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Light of wavelength 440 nm passes through a double slit, yielding a diffraction pattern whose graph of intensity I versus angular position is shown in Fig. 36-44. Calculate (a) the slit width and (b) the slit separation. (c) Verify the displayed intensities of the m=1and m=2 interference fringes.

Short Answer

Expert verified

(a) The slit width is5.0μm.

(b) The slit separation is 20.0μm.

(c) The values of intensities are verified.

Step by step solution

01

Concept/Significance of diffraction minima

The equation for diffraction minimum is given by,

asinθ=mλa=mλsinθ......(1)

Here,λis wavelength,θis angle of diffraction, and a is slit width.

The expression of intensity of diffraction pattern at any angle is given by,
I(θ)=Im(sinαα)......(2)

Here, Imis the maximum intensity, and α=πaλsinθ.

02

(a) Find the slit width

Substitute5.0° forθ ,440×10-9m forλ , and 1 form in equation (1).

a=1440×10-9msin5.0°≈5.0×10-6m=5.0μm

Therefore, the slit width is5.0μm .

03

(b) Find the slit separation

The number of spots is the ratio of dto a. Here, dis the slit separation.

From the given figure, the total number of spots is 9, and is given as follows.

da+1=9d=4a=45.0μm=20μm

Therefore, the slit separation is 20μm.

04

(c) Verify the values of intensities from graph

From the graph, the first interference maximum is occurred at1.25°.

Find the value ofαas follows.

α=π5.0×10-6msin1.25°440×10-9m=0.7787rad

Find the intensity at the second interference maximum.

I=7mW/cm2sin0.7787rad0.7787rad2=5.7mW/cm2

Thus, the intensity at m=1is5.7mW/cm2.

From the graph, the second interference maximum is occurred at 2.5°.

Find the value of αas follows.

α=π5.0×10-6msin2.5°440×10-9m=1.557rad

Find the intensity at the second interference maximum.

I=7mW/cm2sin1.557rad1.557rad2=2.9mW/cm2

Thus, the intensity atm=2 is2.9mW/cm2 .

Therefore, the values of intensities of interference fringes are agreed with the values given in the graph.

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Most popular questions from this chapter

Nuclear-pumped x-ray lasers are seen as a possible weapon to destroy ICBM booster rockets at ranges up to 2000 km. One limitation on such a device is the spreading of the beam due to diffraction, with resulting dilution of beam intensity. Consider such a laser operating at a wavelength of 1.40 nm. The element that emits light is the end of a wire with diameter 0.200 mm. (a) Calculate the diameter of the central beam at a target 2000 km away from the beam source. (b) What is the ratio of the beam intensity at the target to that at the end of the wire? (The laser is fired from space, so neglect any atmospheric absorption.)

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∆θ=∆λ(d/m)2-λ2

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