The Setup
A Steady Flow
Imagine a straight conducting wire. Initially, a constant current I is flowing through it from left to right due to an external source of electromotive force.
Everything is in a steady state, and a constant magnetic field surrounds the wire.
The Disruption
Switching Off
Now, what happens when we suddenly switch off the source? The current doesn't just vanish into thin air. It starts to decrease rapidly towards zero.
This is where the magic of electromagnetism kicks in. According to Lenz's Law, nature abhors a change in magnetic flux. The decreasing current causes a decreasing magnetic field, which in turn induces an electromotive force ε in the wire.
The Resistance
Lenz's Law in Action
The induced electromotive force is given by the equation ε=−LdtdI, where L is the self-inductance of the wire.
Because the current is decreasing, dtdI is negative, making the induced emf positive. This means the induced emf will try to push a current in the same direction as the original current to oppose the decrease.
Therefore, the induced current will flow from left to right, desperately trying to keep the original current alive.
The Catch
The Role of Inductance
But wait, there is a subtle catch here! This entire phenomenon relies on the presence of self-inductance L.
If we consider a perfectly ideal straight wire with absolutely zero self-inductance (L=0), then the induced emf ε will be exactly zero, regardless of how fast the current changes.
In such an idealized scenario, there would be no induced current at all.
The Final Verdict
Taking both practical and ideal scenarios into account, the induced current will either flow from left to right (if there is some inductance) or it will be zero (if the inductance is perfectly zero).
This dual possibility perfectly captures the essence of the problem!