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Figure 35-57 shows an optical fiber in which a central platic core of index of refractionn1=1.58-is surrounded by a plastic sheath of index of refractionn2=1.53. Light can travel along different paths within the central core, leading to different travel times through the fiber, resulting in information loss. Consider light that travels directly along the central axis of the fiber and light that is repeatedly reflected at the critical angle along the core-sheath interface, reflecting from side to side as it travels down the central core. If the fiber length is 300 m, what is the difference in the travel times along these two routes?

Short Answer

Expert verified

Thus, the difference in the travel times along two routes is 51.6ns.

Step by step solution

01

Light travel along different paths within the central core.

A light ray travelling directly along the central axis reaches the end in time

tdirect=Lv1=n1Lc

For the ray taking the critical zig –zag path, only its velocity component along the core axis direction contributes to reach the other end of the fiber. That component isv1cosθ , so the time of travel for this ray is:

tzig-zag=1v1cosθ=n1Lc1-(sinθn1)2

Using results from the previous solution. Plugging in sinθ=n12-n22and simplifying gives:

tzig-zag=n1Lc(n2n1)=n12Lcn3

02

The difference in the travel times along two routes.

The difference is written as follows:

Δt=tzig-zag-tdirect=n1Lcn3-n1Lc=n1Lcn1n2-1

Withn1=1.58,n2=1.53andL=300mgives

Δt=n1Lcn1n2-1

=1.58800m3×108m/s1.581.53-1

=5.16×10-8s

=51.6ns

Hence, the difference in the travel times along two routes is 51.6ns.

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Most popular questions from this chapter

If mirror M2in a Michelson interferometer (fig 35-21) is moved through 0.233mm, a shift of 792 bright fringes occurs. What is the wavelength of the light producing the fringe pattern?

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 r3and 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. Where λis 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.

Figure 35-25 shows two sources s1 and s2 that emit radio waves of wavelengthλin all directions. The sources are exactly in phase and are separated by a distance equal to 1.5λ . The vertical broken line is the perpendicular bisector of the distance between the sources.

(a) If we start at the indicated start point and travel along path 1, does the interference produce a maximum all along the path, a minimum all along the path, or alternating maxima and minima? Repeat for

(b) path 2 (along an axis through the sources) and

(c) path 3 (along a perpendicular to that axis).

The speed of yellow Light (from a sodium lamp) in a certain liquid is measured to be1.92×108ms . What is the index of refraction of this liquid for the Light?

A 600nm-thick soap film n=1.40in air is illuminated with white light in a direction perpendicular to the film. For how many different wavelengths in the 300to 700nm range is there (a) fully constructive interference and (b) fully destructive interference in the reflected light?

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