Analyzing the Setup
Imagine an optical bench setup where an object and a screen are fixed at a certain distance apart. This distance is given as D=100 cm. When we move a convex lens between the object and the screen, we discover a fascinating phenomenon: there are exactly two distinct positions of the lens where a sharp, real image is formed on the screen.
The distance between these two specific lens positions is denoted as d, and in our case, d=40 cm. This entire scenario is a classic application of the Displacement Method, a highly reliable experimental technique used to determine the focal length of a convex lens.
The Master Equation
For the displacement method, the relationship between the focal length f, the distance between the object and screen D, and the displacement of the lens d is given by a direct and elegant formula:
Let's carefully substitute the values we have into this master equation. We plug in D=100 and d=40:
Executing the Calculation
Now, we perform the arithmetic. It is crucial to avoid silly mistakes here. Squaring the terms gives us:
Subtracting the numerator values:
Dividing 8400 by 400, we find the focal length of the convex lens:
The Power Trap
The question doesn't stop at the focal length; it asks for the optical power of the lens. The formula for power is P=f1. However, there is a massive trap here: to calculate power in Diopters (D), the focal length must be in meters.
Let's convert our focal length:
Now, we substitute this into the power formula:
To simplify, we remove the decimal by multiplying the numerator and denominator by 100:
If we evaluate this fraction, it comes out to approximately 4.76 D.
Final Comparison
The problem states that the power of the lens is close to (100N) D. We can rewrite our calculated decimal power in a similar fractional format:
By comparing our result with the given expression 100N, it becomes immediately clear that:
This is our final integer answer. Always remember the critical condition for the displacement method: a real image on the screen is only possible if the distance D is greater than or equal to 4f. If D<4f, no such lens positions will exist!