In an interference arrangement similar to Young's double slit experiment, the slits S₁ and S₂ are illuminated with coherent microwave sources each of frequency 10⁶ Hz. The sources are synchronized to have zero phase difference. The slits are separated by distance d = 150 m. The intensity I(θ)is measured as a function of q, where q is defined as shown. If I₀ is maximum intensity, then I(θ) for 0≤θ≤90° is given by

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Q. In an interference arrangement similar to Young's double-slit experiment, the slits

S_{1}

and

S_{2}

are illuminated with coherent microwave sources, each of frequency

10^{6} H z

. The sources are synchronized to have zero phase difference. The slits are separated by a distance. The slits are separated by a distance

d = 150.0 m

. The intensity

I (θ)

is measured as a function of

θ

, where

θ

is defined as shown in figure. If

I_{0}

is the maximum intensity, then

I (θ)

for

0 \leq θ \leq 90^{o}

is given by :

In an interference arrangement similar to Young's double slit experiment, the slits S₁ and S₂ are illuminated with coherent microwave sources each of frequency 10⁶ Hz. The sources are synchronized to have zero phase difference. The slits are separated by distance d = 150 m. The intensity I(θ)is measured as a function of q, where q is defined as shown. If I₀ is maximum intensity, then I(θ) for 0≤θ≤90° is given by