Magnetic Effect of Current

NEET Physics · 96 questions · Page 1 of 10 · Click an option or "Show Solution" to reveal answer

Q1
A 100-turn closely wound circular coil of radius 5 cm has a magnetic field of 3.14×103 T3.14 \times 10^{-3} \mathrm{~T} at its centre. The current flowing through the coil, and the magnitude of the magnetic moment of this coil are, respectively : (Take μ0=4π×107 T m/A\mu_0=4 \pi \times 10^{-7} \mathrm{~T} \mathrm{~m} / \mathrm{A} )
A 2 A,10 A m22 \mathrm{~A}, 10 \mathrm{~A} \mathrm{~m}^2
B 2.5 A,20 A m22.5 \mathrm{~A}, 20 \mathrm{~A} \mathrm{~m}^2
C 2 A,4 A m22 \mathrm{~A}, 4 \mathrm{~A} \mathrm{~m}^2
D 2.5 A,2 A m22.5 \mathrm{~A}, 2 \mathrm{~A} \mathrm{~m}^2
Correct Answer
Option D
Solution

Magnetic field of a circular loop:

B0=μ0Ni2Ri=2RB0μ0N=2×5×102×3.14×1034π×107×100i=2.5 A\begin{aligned} & B_0=\frac{\mu_0 N i}{2 R} \\ & i=\frac{2 R B_0}{\mu_0 N}=\frac{2 \times 5 \times 10^{-2} \times 3.14 \times 10^{-3}}{4 \pi \times 10^{-7} \times 100} \\ & i=2.5 \mathrm{~A} \end{aligned}

Magnetic moment

M=NiA=100×2.5×3.14×(5×102)2[A=πR2]=2 A m2\begin{aligned} & M=N i A \\ & =100 \times 2.5 \times 3.14 \times\left(5 \times 10^{-2}\right)^2\left[\because A=\pi R^2\right] \\ & =2 \mathrm{~A} \mathrm{~m}^2 \end{aligned}
Q2
A parallel plate capacitor made of circular plates is being charged such that the surface charge density on its plates is increasing at a constant rate with time. The magnetic field arising due to displacement current is:
A Non-zero everywhere with maximum at the imaginary cylindrical surface connecting peripheries of the plates
B Zero between the plates and non-zero outside
C Zero at all places
D Constant between the plates and zero outside the plates
Correct Answer
Option A
Solution

Let the surface charge density be σ=qA\sigma=\dfrac{q}{A} Given dσdt=\dfrac{d \sigma}{d t}= constant

ddt(qA)= constant lAi= constant \therefore \quad \frac{d}{d t}\left(\frac{q}{A}\right)=\text{ constant } \Rightarrow \frac{l}{A} i=\text{ constant }

It means displacement current is constant.

This system will act like a cylindrical wire.

The graph of magnetic field (B) vs rr is

Q3
A model for quantized motion of an electron in a uniform magnetic field BB states that the flux passing through the orbit of the electron in n(hle)n(h l e) where nn is an integer, hh is Planck's constant and ee is the magnitude of electron's charge. According to the model, the magnetic moment of an electron in its lowest energy state will be ( mm is the mass of the electron)
A heBπm\dfrac{h e B}{\pi m}
B heB2πm\dfrac{h e B}{2 \pi m}
C heπm\dfrac{h e}{\pi m}
D he2πm\dfrac{h e}{2 \pi m}
Correct Answer
Option D
Solution

To understand the quantized motion of an electron in a uniform magnetic field and determine its magnetic moment in the lowest energy state, consider the following derivations and equations: Magnetic Force and Centripetal Force: The magnetic force acting on the electron is counterbalanced by the centripetal force necessary for its circular motion: evB=mv2r e v B = \dfrac{m v^2}{r} Solving for the velocity v v : v=eBrm v = \dfrac{e B r}{m} Flux through the Electron's Orbit: The model states that the magnetic flux ϕ \phi through the orbit is linked to Planck’s constant h h as: Bπr2=nhe B \pi r^2 = \dfrac{n h}{e} Rearranging gives: Br2=nheπ B r^2 = \dfrac{n h}{e \pi} Magnetic Moment: The magnetic moment μ \mu is defined as the current I I times the area A A of the orbit: μ=IA=eTπr2 \mu = I A = \dfrac{e}{T} \pi r^2 Considering current due to orbital motion: μ=ev2πr×πr2=evr2 \mu = \dfrac{e v}{2 \pi r} \times \pi r^2 = \dfrac{e v r}{2} Substitute for v v from the earlier velocity equation: μ=12e(eBrm)r=12e2Br2m \mu = \dfrac{1}{2} e \left(\dfrac{e B r}{m}\right) r = \dfrac{1}{2} e^2 \dfrac{B r^2}{m} Using the flux condition Br2=nheπ B r^2 = \dfrac{n h}{e \pi} , we find: μ=12e2nheπm=neh2πm \mu = \dfrac{1}{2} e^2 \dfrac{n h}{e \pi m} = \dfrac{n e h}{2 \pi m} Lowest Energy State: For the lowest energy state, take n=1 n = 1 : μ=eh2πm \mu = \dfrac{e h}{2 \pi m} Thus, the magnetic moment of an electron in its lowest energy state is eh2πm\dfrac{e h}{2 \pi m}.

Q4
An electron (mass 9×1031 kg9 \times 10^{-31} \mathrm{~kg} and charge 1.6×1019C1.6 \times 10^{-19} \mathrm{C} ) moving with speed c/100(c=c / 100(c= speed of light) is injected into a magnetic field B\vec{B} of magnitude 9×104 T9 \times 10^{-4} \mathrm{~T} perpendicular to its direction of motion. We wish to apply an uniform electric field E\vec{E} together with the magnetic field so that the electron does not deflect from its path. Then (speed of light c=3c=3 ×103 ms1\times 10^3 \mathrm{~ms}^{-1})
A E\vec{E} is parallel to B\vec{B} and its magnitude is 27×102 V m127 \times 10^2 \mathrm{~V} \mathrm{~m}^{-1}
B E\vec{E} is parallel to B\vec{B} and its magnitude is 27×104 V m127 \times 10^4 \mathrm{~V} \mathrm{~m}^{-1}
C E\vec{E} is perpendicular to B\vec{B} and its magnitude is 27×104 V m127 \times 10^4 \mathrm{~V} \mathrm{~m}^{-1}
D E\vec{E} is perpendicular to B\vec{B} and its magnitude is 27×102 V m127 \times 10^2 \mathrm{~V} \mathrm{~m}^{-1}
Correct Answer
Option D
Solution

For no deflection of electron, FB=FE\vec{F}_B=\vec{F}_E

e(v×B)=eEE=v×BEBE=vB=c100×9×104=3×108100×9×104=27×102 V m1\begin{aligned} & -e(\vec{v} \times \vec{B})=-e \vec{E} \\ & \Rightarrow \vec{E}=\vec{v} \times \vec{B} \Rightarrow \vec{E} \perp \vec{B} \\ & E=v B=\frac{c}{100} \times 9 \times 10^{-4} \\ & =\frac{3 \times 10^8}{100} \times 9 \times 10^{-4} \\ & =27 \times 10^2 \mathrm{~V} \mathrm{~m}^{-1} \end{aligned}
Q5
A 2 amp current is flowing through two different small circular copper coils having radii ratio 1:21: 2. The ratio of their respective magnetic moments will be
A 2:12: 1
B 4:14: 1
C 1:41: 4
D 1:21: 2
Correct Answer
Option C
Solution

The magnetic moment of a current-carrying circular loop is given by the formula M=I×A M = I \times A , where I I is the current and A A is the area of the loop.

Assuming the current (I I ) is the same for both coils, the magnetic moment is directly proportional to the area of the coil (MA M \propto A ).

For two coils with radii r1 r_1 and r2 r_2 , the areas are A1=πr12 A_1 = \pi r_1^2 and A2=πr22 A_2 = \pi r_2^2 .

Given that the ratio of the radii is 1:2 1:2 , we can write: M1M2=A1A2=πr12πr22=(12)2=14 \dfrac{M_1}{M_2} = \dfrac{A_1}{A_2} = \dfrac{\pi r_1^2}{\pi r_2^2} = \left(\dfrac{1}{2}\right)^2 = \dfrac{1}{4} Thus, the ratio of their respective magnetic moments is 1:4 1:4 .

Q6
A tightly wound 100 turns coil of radius 10 cm10 \mathrm{~cm} carries a current of 7 A7 \mathrm{~A}. The magnitude of the magnetic field at the centre of the coil is (Take permeability of free space as 4π×107SI4 \pi \times 10^{-7} \mathrm{SI} units):
A 44 mT
B 4.4 T
C 4.4 mT
D 44 T
Correct Answer
Option C
Solution

The magnitude of magnetic field due to circular coil of N turns is given by

BC=μ0iN2R=4π×107×7×1002×0.1=4.4×103 T=4.4 mT\begin{aligned} & B_C=\frac{\mu_0 i N}{2 R} \\ & =\frac{4 \pi \times 10^{-7} \times 7 \times 100}{2 \times 0.1} \\ & =4.4 \times 10^{-3} \mathrm{~T} \\ & =4.4 \mathrm{~mT} \end{aligned}
Q7
A parallel plate capacitor is charged by connecting it to a battery through a resistor. If II is the current in the circuit, then in the gap between the plates:
A There is no current
B Displacement current of magnitude equal to II flows in the same direction as II
C Displacement current of magnitude equal to II flows in a direction opposite to that of II
D Displacement current of magnitude greater than II flows but can be in any direction
Correct Answer
Option B
Solution

According to modified Ampere's law

BdI=μ0(IC+ID)\oint B \cdot d I=\mu_0\left(I_C+I_D\right)

For Loop

L1IC0L_1 \quad I_C \neq 0

and

ID=0I_D=0

For Loop

L2IC=0L_2 \quad I_C=0

and

ID0I_D \neq 0

Due to

KCLIC=ID\mathrm{KCL} \quad I_C=I_D
Q8
A long straight wire of length 2 m2 \mathrm{~m} and mass 250 g250 \mathrm{~g} is suspended horizontally in a uniform horizontal magnetic field of 0.7 T0.7 \mathrm{~T}. The amount of current flowing through the wire will be (g=9.8 ms2)\left(\mathrm{g}=9.8 \mathrm{~ms}^{-2}\right) :
A 2.45 A
B 2.25 A
C 2.75 A
D 1.75 A
Correct Answer
Option D
Solution
mg=iB250×103×9.8=i×2×0.7i=0.250×9.82×0.7=0.250×7i=1.75 A\begin{aligned} & \mathrm{m g=i \ell B} \\\\ & 250 \times 10^{-3} \times 9.8=\mathrm{i} \times 2 \times 0.7 \\\\ & \mathrm{i}=\frac{0.250 \times 9.8}{2 \times 0.7}=0.250 \times 7 \\\\ & \mathrm{i}=1.75 \mathrm{~A} \end{aligned}
Q9
A uniform electric field and a uniform magnetic field are acting along the same direction in a certain region. If an electron is projected in the region such that its velocity is pointed along the direction of fields, then the electron:
A will turn towards right of direction of motion
B will turn towards left of direction of motion
C speed will decrease
D speed will increase
Correct Answer
Option C
Solution

Speed of electron will decrease due to electric force magnetic force of electron is zero.

Q10
A wire carrying a current II along the positive x\mathrm{x}-axis has length LL. It is kept in a magnetic field B=(2i^+3j^4k^)T\overrightarrow{\mathrm{B}}=(2 \hat{\mathrm{i}}+3 \hat{\mathrm{j}}-4 \hat{\mathrm{k}}) \mathrm{T}. The magnitude of the magnetic force acting on the wire is :
A 5 IL\sqrt{5} \mathrm{~IL}
B 5 IL5 \mathrm{~IL}
C 3\sqrt{3} IL
D 3 IL
Correct Answer
Option B
Solution
F=I(×B)\vec{F}=I(\vec{\ell} \times \vec{B})
=I[(Li^)×(2i^+3j^4k^)]=I(4Lj^+3Lk^)\begin{aligned} & =I[(L \hat{i}) \times(2 \hat{i}+3 \hat{j}-4 \hat{k})] \\\\ & =I(4 L \hat{j}+3 L \hat{k}) \end{aligned}
F=5 IL |\vec{F}|=5 \text{ IL }
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