {R + 4R} \right)\Omega = 5R\Omega
i=ndϕRtotdt=n(W2W1)5Rti = {{nd\phi } \over {{R_{tot}}dt}} = {{ - n\left( {{W_2} - {W_1}} \right)} \over {5Rt}}

( as

W2&W1{W_2}\,\,\& \,\,{W_1}

are magnetic flux )

Q53
12 V12 \mathrm{~V} battery connected to a coil of resistance 6Ω6 \Omega through a switch, drives a constant current in the circuit. The switch is opened in 1 ms1 \mathrm{~ms}. The emf induced across the coil is 20 V20 \mathrm{~V}. The inductance of the coil is :
A 5 mH5 ~ \mathrm{mH}
B 8 mH8 ~\mathrm{mH}
C 10 mH10~ \mathrm{mH}
D 12 mH12 ~\mathrm{mH}
Correct Answer
Option C
Solution

When the switch is closed, the circuit is a simple DC circuit and the current in the circuit is given by Ohm's law: I=VR=12V6Ω=2AI = \dfrac{V}{R} = \dfrac{12\text{V}}{6\Omega} = 2\text{A}.

When the switch is opened, the current in the circuit drops to zero instantaneously.

However, the magnetic field generated by the current in the coil does not disappear immediately, and it continues to produce a back EMF that opposes the change in current.

This back EMF induces a voltage across the coil that can be calculated using Faraday's law of induction: E=LΔIΔt\mathcal{E} = -L\dfrac{\Delta I}{\Delta t}, where E\mathcal{E} is the induced voltage, LL is the inductance of the coil, and ΔI/Δt\Delta I/\Delta t is the rate of change of current in the coil.

In this case, we know that the induced voltage is 20V20\text{V} and the rate of change of current is ΔI/Δt=2A/(1ms)=2×103A/s\Delta I/\Delta t = -2\text{A}/(1\text{ms}) = -2\times 10^3\text{A/s}.

Substituting these values into the equation above, we get: 20V=L×(2×103A/s)20\text{V} = -L\times(-2\times 10^3\text{A/s}).

Solving for LL, we get: L=20V2×103A/s=0.01HL = \dfrac{20\text{V}}{2\times 10^3\text{A/s}} = 0.01\text{H}.

Therefore, the inductance of the coil is 0.01H0.01\text{H}, or 10 mH.

Q54
Consider a circular coil of wire carrying constant current I, forming a magnetic dipole. The magnetic flux through an infinite plane that contains the circular coil and excluding the circular coil area is given by ϕ\phi i. The magnetic flux through the area of the circular coil area is given by ϕ\phi 0. Which of the following option is correct?
A ϕ\phi i = ϕ\phi 0
B ϕ\phi i < ϕ\phi 0
C ϕ\phi i >> ϕ\phi 0
D ϕ\phi i = - ϕ\phi 0
Correct Answer
Option D
Solution

As, magnetic field lines forms a closed loop, hence each line from circular area will pass through outer area in opposite direction hence ϕ\phii = - ϕ\phi0.

Q55
When the current changes from +2A + 2A to 2A-2A in 0.050.05 second, an e.m.f.e.m.f. of 88 VV is inducted in a coil. The coefficient of self- induction of the coil is
A 0.2H0.2H
B 0.4H0.4H
C 0.80.8 HH
D 0.10.1 HH
Correct Answer
Option D
Solution
e=ΔϕΔt=Δ(LI)Δt=LΔIΔte = - {{\Delta \phi } \over {\Delta t}} = {{ - \Delta \left( {LI} \right)} \over {\Delta t}} = - L{{\Delta I} \over {\Delta t}}

\therefore

e=LΔIΔt8=L×40.05\left| e \right| = L{{\Delta I} \over {\Delta t}} \Rightarrow 8 = L \times {4 \over {0.05}}
L=8×0.054=0.1H\Rightarrow L = {{8 \times 0.05} \over 4} = 0.1H
Q56
A coil is places perpendicular to a magnetic field of 5000 T5000 \mathrm{~T}. When the field is changed to 3000 T3000 \mathrm{~T} in 2 s2 \mathrm{~s}, an induced emf of 22 V22 \mathrm{~V} is produced in the coil. If the diameter of the coil is 0.02 m0.02 \mathrm{~m}, then the number of turns in the coil is:
A 35
B 70
C 7
D 140
Correct Answer
Option B
Solution
ε=N(Δϕt)Δϕ=(ΔB)ABi=5000 T, Bf=3000 T d=0.02 mr=0.01 mΔϕ=(ΔB)A=(2000)π(0.01)2=0.2πε=N(Δϕt)22=N(0.2π2)N=70\begin{aligned} \varepsilon & =\mathrm{N}\left(\frac{\Delta \phi}{\mathrm{t}}\right) \\ \Delta \phi & =(\Delta \mathrm{B}) \mathrm{A} \\ \mathrm{B}_{\mathrm{i}} & =5000 \mathrm{~T}, \\ \mathrm{~B}_{\mathrm{f}} & =3000 \mathrm{~T} \\ \mathrm{~d} & =0.02 \mathrm{~m} \\ \mathrm{r} & =0.01 \mathrm{~m} \\ \Delta \phi & =(\Delta \mathrm{B}) \mathrm{A} \\ & =(2000) \pi(0.01)^2=0.2 \pi \\ \varepsilon & =\mathrm{N}\left(\frac{\Delta \phi}{\mathrm{t}}\right) \Rightarrow 22=\mathrm{N}\left(\frac{0.2 \pi}{2}\right) \\ \mathrm{N} & =70 \end{aligned}
Q57
A transformer has an efficiency of 80%80 \% and works at 10 V10 \mathrm{~V} and 4 kW4 \mathrm{~kW}. If the secondary voltage is 240 V240 \mathrm{~V}, then the current in the secondary coil is :
A 1.33 A1.33 \mathrm{~A}
B 13.33 A13.33 \mathrm{~A}
C 1.59 A1.59 \mathrm{~A}
D 15.1 A15.1 \mathrm{~A}
Correct Answer
Option B
Solution

To find the current in the secondary coil of the transformer, we first need to calculate the output power, taking into account the efficiency.

The efficiency (η\eta) of the transformer is given by the ratio of the output power (

PoutP_{\text{out}}

) to the input power (

PinP_{\text{in}}

) times 100%. The given efficiency is

η=80%\eta = 80\%

or

η=0.8\eta = 0.8

in decimal form. The input power is also given as

Pin=4kWP_{\text{in}} = 4 \text{kW}

or

Pin=4000WP_{\text{in}} = 4000 \text{W}

. Let's calculate

PoutP_{\text{out}}

using the efficiency formula:

Pout=η×Pin=0.8×4000W=3200WP_{\text{out}} = \eta \times P_{\text{in}} = 0.8 \times 4000 \text{W} = 3200 \text{W}

Now that we have

PoutP_{\text{out}}

, we can calculate the secondary current (

IsecondaryI_{\text{secondary}}

) using the formula:

Pout=Vsecondary×IsecondaryP_{\text{out}} = V_{\text{secondary}} \times I_{\text{secondary}}

We are given

Vsecondary=240VV_{\text{secondary}} = 240 \text{V}

. Isolating

IsecondaryI_{\text{secondary}}

gives us:

Isecondary=PoutVsecondaryI_{\text{secondary}} = \frac{P_{\text{out}}}{V_{\text{secondary}}}

Substituting the known values:

Isecondary=3200W240VI_{\text{secondary}} = \frac{3200 \text{W}}{240 \text{V}}
Isecondary=3200240I_{\text{secondary}} = \frac{3200}{240}
Isecondary=13.33AI_{\text{secondary}} = 13.33 \text{A}

Therefore, the current in the secondary coil is

13.33A13.33 \text{A}

, which corresponds to Option B.

Q58
A 10 m long horizontal wire extends from North East to South West. It is falling with a speed of 5.0 ms–1, at right angles to the horizontal component of the earth's magnetic field of 0.3 × \times 10–4 Wb/m2. The value of the induced emf in wire is :
A 0.3 × \times 10–3 V
B 2.5 × \times 10–3 V
C 1.5 × \times 10–3 V
D 1.1 × \times 10–3 V
Correct Answer
Option D
Solution

Induied emf = Bv

\ell

sin 45o = 0.3 ×\times 10-4 ×\times 5 ×\times 10 ×\times sin 45o = 1.1 ×\times 10-3 V

Q59
Two coaxial solenoids are made by winding thin insulated wire over a pipe of cross-sectional area A=A= 10cm210\,\,c{m^2} and length =20=20 cmcm . If one of the solenoid has 300300 turns and the other 400400 turns, their mutual inductance is (μ0=4π×107TmA1)\left( {{\mu _0} = 4\pi \times {{10}^{ - 7}}\,Tm\,{A^{ - 1}}} \right)
A 2.4π×105H2.4\pi \times {10^{ - 5}}H
B 4.8π×104H4.8\pi \times {10^{ - 4}}H
C 4.8π×105H4.8\pi \times {10^{ - 5}}H
D 2.4π×104H2.4\pi \times {10^{ - 4}}H
Correct Answer
Option D
Solution
M=μ0N1N2AM = {{{\mu _0}{N_1}{N_2}A} \over \ell }
=4π×107×300×400×100×1040.2= {{4\pi \times {{10}^{ - 7}} \times 300 \times 400 \times 100 \times {{10}^{ - 4}}} \over {0.2}}
=2.4π×104H= 2.4\pi \times {10^{ - 4}}H
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