Step 1: The effective focal length of the lens combination is given by:
\[ \frac{1}{F} = \frac{1}{f_1} + \frac{1}{f_2} \]
Step 2: Since \( f_1>f_2 \) and \( f_2 \) is negative for a diverging lens:
\[ \frac{1}{F} = \frac{1}{f_1} - \frac{1}{|f_2|} \]
Step 3: If \( f_1 \) dominates, the net effect is converging.
\( \text{Combination acts as a converging lens.} \)
(ii) Condition: \( f_1<f_2 \)
Solution:
Step 1: Using the same formula:
\[ \frac{1}{F} = \frac{1}{f_1} + \frac{1}{f_2} \]
Step 2: If \( f_1<f_2 \), the negative focal length of the diverging lens dominates.
\[ \frac{1}{F}<0 \]
Step 3: The net effect is a diverging lens.
\( \text{Combination acts as a diverging lens.} \)
(iii) Condition: \( f_1 = f_2 \)
Solution:
Step 1: Using the lens formula:
\[ \frac{1}{F} = \frac{1}{f_1} + \frac{1}{f_2} \]
Step 2: If \( f_1 \) and \( f_2 \) are equal in magnitude but opposite in sign:
\[ \frac{1}{F} = 0 \Rightarrow F = \infty \]
Step 3: The combination acts as a plane parallel glass.
\( \text{Combination acts as a plane glass.} \)
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