To solve the problem, we need to determine where an object should be placed on the optic axis such that a real and inverted image is formed at the same location by a thin convex lens with one surface silvered. We will employ the lens-maker's formula and mirror formula in conjunction. The lens functions both as a lens and a mirror, forming a catadioptric system.
- Begin with the lens-maker's formula for a thin lens:
\(\frac{1}{f} = \left(\frac{\mu_2}{\mu_1} - 1\right)\left(\frac{1}{|R_1|} - \frac{1}{|R_2|}\right)\) - Determine the focal length of the lens before silvering, \(f'\):
\( \frac{1}{f'} = \left(\frac{\mu_2 - \mu_1}{\mu_1}\right)\left(\frac{1}{|R_1|} - \frac{1}{|R_2|}\right) \) - Once the second surface is silvered, the setup functions as a lens-mirror system. The effective focal length \(F\) of the system is:
\(\frac{1}{F} = \frac{2}{f'} + \frac{1}{r}\)
where \(r = -|R_2|\) due to the mirror's curvature. - Substitute the value of \(f'\):
\(\frac{1}{F} = \frac{2 \mu_1}{(\mu_2 - \mu_1)} \left(\frac{1}{|R_1|} - \frac{1}{|R_2|}\right) - \frac{1}{|R_2|}\) - Simplify to find the effective focal length:
\(\frac{1}{F} = \frac{\mu_1 \left(2|R_2| - |R_1|\right)}{|R_1| |R_2| (\mu_2 - \mu_1)}\) - For the formation of a real and inverted image at the object location (autoconjugate point), the object distance \(u\) should be equal to the effective focal length in magnitude. Therefore, \(u = F\).
- Simplifying using the effective focal length formula, the object distance is:
\(u = \frac{\mu_1 |R_1| |R_2|}{\mu_2 (|R_1| + |R_2|) - \mu_1 |R_2|}\)
This is the correct expression for the object distance for the condition specified. Thus, the object should be placed at this distance for a real and inverted image to form at the same location.