The induced EMF in a moving conductor is given by:
\[
E = B \frac{dA}{dt}
\]
The area enclosed by the rails at any time \( t \) is:
\[
A = \frac{1}{2} l^2
\]
Since the length of the moving bar is proportional to time \( t \), we assume:
\[
l = vt
\]
Then:
\[
A = \frac{1}{2} (vt)^2 = \frac{1}{2} v^2 t^2
\]
Differentiating with respect to \( t \):
\[
\frac{dA}{dt} = v^2 t
\]
Thus, the induced EMF is:
\[
E = B v^2 t
\]
Comparing with \( E \propto t^n \), we get \( n = 2 \).