JEE Challenger
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Jump Heights of Rings on Solenoids and Resistivity Relation

Two metallic rings A and B, identical in shape and size but having different resistivities ρA\rho_A and ρB\rho_B, are kept on top of two identical solenoids as shown in the figure. When current II is switched on in both the solenoids in identical manner, the rings A and B jump to heights hAh_A and hBh_B, respectively, with hA>hBh_A > h_B. The possible relation(s) between their resistivities and their masses mAm_A and mBm_B is(are)

Diagram 0

Options

A

ρA>ρB\rho_A > \rho_B and mA=mBm_A = m_B

B

ρA<ρB\rho_A < \rho_B and mA=mBm_A = m_B

Correct
C

ρA>ρB\rho_A > \rho_B and mA>mBm_A > m_B

D

ρA<ρB\rho_A < \rho_B and mA<mBm_A < m_B

Correct

Step-by-Step Solution

To find the relation between the resistivities and masses of the two rings, we analyze the electromagnetic force and motion of the rings when the current is switched on.

  1. Induced EMF and Resistance:
    Since both rings AA and BB are identical in shape and size and are placed symmetrically on identical solenoids, the rate of change of magnetic flux through each ring is the same during the switching-on of current:
    E=−dΦdt\mathcal{E} = -\frac{d\Phi}{dt}

    The electrical resistance of a ring is given by:
    R=ρlAcR = \rho \frac{l}{A_c}
    where ρ\rho is the resistivity, ll is the perimeter, and AcA_c is the cross-sectional area of the ring. Since ll and AcA_c are identical for both rings:
    R∝ρR \propto \rho

  2. Induced Current and Repulsive Force:
    The induced current ii in the ring is:
    i=ER∝1ρi = \frac{\mathcal{E}}{R} \propto \frac{1}{\rho}

    The upward electromagnetic force exerted on the ring due to the diverging magnetic field at the end of the solenoid is given by:
    Fmag=iBr(2πr)∝i∝1ρF_{\text{mag}} = i B_r (2\pi r) \propto i \propto \frac{1}{\rho}
    where BrB_r is the radial component of the magnetic field and rr is the radius of the ring.

  3. Motion and Jump Height:
    The current rises rapidly over a very short time interval Δt\Delta t, imparting an upward impulse JJ to the ring:
    J=∫Fmag dt∝1ρJ = \int F_{\text{mag}} \, dt \propto \frac{1}{\rho}

    The initial velocity vv acquired by the ring immediately after the impulse is:
    v=Jm∝1mρv = \frac{J}{m} \propto \frac{1}{m\rho}

    Neglecting air resistance, the maximum height hh attained by the ring is:
    h=v22g∝1m2ρ2h = \frac{v^2}{2g} \propto \frac{1}{m^2 \rho^2}

    Therefore, the jump height hh is inversely dependent on both the mass mm and the resistivity ρ\rho of the ring. A ring will jump higher if it has smaller resistivity and/or smaller mass.

  4. Evaluating the Given Conditions:
    We are given that:
    hA>hBh_A > h_B

    • Case 1: If mA=mBm_A = m_B, then for hA>hBh_A > h_B, ring AA must experience a greater upward force, which requires:
      ρA<ρB\rho_A < \rho_B
      This matches option (B).

    • Case 2: If ρA<ρB\rho_A < \rho_B and mA<mBm_A < m_B, both the lower resistivity and the smaller mass contribute to giving ring AA a larger acceleration and initial velocity, definitively ensuring:
      hA>hBh_A > h_B
      This matches option (D).

    • Options (A) and (C): Both state ρA>ρB\rho_A > \rho_B with mA≥mBm_A \ge m_B, which would result in hA<hBh_A < h_B, contradicting the given condition.

Hence, the possible relations are (B) and (D).