Let $f_a$ be the focal length of the convex lens in air and $f_l$ be the focal length of the convex lens in liquid.
Let $n_g$ be the refractive index of the lens material, $n_a$ be the refractive index of air, and $n_l$ be the refractive index of the liquid.
Let $R_1$ and $R_2$ be the radii of curvature of the lens surfaces.
The lens maker's formula for a lens in air is given by:
$$\frac{1}{f_a} = \left(\frac{n_g}{n_a} - 1\right) \left(\frac{1}{R_1} - \frac{1}{R_2}\right)$$
The lens maker's formula for a lens in liquid is given by:
$$\frac{1}{f_l} = \left(\frac{n_g}{n_l} - 1\right) \left(\frac{1}{R_1} - \frac{1}{R_2}\right)$$
We are given that $n_g = 1.52$, $n_a = 1$, and $n_l = 1.65$.
Dividing the second equation by the first equation, we get:
$$\frac{f_l}{f_a} = \frac{\frac{n_g}{n_a} - 1}{\frac{n_g}{n_l} - 1} = \frac{\frac{1.52}{1} - 1}{\frac{1.52}{1.65} - 1} = \frac{1.52 - 1}{\frac{1.52 - 1.65}{1.65}} = \frac{0.52}{\frac{-0.13}{1.65}} = \frac{0.52 \times 1.65}{-0.13} = \frac{0.858}{-0.13} = -6.6$$
Thus, $f_l = -6.6 f_a$.
Given that $f_a = 15$ cm, we have:
$f_l = -6.6 \times 15 = -99$ cm.
Since $f_l$ is negative, the convex lens in the liquid behaves as a diverging lens, or a concave lens.
Final Answer: The final answer is $\boxed{-99cm}$