Multiple Choice Questions (MCQs) for JEE Physics: Moving Charges and Magnetism
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Multiple Choice Questions
(a) \( \frac{\mu_0}{4\pi}\frac{qvR}{(R^2+x^2)^{3/2}} \)
(b) \( \frac{\mu_0}{4\pi}\frac{qv}{R^2+x^2} \)
(c) \( \frac{\mu_0}{4\pi}\frac{qv}{x^2} \)
(d) \( \frac{\mu_0}{4\pi}\frac{qv}{R^2} \)
Show Answer & Explanation
Answer: (b) \( \frac{\mu_0}{4\pi}\frac{qv}{R^2+x^2} \)
Explanation:
1. The distance from the charge to the point is \( r=\sqrt{R^2+x^2} \) and the velocity is perpendicular to the line joining them (velocity is tangential, the line has no tangential part).
2. So \( \sin\theta=1 \) and \( B=\frac{\mu_0}{4\pi}\frac{qv}{R^2+x^2} \).
3. The direction of this field keeps turning as the charge goes round, so the field is constant in magnitude only.
Teacher's Note:
1. Sketch the geometry and decide the direction of each contribution before putting in numbers.
2. Straight-wire formulas depend on the angles the ends subtend at the point.
(a) \( 5.0\times10^{-5} \) T, out of the plane
(b) \( 1.0\times10^{-4} \) T, into the plane
(c) \( 1.0\times10^{-4} \) T, out of the plane
(d) zero
Show Answer & Explanation
Answer: (c) \( 1.0\times10^{-4} \) T, out of the plane
Explanation:
1. The straight parts along the x-axis point at O along their own line, so they give no field at O.
2. Each vertical part is a semi-infinite wire starting at the foot of the perpendicular from O, at distance \( d=0.02 \) m: \( B=\frac{\mu_0 i}{4\pi d}=\frac{10^{-7}\times10}{0.02}=5\times10^{-5} \) T.
3. Right-hand rule: the downward current on the left and the upward current on the right both give a field out of the page at O, so they add: \( 1.0\times10^{-4} \) T out of the plane.
Teacher's Note:
1. Sketch the geometry and decide the direction of each contribution before putting in numbers.
2. Straight-wire formulas depend on the angles the ends subtend at the point.
(a) \( \mu_0 n i \)
(b) \( \frac12\mu_0 n i \)
(c) \( 2\mu_0 n i \)
(d) \( \frac{\mu_0 n i}{4} \)
Show Answer & Explanation
Answer: (b) \( \frac12\mu_0 n i \)
Explanation:
1. Use an Amperian rectangle of length l straddling the sheet, with two sides parallel to the sheet at equal distances on both sides; the field is parallel to the sheet and equal in magnitude on the two sides, opposite in sense.
2. Ampere's law: \( B\,l+B\,l=\mu_0 (n l) i \).
3. So \( B=\frac12\mu_0 n i \), independent of the distance.
Teacher's Note:
1. Sketch the geometry and decide the direction of each contribution before putting in numbers.
2. Straight-wire formulas depend on the angles the ends subtend at the point.
(a) \( \frac{K}{n} \)
(b) \( \frac{2K}{n} \)
(c) \( \frac{K}{4n} \)
(d) \( \frac{K}{2n} \)
Show Answer & Explanation
Answer: (d) \( \frac{K}{2n} \)
Explanation:
1. The sheet gives a uniform field \( \frac{\mu_0 K}{2} \) parallel to its plane, perpendicular to the current direction.
2. For the net field to vanish the solenoid field must cancel it: \( \mu_0 n i=\frac{\mu_0 K}{2} \).
3. So \( i=\frac{K}{2n} \).
Teacher's Note:
1. Sketch the geometry and decide the direction of each contribution before putting in numbers.
2. Straight-wire formulas depend on the angles the ends subtend at the point.
(a) \( \frac{\mu_0 K}{2} \), parallel to the sheets
(b) \( \mu_0 K \), parallel to the sheets
(c) zero
(d) \( 2\mu_0 K \), perpendicular to the sheets
Show Answer & Explanation
Answer: (b) \( \mu_0 K \), parallel to the sheets
Explanation:
1. Each large sheet gives a uniform field \( \frac{\mu_0K}{2} \) parallel to itself, with directions given by the right-hand rule.
2. Between the sheets the two fields point the same way (below the upper sheet and above the lower sheet), so they add: \( \mu_0K \).
3. Outside the pair the fields oppose and cancel.
Teacher's Note:
1. Sketch the geometry and decide the direction of each contribution before putting in numbers.
2. Straight-wire formulas depend on the angles the ends subtend at the point.
(a) 4 A
(b) 2.5 A
(c) 6 A
(d) 1.5 A
Show Answer & Explanation
Answer: (a) 4 A
Explanation:
1. Force \( F=evB \) gives \( B=\frac{3.2\times10^{-20}}{1.6\times10^{-19}\times4\times10^5}=5\times10^{-7} \) T.
2. Both fields at R have the same direction (same-direction currents, R on the same side of both): \( B=2\times10^{-7}\left(\frac{2.5}{5}+\frac{I}{2}\right) \).
3. Setting equal to \( 5\times10^{-7} \): \( 0.5+\frac I2=2.5 \), so \( I=4 \) A.
Teacher's Note:
1. Take the charge and mass ratio first; every circular-motion result follows from it.
2. Check the direction with the right-hand rule for the sign of the charge.
(a) \( \frac{\pi m}{2qB} \)
(b) \( \frac{\pi m}{qB} \)
(c) \( \frac{3\pi m}{2qB} \)
(d) \( \frac{2\pi m}{qB} \)
Show Answer & Explanation
Answer: (a) \( \frac{\pi m}{2qB} \)
Explanation:
1. Period of revolution \( T=\frac{2\pi m}{qB} \).
2. The arc is one quarter of a circle (\( 90^\circ \)), so \( t=\frac T4=\frac{\pi m}{2qB} \).
Teacher's Note:
1. Take the charge and mass ratio first; every circular-motion result follows from it.
2. Check the direction with the right-hand rule for the sign of the charge.
(a) \( 45^\circ \)
(b) \( 60^\circ \)
(c) \( 90^\circ \)
(d) \( 180^\circ \)
Show Answer & Explanation
Answer: (c) \( 90^\circ \)
Explanation:
1. Radius of the circle \( r=\frac{mv}{qB} \). On leaving the far edge the deviation \( \theta \) satisfies \( \sin\theta=\frac dr \).
2. With \( d\approx r \) (slightly smaller): \( \sin\theta\approx1 \), so \( \theta\approx90^\circ \).
Teacher's Note:
1. Take the charge and mass ratio first; every circular-motion result follows from it.
2. Check the direction with the right-hand rule for the sign of the charge.
(a) \( 30^\circ \)
(b) \( 60^\circ \)
(c) \( 90^\circ \)
(d) \( 45^\circ \)
Show Answer & Explanation
Answer: (d) \( 45^\circ \)
Explanation:
1. Radius \( r=\frac{mv}{qB} \), so \( \sin\theta=\frac dr=\frac1{\sqrt2} \).
2. Hence \( \theta=45^\circ \).
Teacher's Note:
1. Take the charge and mass ratio first; every circular-motion result follows from it.
2. Check the direction with the right-hand rule for the sign of the charge.
(a) \( \frac{q\mu_0 n i\, r}{m} \)
(b) \( \frac{q\mu_0 n i\, r}{2m} \)
(c) \( \frac{q\mu_0 n i\, r}{4m} \)
(d) \( \frac{2q\mu_0 n i\, r}{m} \)
Show Answer & Explanation
Answer: (b) \( \frac{q\mu_0 n i\, r}{2m} \)
Explanation:
1. Inside the solenoid \( B=\mu_0 n i \) along the axis; the particle moves on a circle that passes through its starting point on the axis.
2. The farthest it can get from the axis is the diameter \( 2\rho \) of that circle, so it just reaches the wall when \( 2\rho=r \).
3. With \( \rho=\frac{mv}{qB} \): \( v=\frac{qBr}{2m}=\frac{q\mu_0 n i r}{2m} \).
Teacher's Note:
1. Take the charge and mass ratio first; every circular-motion result follows from it.
2. Check the direction with the right-hand rule for the sign of the charge.
(a) \( 1.6\times10^{5} \) m/s
(b) \( 6.4\times10^{7} \) m/s
(c) \( 1.6\times10^{7} \) m/s
(d) \( 3.2\times10^{7} \) m/s
Show Answer & Explanation
Answer: (c) \( 1.6\times10^{7} \) m/s
Explanation:
1. No deflection means \( eE=evB \).
2. So \( v=\frac EB=\frac{3.2\times10^4}{2\times10^{-3}}=1.6\times10^7 \) m/s.
Teacher's Note:
1. Take the charge and mass ratio first; every circular-motion result follows from it.
2. Check the direction with the right-hand rule for the sign of the charge.
(a) \( \frac{B\,i}{n e} \)
(b) \( \frac{B\,i}{n\pi r^2 e} \)
(c) \( \frac{B\,i\,e}{n\pi r^2} \)
(d) \( \frac{i}{n\pi r^2 e B} \)
Show Answer & Explanation
Answer: (b) \( \frac{B\,i}{n\pi r^2 e} \)
Explanation:
1. Magnetic force on an electron \( e v_d B \) is balanced by the electric force \( eE \).
2. So \( E=v_dB=\frac{B\,i}{n\pi r^2 e} \).
Teacher's Note:
1. Take the charge and mass ratio first; every circular-motion result follows from it.
2. Check the direction with the right-hand rule for the sign of the charge.
(a) 0.5 T and 50000 V/m
(b) 0.05 T and 500 V/m
(c) 0.1 T and 10000 V/m
(d) 0.05 T and 5000 V/m
Show Answer & Explanation
Answer: (d) 0.05 T and 5000 V/m
Explanation:
1. Circle: \( B=\frac{mv}{qr}=\frac{1.6\times10^{-27}\times10^5}{1.6\times10^{-19}\times0.02}=0.05 \) T.
2. Undeflected: \( E=vB=10^5\times0.05=5000 \) V/m.
Teacher's Note:
1. Take the charge and mass ratio first; every circular-motion result follows from it.
2. Check the direction with the right-hand rule for the sign of the charge.
(a) \( \sqrt{\frac{2qE_0x}{m}} \)
(b) \( \sqrt{\frac{qE_0x}{m}} \)
(c) \( \frac{qE_0x}{mB_0} \)
(d) \( \sqrt{\frac{2qE_0x}{m}}\,\frac{E_0}{B_0} \)
Show Answer & Explanation
Answer: (a) \( \sqrt{\frac{2qE_0x}{m}} \)
Explanation:
1. The magnetic force does no work, so only the electric force changes the kinetic energy.
2. Work-energy theorem: \( \frac12mv^2=qE_0x \).
3. So \( v=\sqrt{\frac{2qE_0x}{m}} \).
Teacher's Note:
1. Take the charge and mass ratio first; every circular-motion result follows from it.
2. Check the direction with the right-hand rule for the sign of the charge.
(a) 0.08 N
(b) 0.06 N
(c) 0.1 N
(d) 0.6 N
Show Answer & Explanation
Answer: (b) 0.06 N
Explanation:
1. \( F=ilB\sin\theta=10\times0.10\times0.1\times0.6=0.06 \) N.
Teacher's Note:
1. Use F = i l B sin(theta) with l the effective straight length between the ends.
2. A closed loop in a uniform field has zero net force.
(a) \( \sqrt3\, i\ell B_0 \)
(b) \( \sqrt2\, i\ell B_0 \)
(c) \( i\ell B_0 \)
(d) \( 2\, i\ell B_0 \)
Show Answer & Explanation
Answer: (b) \( \sqrt2\, i\ell B_0 \)
Explanation:
1. \( \vec F=i\ell\,\hat j\times B_0(\hat i+\hat j+\hat k)=i\ell B_0(-\hat k+\hat i) \).
2. Magnitude \( i\ell B_0\sqrt{1+1}=\sqrt2\,i\ell B_0 \). (The component of B along the wire does not contribute.)
Teacher's Note:
1. Use F = i l B sin(theta) with l the effective straight length between the ends.
2. A closed loop in a uniform field has zero net force.
(a) \( iB\lambda \)
(b) \( \frac{iB\lambda}{4} \)
(c) \( 2\pi iBA \)
(d) \( \frac{iB\lambda}{2} \)
Show Answer & Explanation
Answer: (d) \( \frac{iB\lambda}{2} \)
Explanation:
1. For a curved wire in a uniform field \( \vec F=i\,\vec L\times\vec B \) with \( \vec L \) the vector joining the end points.
2. The end points are (0, 0) and \( (\frac\lambda2,0) \), so \( L=\frac\lambda2 \) and \( F=\frac{iB\lambda}{2} \).
Teacher's Note:
1. Use F = i l B sin(theta) with l the effective straight length between the ends.
2. A closed loop in a uniform field has zero net force.
(a) \( 2iB_0\ell \)
(b) \( iB_0\ell \)
(c) \( \frac{iB_0\ell}{2} \)
(d) zero
Show Answer & Explanation
Answer: (b) \( iB_0\ell \)
Explanation:
1. The forces on the two edges parallel to the x-axis are equal and opposite, since B is the same along each of them.
2. The two edges parallel to the y-axis at \( x_0 \) and \( x_0+\ell \) have forces \( i\ell B(x_0) \) and \( i\ell B(x_0+\ell) \) in opposite directions.
3. Net \( i\ell\,(B(x_0)-B(x_0+\ell))=i\ell B_0\frac{\ell}{\ell}=iB_0\ell \), independent of position.
Teacher's Note:
1. Use F = i l B sin(theta) with l the effective straight length between the ends.
2. A closed loop in a uniform field has zero net force.
(a) \( 4\times10^{-3} \) N/m
(b) \( 2\times10^{-3} \) N/m
(c) \( 6\times10^{-3} \) N/m
(d) \( 1.2\times10^{-2} \) N/m
Show Answer & Explanation
Answer: (c) \( 6\times10^{-3} \) N/m
Explanation:
1. Identical resistances share the current equally: 20 A in each wire.
2. Attraction by CD (2 cm): \( \frac{\mu_0 i^2}{2\pi(0.02)}=\frac{2\times10^{-7}\times400}{0.02}=4\times10^{-3} \) N/m; by EF (4 cm): \( 2\times10^{-3} \) N/m.
3. Both pull the same way, so the total is \( 6\times10^{-3} \) N/m towards the other wires.
Teacher's Note:
1. Use F = i l B sin(theta) with l the effective straight length between the ends.
2. A closed loop in a uniform field has zero net force.
(a) \( 2.8\times10^{-5} \) J/m
(b) \( 1.4\times10^{-5} \) J/m
(c) \( 5.5\times10^{-5} \) J/m
(d) \( 4.0\times10^{-4} \) J/m
Show Answer & Explanation
Answer: (a) \( 2.8\times10^{-5} \) J/m
Explanation:
1. Force per unit length \( f=\frac{\mu_0 i_1i_2}{2\pi r} \) (attraction).
2. Work \( =\int_{r_1}^{r_2}f\,dr=\frac{\mu_0i_1i_2}{2\pi}\ln\frac{r_2}{r_1}=2\times10^{-7}\times200\times\ln2 \).
3. This is \( 2.77\times10^{-5} \) J/m.
Teacher's Note:
1. Use F = i l B sin(theta) with l the effective straight length between the ends.
2. A closed loop in a uniform field has zero net force.
(a) \( \frac{mg}{\mu id} \)
(b) \( \frac{\mu mg}{id} \)
(c) \( \frac{\mu mg}{i\ell} \)
(d) \( \frac{\mu mg}{2id} \)
Show Answer & Explanation
Answer: (b) \( \frac{\mu mg}{id} \)
Explanation:
1. Only the length between the rails, d, carries current in the field, and it is perpendicular to a vertical field: force \( Bid \).
2. To start sliding this force must equal the limiting friction \( \mu mg \).
3. So \( B=\frac{\mu mg}{id} \).
Teacher's Note:
1. Use F = i l B sin(theta) with l the effective straight length between the ends.
2. A closed loop in a uniform field has zero net force.
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