Step 1: Use the ratio of the two lens equations.
The geometrical factor \(\left(\frac{1}{R_1}-\frac{1}{R_2}\right)\) is common to the lens in air and in the liquid, so dividing the two lens maker equations eliminates it:
\[\frac{f_{med}}{f_{air}} = \frac{\left(\dfrac{n_g}{n_{air}} - 1\right)}{\left(\dfrac{n_g}{n_{med}} - 1\right)}\]
Step 2: Insert the refractive indices.
Glass in air: \(\frac{n_g}{n_{air}} - 1 = \frac{3}{2} - 1 = \frac{1}{2}\).
Glass in carbon disulphide: \(\frac{n_g}{n_{med}} - 1 = \frac{3/2}{5/3} - 1 = \frac{9}{10} - 1 = -\frac{1}{10}\).
Step 3: Form the ratio.
\[\frac{f_{med}}{f_{air}} = \frac{1/2}{-1/10} = \frac{1}{2}\times(-10) = -5\]
Step 4: Solve for the new focal length.
\[f_{med} = -5 \times f_{air} = -5 \times 15 = -75\ \text{cm}\]
Step 5: Nature of the lens.
The magnitude of the focal length increases from 15 cm to 75 cm and the sign turns negative. A negative focal length means the convex lens now diverges light, so in carbon disulphide it acts as a concave (diverging) lens, because the surrounding liquid is optically denser than the glass.
\[\boxed{f = -75\ \text{cm};\ \text{diverging (concave) behaviour}}\]