For a lens with two spherical surfaces, the focal length \( f \) is related to the radii of curvature \( R_1 \) and \( R_2 \) of the surfaces by the lens maker’s formula:
\[
\frac{1}{f} = \left( \mu - 1 \right) \left( \frac{1}{R_1} - \frac{1}{R_2} \right)
\]
where:
- \( \mu \) is the refractive index of the material of the lens,
- \( R_1 \) is the radius of curvature of the first surface,
- \( R_2 \) is the radius of curvature of the second surface.
For a biconvex lens, both surfaces have the same radius of curvature, \( R_1 = +R \) and \( R_2 = -R \). Substituting these values into the lens maker’s formula:
\[
\frac{1}{f} = \left( \mu - 1 \right) \left( \frac{1}{R} - \frac{1}{-R} \right)
\]
\[
\frac{1}{f} = \left( \mu - 1 \right) \left( \frac{2}{R} \right)
\]
\[
f = \frac{R}{2(\mu - 1)}
\]
Now, to find the condition under which the focal length \( f \) is equal to \( R \), set \( f = R \):
\[
R = \frac{R}{2(\mu - 1)}
\]
Solving for \( \mu \):
\[
2(\mu - 1) = 1
\]
\[
\mu - 1 = \frac{1}{2}
\]
\[
\mu = \frac{3}{2}
\]
Thus, for the focal length to be equal to the radius of curvature, the refractive index of the material must be \( \mu = \frac{3}{2} \).
Next, when one of the surfaces of the biconvex lens is made plane, the radius of curvature of that surface becomes infinite, i.e., \( R_2 = \infty \). Using the lens maker’s formula again with \( R_1 = +R \) and \( R_2 = \infty \):
\[
\frac{1}{f} = \left( \mu - 1 \right) \left( \frac{1}{R} - \frac{1}{\infty} \right)
\]
\[
\frac{1}{f} = \left( \mu - 1 \right) \frac{1}{R}
\]
\[
f = \frac{R}{\mu - 1}
\]
Substitute \( \mu = \frac{3}{2} \) into this equation:
\[
f = \frac{R}{\frac{3}{2} - 1}
\]
\[
f = \frac{R}{\frac{1}{2}} = 2R
\]
Thus, when one surface is made plane, the new focal length of the lens will be \( 2R \).