For an equiconvex lens, the relation for focal length is given by:
\(\frac{1}{A} = \left(\frac{3}{2} - 1 \right) \left( \frac{1}{R} - \frac{1}{-R} \right)\)
Simplifying this equation:
\(\frac{1}{f} = \frac{1}{2} \times \frac{2}{R}\)
\(R = f\)
For the second lens, we have:
\(\frac{1}{f_2} = \left(\frac{4}{3} - 1\right) \left( \frac{1}{-f} - \frac{1}{-f} \right)\)
Simplifying the equation:
\(\frac{1}{f_2} = \frac{1}{3} \times \frac{2}{-f}\)
\(f_2 = \frac{-3f}{2}\)
The formula for the combination of focal lengths is:
\(\frac{1}{f'} = \frac{1}{f_1} + \frac{1}{f_2} + \frac{1}{f_3}\)
Substituting the values for \( f_1 \), \( f_2 \), and \( f_3 \):
\(\frac{1}{f'} = \frac{1}{f} + \frac{2}{-3f} + \frac{1}{f}\)
Simplifying:
\(\frac{1}{f'} = \frac{3 - 2 + 3}{3f} = \frac{4}{3f}\)
\(f' = \frac{3f}{4}\)
The effective focal length of the combination of these lenses is \( f' = \frac{3f}{4} \), where \( f \) is the focal length of the first lens.
AB is a part of an electrical circuit (see figure). The potential difference \(V_A - V_B\), at the instant when current \(i = 2\) A and is increasing at a rate of 1 amp/second is:
Lenses that are made by combining two spherical transparent surfaces are called spherical lenses. In general, there are two kinds of spherical lenses. Lenses that are made by joining two spherical surfaces that bulge outward are convex lenses, whereas lenses that are made by joining two spherical surfaces that curve inward are concave lenses.