
The induced electromotive force (EMF) in a conductor in motion is calculated as: \[ E = B \frac{dA}{dt} \] The area \(A\) contained within the rails at time \(t\) is expressed as: \[ A = \frac{1}{2} l^2 \] Given that the length \(l\) of the moving bar is directly proportional to time \(t\), it can be represented as: \[ l = vt \] Consequently, the area becomes: \[ A = \frac{1}{2} (vt)^2 = \frac{1}{2} v^2 t^2 \] Differentiating \(A\) with respect to \(t\) yields: \[ \frac{dA}{dt} = v^2 t \] Therefore, the induced EMF is: \[ E = B v^2 t \] When this is compared to the expression \( E \propto t^n \), it is determined that \( n = 2 \).