
Answer:

\[ n = \frac{d_{ac}}{d_{ap}}\]
where $n$ is the index of refraction. (You can derive this with Snell's law and some geometric ideas.) Now, we recall the thin lens equation.
\[ \frac{1}{d_o}+\frac{1}{d_i}=\frac{1}{f} \]
where $d_o$, $d_i$, and $f$ are the object distance, the image distance, and the focal length. From the second figure, the object distance is $b+d_{ap}$. The apparent distance is $d_{ap}=d_{ac}/n$, so we have
\[ d_{ap} = \frac{30}{n} \]
You can plug in the thin lens equation and solve for $n$.
\begin{eqnarray*}
\frac{1}{b+\frac{30}{n}}&+&\frac{1}{d_i}=\frac{1}{f} \\
\frac{1}{b+\frac{30}{n}}&=&\frac{1}{f}-\frac{1}{d_i} \\
\frac{1}{b+\frac{30}{n}}&=&\frac{d_i-f}{d_if} \\
b+\frac{30}{n}&=&\frac{d_if}{d_i-f} \\
\frac{30}{n}&=&\frac{d_if}{d_i-f} - b \\
\frac{n}{30}&=&\frac{1}{\frac{d_if}{d_i-f} - b} \\
n&=&\frac{30}{\frac{d_if}{d_i-f} - b}
\end{eqnarray*}
Therefore, we obtain
\[ n= 1.5\]
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