Magnetic Dipoles and Galvanometers: questions with solutions
3 free questions from this chapter (the full set has 30). Marking: Multi-correct: +4 all correct, +1 per correct option if none wrong, −2 if any wrong · Numerical: +4 / 0 · Matching: +3 / −1.
Question 1Level 2 · ExamSingle correct
A thin insulated wire of length L carries a steady current I. In arrangement 1 the whole wire is bent into a single-turn square loop. In arrangement 2 the same whole wire is wound into a flat, closely wound circular coil of exactly two turns, both turns having the same radius. In each case the leads are twisted together and contribute nothing. The ratio m1/m2 of the magnitudes of the magnetic moments in arrangements 1 and 2 is ______. Exactly one option is correct.
A4π
Bπ2
C2π
Dπ
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Answer: C
Square: side L/4, so m1=I16L2.
Two-turn coil: each turn has circumference L/2, so radius r=4πL and m2=2Iπr2=8πIL2.
m2m1=L2/(8π)L2/16=2π.
General result: a wire of length L wound into n circular turns has m=4πnIL2, so adding turns of a fixed wire reduces m.
Difficulty: Hard
Question 2Level 3 · AdvancedSingle correct
Use right-handed axes x,y,z. A closed loop of thin wire runs along six edges of a cube of edge a that has one corner at the origin O and its edges along the positive axes. The wire goes, in order, O(0,0,0)→(a,0,0)→(a,a,0)→(a,a,a)→(0,a,a)→(0,0,a)→O, and carries a steady current I in that sense. The loop is placed in a uniform magnetic field B=B0y^. The torque on the loop is ______. Exactly one option is correct.
AIa2B0(−x^+z^)
BIa2B0(x^−z^)
CIa2B0(x^+z^)
D3Ia2B0x^
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Answer: A
For any closed loop (planar or not) in a uniform field, the net force is zero and the torque is τ=m×B with m=IA, where the vector area is A=21∮r×dl. For a polygon with vertices r1,…,rn: A=21∑ri×ri+1.
Non-zero terms: (a,0,0)×(a,a,0)=a2z^; (a,a,0)×(a,a,a)=a2(x^−y^); (a,a,a)×(0,a,a)=a2(−y^+z^); (0,a,a)×(0,0,a)=a2x^.
Sum =a2(2,−2,2), so A=a2(x^−y^+z^). (Check: adding the internal edges from (0,a,0) splits the loop into three square loops on the faces z=0, y=a and x=0; their vector areas are a2z^, −a2y^ and a2x^.)
τ=Ia2(x^−y^+z^)×B0y^=Ia2B0(x^×y^+z^×y^)=Ia2B0(z^−x^).
So τ=Ia2B0(−x^+z^), magnitude 2Ia2B0. (Confirmed by summing r×(Idl×B) over the six edges numerically.)
Difficulty: Peak challenge
Question 3Level 3 · AdvancedSingle correct
A thin non-conducting disc of radius R and mass M has its mass distributed uniformly over its area. A total charge Q is spread over the disc with surface charge density proportional to the distance r from the centre (σ=kr, k constant). The disc rotates with constant angular speed ω about its own axis (perpendicular to the disc through its centre). The ratio of the magnitude of its magnetic moment to the magnitude of its angular momentum is ______. Exactly one option is correct.
A2MQ
B5M3Q
C3M2Q
D4M3Q
Show answer and solution
Answer: B
Ring between r and r+dr: charge dq=kr⋅2πrdr, current dI=dq2πω=kωr2dr, moment dm=πr2dI=πkωr4dr.
m=5πkωR5 and Q=∫0R2πkr2dr=32πkR3, so m=103QωR2.
Angular momentum (uniform mass): L=21MR2ω.
Lm=MR2ω/23QωR2/10=5M3Q.
The ratio exceeds Q/(2M) because the charge sits farther out than the mass.
Difficulty: Very hard
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