A narrow tube is bent in the form of a circle of radius
as shown Two small holes
are made in the tube at positions right angle to each other. A source placed at
generated a wave of intensity
which is equally divided into two parts. One part travels along the longer path while the other travels along the shorter path. Both the waves meet the point
where a detector is placed.
If maxima is found at the detector then, the magnitude of wavelength cannot be
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For a maxima at D , path difference Δ x = n λ
2 3 π R − 2 π R = n λ
⇒ λ = n π R
λ = π R , 2 π R , 3 π R , 4 π R , e t c .