\(f\)
\(2f\)
\(\frac f2\)
\(\frac f4\)
To determine the new focal length when a convex lens is cut into two equal parts, we need to consider the effect of dividing the lens on its optical properties. The focal length \( f \) of a lens is given by the lens maker's formula:
\( \frac{1}{f} = (\mu-1)\left(\frac{1}{R_1} - \frac{1}{R_2}\right) \)
where \( \mu \) is the refractive index and \( R_1, R_2 \) are the radii of curvature of the lens surfaces. However, when we physically cut a convex lens (which is initially symmetrical and thin) into two equal halves, the curvature and refractive index remain unchanged, but the aperture area is reduced.
For the new lens piece, the lens maintains its curvature properties but the diameter (or the aperture of the lens) is halved. This effectively changes the lens's ability to converge rays. A larger aperture allows better convergence due to less diffraction at the edges. Dividing the lens reduces the aperture, influencing the effective focal length of each piece.
For a lens cut along the principal axis, you essentially have a lens with half the aperture area, which increases the converging power given by:
\( \text{New focal length} = \frac{f}{2} \)
This is because the portioned lens should act equivalently to the original smaller, complete lens with half the aperture area: focusing light to the same point but needing adjustment numerically due to geometry and optics context.
Therefore, the focal length of each half of the original lens is \(\frac{f}{2}\).
When light travels from an optically denser medium to an optically rarer medium, at the interface it is partly reflected back into the same medium and partly refracted to the second medium. The angle of incidence corresponding to an angle of refraction 90° is called the critical angle (ic) for the given pair of media. This angle is related to the refractive index of medium 1 with respect to medium 2. Refraction of light through a prism involves refraction at two plane interfaces. A relation for the refractive index of the material of the prism can be obtained in terms of the refracting angle of the prism and the angle of minimum deviation. For a thin prism, this relation reduces to a simple equation. Laws of refraction are also valid for refraction of light at a spherical interface. When an object is placed in front of a spherical surface separating two media, its image is formed. A relation between object and image distance, in terms of refractive indices of two media and the radius of curvature of the spherical surface can be obtained. Using this relation for two surfaces of lens, ’lensemaker formula’ is obtained.
