Analyzing the Setup
Imagine you are standing in a lab, setting up a Young's Double Slit Experiment. But instead of the usual setup, you place the screen perpendicular to the line joining the two sources! Let's break down what happens in this unique geometry.
The two coherent sources, S1 and S2, are located on the y-axis. The screen is placed parallel to the x-z plane at a distance D=3 m. The origin O is exactly where the y-axis pierces the screen.
The Master Equation
Path Difference at the Origin
To understand the interference pattern, we must first look at the center of our screen, point O. What is the path difference between the light waves reaching this point?
Since O lies directly on the line passing through S1 and S2, the wave from S1 has to travel an extra distance exactly equal to the separation between the sources, d, compared to the wave from S2.
Therefore, the path difference at the origin is simply ΔxO=d.
Final Calculation
Bright or Dark?
Now, let's plug in the numbers. We are given d=0.6003 mm, which is 600300 nm. The wavelength of the light is λ=600 nm.
Let's find how many wavelengths fit into this path difference:
λΔxO=600600300=1000.5
This means the path difference is exactly 1000.5λ, or (1000+21)λ. Because it is an odd multiple of half the wavelength, the waves arrive perfectly out of phase. This results in destructive interference, making the region very close to point O completely dark!
The Geometry of the Fringes
Finally, what is the shape of the fringes on the screen? In 3D space, the locus of points that have a constant path difference from two fixed points is a hyperboloid.
When we intersect this hyperboloid with a flat screen that is perpendicular to the axis of the sources, the cross-sections are perfect circles. However, our screen only exists for z>0. Therefore, we will observe semi-circular bright and dark bands centered at O.