The Young's Double Slit Experiment (YDSE) is a beautiful demonstration of the wave nature of light. Usually, we rely on the small-angle approximation where the path difference is simply dsinθ. However, this problem throws a curveball! The point P is directly in front of one of the slits, and the screen is relatively close. This means we must abandon our approximations and rely on pure, unadulterated geometry.
Analyzing the Setup
Let's visualize the physical reality of the setup. We have two coherent slits, S1 and S2, separated by a distance d. The screen is placed at a distance D=2d from the plane of the slits.
The point of interest, P, lies exactly opposite to the upper slit S1. We are given a crucial piece of information: the first minimum of the interference pattern forms exactly at this point P.
The Master Equation
What does it mean for a minimum to form? It means the light waves from S1 and S2 arrive at P completely out of phase, destructively interfering with each other.
The general condition for the
n-th minimum is that the path difference
Δx must be an odd multiple of half the wavelength:
Δx=(2n−1)2λ
Since we are dealing with the
first minimum, we set
n=1. This simplifies our master equation to:
Δx=2λ
The Geometry of Path Lengths
To find the path difference, we need the exact distances the light travels from each slit to point P.
First, consider the ray from
S1. Because
P is directly in front of
S1, the light travels in a straight horizontal line. The length of this path is simply the distance to the screen:
S1P=2d
Next, consider the ray from S2. This ray must travel diagonally to reach P. If we look closely, the slits S1, S2, and the point P form a perfect right-angled triangle. The distance between the slits is the vertical leg (d), and the distance to the screen is the horizontal leg (2d).
Using the Pythagorean theorem, the hypotenuse
S2P is:
Final Calculation
Now we have both path lengths. The path difference
Δx is the difference between the longer path and the shorter path:
Δx=S2P−S1P
We can factor out
d to make it cleaner:
We know from our master equation that this path difference must equal
2λ for the first minimum to occur. Equating the two expressions:
Finally, isolating the slit separation
d, we get our elegant final answer:
This perfectly matches option (c). By trusting the geometry rather than blindly applying standard formulas, we navigated the trap and arrived at the correct solution!