Step 1: Beer–Lambert law: \(I_o = I_i e^{-\mu L}\), where \(\mu\) is the absorption coefficient and \(L\) is the path length through the absorber. Hence
\[
\log\!\left(\frac{I_i}{I_o}\right)=\mu L .
\]
Step 2: Here \(\mu = 1\ \text{cm}^{-1}\), so \(\log(I_i/I_o) = L\). The ray passes through the disc along a chord whose distance from the center is \(t\). The chord length is
\[
L = 2\sqrt{R^2 - t^2}.
\]
Step 3: Therefore,
\[
\log\!\left(\frac{I_i}{I_o}\right)=2\sqrt{R^2 - t^2}.
\]