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Figure 35-40 shows two isotropic point sources of light (S1and S2) that emit in phase at wavelength 400 nm and at the same amplitude. A detection point P is shown on an x-axis that extends through source S1. The phase difference ϕbetween the light arriving at point P from the two sources is to be measured as P is moved along the x axis from x=0 out to x=+∞.The results out to xs=10×10-7m are given in Fig. 35-41. On the way out to +∞ , what is the greatest value of x at which the light arriving at from S1is exactly out of phase with the light arriving at P from S2?

Short Answer

Expert verified

The maximum value of x for which the light arriving from sources S1 and S2 to point out of phase is 3500nm.

Step by step solution

01

Identification of given data

The phase difference of fringe pattern varies with the path difference. For minimum phase difference path difference should be minimum and vice versa.

The separation is xs=10×10-7m.

The wavelength of the light is λ=400nmλ=400nmλ=400nm.

02

Determination of greatest value of x for which the light arriving to point P from both sources is out of phase

The path difference between positions x=0 and x is given as:

Δx=d2+x2-x

Here, d is the separation between sources S1and S2. Its value from the figure 35-40 is 3λ.

The phase difference is given as:

ϕ0-ϕs=2πλΔx

Here, ϕ0and ϕs are the phase angle for positions x=0and x=xs, which are 6πand 5πfrom the given graph in figure 35-41.

Substitute all the values in equation.

6π-5π=2πλd2+x2-x3λ2+x2-x=λ29λ2+x2=x+λ229λ2+x2=λ24+2λ2x+x2

λx=9λ2-λ24λx=9λ2-λ24

λx=9λ2-λ24

x=35λ4=35400nm4=3500nm

Therefore, the maximum value of x for which the light arriving from sources S1 and S2to point out of phase is 3500nm.

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Most popular questions from this chapter

In Fig. 35-4, assume that two waves of light in air, of wavelength 400nm, are initially in phase. One travels through a glass layer of index of refraction n1=1.60and thickness L. The other travels through an equally thick plastic layer of index of refraction n2=1.50. (a) What is the smallest value Lshould have if the waves are to end up with a phase difference of 5.65 rad? (b) If the waves arrive at some common point with the same amplitude, is their interference fully constructive, fully destructive, intermediate but closer to fully constructive, or intermediate but closer to fully destructive?

Transmission through thin layers. In Fig. 35-43, light is incident perpendicularly on a thin layer of material 2 that lies between (thicker) materials 1 and 3. (The rays are tilted only for clarity.) Part of the light ends up in material 3 as rayr3(the light does not reflect inside material 2) andr4(the light reflects twice inside material 2). The waves ofr3and r4interfere, and here we consider the type of interference to be either maximum (max) or minimum (min). For this situation, each problem in Table 35-3 refers to the indexes of refraction n1,n2and n3the type of interference, the thin-layer thickness Lin nanometers, and the wavelength λin nanometers of the light as measured in air. Whereλis missing, give the wavelength that is in the visible range. Where Lis missing, give the second least thickness or the third least thickness as indicated.

A thin film of acetone n=1.25coats a thick glass platen=1.50White light is incident normal to the film. In the reflections, fully destructive interference occurs at 600nmand fully constructive interference at700nm. Calculate the thickness of the acetone film.

Figure 35-26 shows two rays of light, of wavelength 600nm, that reflectfrom glass surfaces separated by 150nm. The rays are initially in phase.

(a) What is the path length difference of the rays?

(b) When they have cleared the reflection region, are the rays exactly in phase, exactly out of phase, or in some intermediate state?

Suppose that the two waves in Fig. 35-4 have a wavelength λ=500nmin air. What multiple of λgives their phase difference when they emerge if (a) n1=1.50, n2=16and L=8.50μm; (b) n1=1.62, n2=1.72, and L=8.50μm; and (c) n1=1.59, n2=1.79, and L=3.25μm? (d) Suppose that in each of these three situations, the waves arrive at a common point (with the same amplitude) after emerging. Rank the situations according to the brightness the waves produce at the common point.

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