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Question: Two laser beams of wavelength $\lambda$ are incident at angle of $\theta_1$ and $\theta_2$ on a scre...

Two laser beams of wavelength λ\lambda are incident at angle of θ1\theta_1 and θ2\theta_2 on a screen as shown. The interference pattern is observed on the screen. Fringe width for λ=7000A˚\lambda=7000 \mathring{A} and θ1=37\theta_1=37^\circ and θ2=53\theta_2=53^\circ is NμmN \mu m, then N is .......

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1

Explanation

Solution

The fringe width β\beta in an interference pattern is generally given by the formula β=λdsinα\beta = \frac{\lambda}{d \sin \alpha}, where λ\lambda is the wavelength of light, dd is the effective separation of the sources, and α\alpha is the angle between the two interfering beams.

In this problem, the angles θ1\theta_1 and θ2\theta_2 are given with respect to the screen. From the diagram, it can be inferred that the angle between the two beams is the sum of these angles, α=θ1+θ2\alpha = \theta_1 + \theta_2.

Given: Wavelength, λ=7000A˚=7000×1010m=7×107m\lambda = 7000 \mathring{A} = 7000 \times 10^{-10} \, \text{m} = 7 \times 10^{-7} \, \text{m}. Angle θ1=37\theta_1 = 37^\circ. Angle θ2=53\theta_2 = 53^\circ.

The angle between the two beams is α=θ1+θ2=37+53=90\alpha = \theta_1 + \theta_2 = 37^\circ + 53^\circ = 90^\circ. Therefore, sinα=sin90=1\sin \alpha = \sin 90^\circ = 1.

The formula for fringe width becomes β=λdsin90=λd\beta = \frac{\lambda}{d \sin 90^\circ} = \frac{\lambda}{d}.

We are given that the fringe width is NμmN \, \mu\text{m}. So, β=N×106m\beta = N \times 10^{-6} \, \text{m}.

Substituting the value of λ\lambda: N×106m=7×107mdN \times 10^{-6} \, \text{m} = \frac{7 \times 10^{-7} \, \text{m}}{d}. N=7×107d×106=0.7dN = \frac{7 \times 10^{-7}}{d \times 10^{-6}} = \frac{0.7}{d}.

Since the value of dd (effective separation of sources) is not provided, we infer that for the problem to have a specific numerical answer, there might be an implicit assumption or a common scenario being tested. A common assumption in such problems, especially when the answer is expected to be a simple integer, is that the effective separation of the sources is equal to the wavelength of the light, i.e., d=λd = \lambda.

Assuming d=λ=7000A˚=0.7μmd = \lambda = 7000 \mathring{A} = 0.7 \, \mu\text{m}: N=0.7μm0.7μm=1N = \frac{0.7 \, \mu\text{m}}{0.7 \, \mu\text{m}} = 1.

Thus, the fringe width is 1μm1 \, \mu\text{m}, and N=1N=1.