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The two point sources in Fig 35-61 emit coherent waves. Show that all curves (such as the one shown), over which the phase difference for rays r1and r2in a constant, are hyperbolas. (Hint: A constant phase difference implies a constant difference in length between r1and r2).

Short Answer

Expert verified

All curves are hyperbola.

Step by step solution

01

The given data:

Two rays are r1and r2.

02

Formula of distance between two points:

The distance between two points is the length of a line that connects two points in a plane.

The formula for finding the distance between two points is usually given by,

d=(x2−x1)2+(y2−y1)2

This formula is used to find the distance between any two points in the coordinate plane or x-y plane.

03

According to the question:

Let S1a,0and S2−a,0.

Let the point with constant path difference is x,yP.

localid="1663399680029" S2P−S1P=cx+a2+y2−x-a2+y2=c

04

All curves over the phase difference: 

Squaring both of the sides of equation (1) , and you have

2(x+a)2+2y2−c2=2(x+a)2+y2(x−a)2+y2x+a2+y2−c222=x+a2+y2x-a2+y2(x+a)4+y4+c44+2y2(x+a)2−y2c2−c2(x+a)2=(x+a)2(x−a)2+(x+a)2y2+(x−a)2y2+y4

y4+2y2(x+a)2−y2c2=(x+a)2(x−a)2+(x+a)2y2+(x−a)2y2+y4+(x+a)4−c44+c2(x+a)22y2(x+a)2−y2c2−(x+a)2y2−(x−a)2y2=(x+a)2(x−a)2+(x+a)4−c44+c2(x+a)2

After solving the above equation gives:

y2((x+a)2−c2−(x−a)2)=(x+a)2((x−a)2+(x+a)2+c2)−c44y2(4xa−c2)=(x+a)2(2x2+2a2+c2)−c44(x+a)2(2x2+2a2+c2)−y2(4xa−c2)=c44

(x+a)2×4(2x2+2a2+c2)c4−y2×4(4xa−c2)c4=1x2a2−y2β2=1

Thus, the equation obtain is:

x2a2−y2β2=1

Here, βis a constant,

Above equation is an equation of hyperbola.

Hence, all curves are hyperbola.

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Most popular questions from this chapter

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?

A thin flake of mica (n = 1.58) is used to cover one slit of a double-slit interference arrangement. The central point on the viewing screen is now occupied by what had been the seventh bright side fringe (m = 7). If λ=550nm , what is the thickness of the mica?

In Fig. 35-38, sourcesand emit long-range radio waves of wavelength400m , with the phase of the emission from ahead of that from source Bby 90° .The distance rA from Ato detector Dis greater than the corresponding distance localid="1663043743889" rBby 100m .What is the phase difference of the waves at D ?

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 ray r3(the light does not reflect inside material 2) and r4(the light reflects twice inside material 2). The waves of r3andr4interfere, 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 refractionn1,n2andn3the type of interference, the thin-layer thicknessLin nanometers, and the wavelengthλin nanometers of the light as measured in air. Whereλis missing, give the wavelength that is in the visible range. WhereLis missing, give the second least thickness or the third least thickness as indicated.

In Fig. 35-39, two isotropic point sources S1 and S2 emit light in phase at wavelength λ and at the same amplitude. The sources are separated by distance 2d=6λ. They lie on an axis that is parallel to an x axis, which runs along a viewing screen at distance D=20.0λ. The origin lies on the perpendicular bisector between the sources. The figure shows two rays reaching point P on the screen, at positionxP. (a) At what value of xPdo the rays have the minimum possible phase difference? (b) What multiple ofλ gives that minimum phase difference? (c) At what value ofxPdo the rays have the maximum possible phase difference? What multiple of λ gives (d) that maximum phase difference and (e) the phase difference when xP=6λ ? (f) When xP=6λ, is the resulting intensity at point P maximum, minimum, intermediate but closer to maximum, or intermediate but closer to minimum?

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