A thin equiconvex lens of glass (μ=32) having a focal length of 30 cm in air is placed at a distance of 10 cm from a plane mirror, which, in turn is placed with its plane perpendicular to the optic axis of the lens. Water (μ=43) fills the space between lens and mirror. A parallel beam of light is incident on the lens parallel to the principal axis. Choose the correct option(s):
Final image is 18 cm right to the lens.
If mirror is rotated by 1∘, as shown in figure, final image is displaced by \(\frac{\pi}{3}~cm\).
The focal length of the glass lens is 30 cm
1f(μ−1)(1R1−1R2)=2(μ−1)R
The radius of curvature, R = 30 cm.
The object distance, u=∞.
Now we apply Gauss’s law at surface S1 and S2.
32v1−1u=32−130……(1)43v−32v1=−16−30……(2)⇒v=60 cm
After reflection from the mirror, the light rays appear to converge to a point 40 cm to the right of the convex lens. This serves as virtual object for the lens: u = +40cm
32v1−43+40=16301v−32v1=−12−30
⇒v=18cm to the right of convex lens.
If the mirror is rotated by 1∘ the reflected ray rotates by 2∘. The virtual object for the lens formed by the reflection from the mirror is displaced by:
Δy1=50×2π180 cm
The magnification due to the refraction at the two surfaces of the lens is
m=m1m2=(vμ3v1μ2)×(v1μ2uμ1)=(vμ3uμ1)=18140(43)=1830
The displacement of the final image is
1830×50×2π180 cm=π3 cm