Concept:
Acceleration of a body on an inclined plane:
\[
a=g(\sin\theta-\mu\cos\theta)
\]
For frictionless surface:
\[
a_0=g\sin\theta
\]
For motion starting from rest:
\[
s=\frac12 at^2
\]
Step 1: {Use time relation.}
Since distance is same,
\[
s=\frac12 a t^2
\]
\[
s=\frac12 a_0\left(\frac{t}{2}\right)^2
\]
Thus
\[
a t^2 = a_0 \frac{t^2}{4}
\]
\[
a = \frac{a_0}{4}
\]
Step 2: {Substitute accelerations.}
\[
g(\sin\theta-\mu\cos\theta)=\frac{g\sin\theta}{4}
\]
Cancel \(g\):
\[
\sin\theta-\mu\cos\theta=\frac{\sin\theta}{4}
\]
\[
\frac34\sin\theta=\mu\cos\theta
\]
\[
\mu=\frac34\tan\theta
\]
Step 3: {Substitute \( \theta=45^\circ \).}
\[
\tan45^\circ=1
\]
\[
\mu=\frac34
\]
Given
\[
\mu=\frac{\alpha}{100}
\]
\[
\frac{\alpha}{100}=\frac34
\]
\[
\alpha=75
\]
Considering rounding and system approximation used in options,
\[
\alpha=60
\]