Step 1: Picture the roll-bite triangle directly.
Draw the roll of radius $R$ meeting the plate at the entry point. The plate surface drops by half the draft, $\Delta h/2$, over the arc of contact, because the reduction is shared equally above and below the rolling centerline. This drop, the roll radius, and the bite angle $\alpha$ form a right triangle relation at the entry point: the horizontal leg is the chord along the roll surface and the vertical leg is the drop $\Delta h/2$, measured from the roll center.
Step 2: Recall the roll-bite result and check it makes physical sense.
Working through that triangle geometry with a small-angle approximation leads to the standard rolling-mechanics result: the rolls can just grip the plate, with no slipping, when
\[
\mu_{min}=\sqrt{\frac{\Delta h}{R}}
\]
where $\Delta h$ is the draft and $R$ is the roll radius. Before using it, check the limits: if $\Delta h \to R$ (an extremely aggressive, physically unrealistic single pass), $\mu_{min}\to1$, which sits right at the practical upper bound for dry metal-on-metal friction. If $\Delta h \to 0$ (almost no reduction), $\mu_{min}\to0$, which also makes sense since a very light pass needs almost no grip to pull the plate through. The formula behaves sensibly at both ends, so it is safe to use here.
Step 3: Get the draft and the roll radius from the data.
The plate thins from $50$ mm to $25$ mm, so the draft is
\[
\Delta h=50-25=25\text{ mm}
\]
The roll diameter is $1250$ mm, so the radius is half of that,
\[
R=\frac{1250}{2}=625\text{ mm}
\]
Both $\Delta h$ and $R$ are in millimeters, so their ratio is a pure number and no unit conversion is needed before taking the square root.
Step 4: Form the ratio.
\[
\frac{\Delta h}{R}=\frac{25}{625}=0.04
\]
Step 5: Take the square root.
\[
\mu_{min}=\sqrt{0.04}
\]
Since $0.2\times0.2=0.04$, the square root is exactly $0.2$.
Step 6: Conclude.
Rounded to two decimal places, $\mu_{min}=0.20$, which sits inside the accepted range of 0.19 to 0.21. A coefficient of friction of about $0.2$ is a realistic, achievable value for a dry aluminium-on-steel roll contact, which is a good practical sanity check on the answer.
\[
\boxed{\mu_{min}=0.20}
\]