We are given a thin convex lens with refractive index \( \mu_2 \), placed in a liquid with refractive index \( \mu_1 \), and the radii of curvature of the lens are \( |R_1| \) and \( |R_2| \). The second surface is silver-polished. We need to find the position of the object on the optic axis that will result in a real and inverted image being formed at the same place. To begin, we use the formula for the focal length of a lens: \[ \frac{1}{f_L} = \left( \frac{\mu_2 - \mu_1}{\mu_1} \right) \left( \frac{1}{R_1} + \frac{1}{R_2} \right) \] Now, for this system, the object distance \( u \) is related to the focal length. The lens equation gives us: \[ \frac{1}{f_L} = \frac{1}{u} + \frac{1}{v} \] Where \( u \) is the object distance and \( v \) is the image distance. In this case, the image is formed at the same location as the object, so the object distance is equal to the image distance, \( u = v \). Thus, the object should be placed at the following distance: \[ u = \frac{\mu_1 |R_1| |R_2|}{\mu_2 (|R_1| + |R_2|) - \mu_1 |R_2|} \] This matches option (2).