Step 1: Understand rolling motion energy.
For a rolling solid disc:
\[
K = \frac{1}{2}mv^2 + \frac{1}{2}I\omega^2
\]
For solid disc:
\[
I = \frac{1}{2}mr^2, \quad v = \omega r
\]
Step 2: Substitute rotational energy.
\[
K = \frac{1}{2}mv^2 + \frac{1}{2} \cdot \frac{1}{2}mr^2 \cdot \frac{v^2}{r^2}
\]
\[
K = \frac{1}{2}mv^2 + \frac{1}{4}mv^2
\]
\[
K = \frac{3}{4}mv^2
\]
Step 3: Substitute values.
\[
K = \frac{3}{4} \times 100 \times (0.2)^2
\]
\[
K = \frac{3}{4} \times 100 \times 0.04
\]
\[
K = \frac{3}{4} \times 4
\]
\[
K = 3 \, \text{J}
\]
Step 4: Work done to stop the disc.
Work required = initial kinetic energy:
\[
W = 3 \, \text{J}
\]
Step 5: Final conclusion.
Thus, absolute work done to stop the rolling disc is:
\[
\boxed{3 \, \text{J}}
\]