Analyzing the Setup
Imagine two identical solenoids, each with a metallic ring resting on top
Ring A and Ring B are identical in shape and size, but they have different resistivities (ρA and ρB) and possibly different masses (mA and mB). This classic setup is a beautiful demonstration of the interplay between electromagnetism and classical mechanics.
The Master Equation
Faraday's Law
When we switch on the current in the solenoids, a magnetic field suddenly builds up. According to Faraday's Law, this changing magnetic flux induces an electromotive force (EMF) in both rings.
Since the rings have the exact same dimensions and are placed in identical changing magnetic fields, the induced EMF e is identical for both. However, their resistivities are different. The induced current i is simply the EMF divided by the resistance R.
Since resistance is proportional to resistivity (R∝ρ), the current is inversely proportional to the resistivity (i∝ρ1).
The Magnetic Kick
By Lenz's Law, this induced current creates a magnetic field that opposes the solenoid's field, resulting in a sudden upward repulsive force
This force acts for a very short time, delivering an upward impulse J to the rings.
This impulse gives the rings an initial upward velocity v. Since impulse equals the change in momentum (J=mv), the velocity v is proportional to the current divided by the mass.
Flight and Final Calculation
Now, the rings shoot up into the air like projectiles
The maximum height h they reach is given by kinematics as v2/2g. Therefore, the height is inversely proportional to the square of mass times resistivity.
The problem states that ring A jumps higher than ring B (hA>hB). This means the product of mass and resistivity for A must be strictly less than that for B.
Looking at our options:
- If ρA<ρB and mA=mB, then mAρA<mBρB holds perfectly. (Option b)
- If ρA<ρB and mA<mB, then mAρA<mBρB holds again. (Option d)
Thus, options (b) and (d) are the correct answers.