The induced electromotive force (EMF) in a conductor undergoing motion is expressed as:
\[
E = B \frac{dA}{dt}
\]
The area \( A \) enclosed by the conducting rails at time \( t \) is given by:
\[
A = \frac{1}{2} l^2
\]
Given that the length \( l \) of the moving bar is directly proportional to time \( t \), we establish the relationship:
\[
l = vt
\]
Substituting this into the area equation yields:
\[
A = \frac{1}{2} (vt)^2 = \frac{1}{2} v^2 t^2
\]
Differentiating the area \( A \) with respect to time \( t \) gives:
\[
\frac{dA}{dt} = v^2 t
\]
Consequently, the induced EMF \( E \) is determined to be:
\[
E = B v^2 t
\]
By comparing this result with the proportionality \( E \propto t^n \), we deduce that \( n = 2 \).