Question: Figure depicts a simplistic optical fiber: a plastic core(n1=1.58)is surrounded by a plastic sheath (n2=1.53). A light ray is incident on one end of the fiber at angle.The ray is to undergo total internal reflection at point A, where it encounters the core–sheath boundary. (Thus there is no loss of light through that boundary.) What is the maximum value of θthat allows total internal reflection at A?

Figure:

Short Answer

Expert verified

The maximum value of θthat allows total internal reflection at A is 23.2.

Step by step solution

01

Given

  1. Refractive index of the plastic core,n1=1.58
  2. Refractive index of the plastic sheath,n2=1.53
02

Understanding the concept

By using the concept of the critical angle and Snell’s law, we can find the value of θthat allows the total internal reflection.

Formula:

Critical angle is

θc=sin-1n2n1

Snell’s law is :

n1sinθ1=n2sinθ2

03

Calculate the maximum value of θ that allows total internal refection at A.

The critical angle is given by

θc=sin-1n2n1θc=sin-11.531.58=75.547

So, by geometry, the incident angle is

θ1=90-θcθ1=90-75.547o=14.45

Now, we have to apply Snell’s law,

nairsinθ=n1sinθ1

Since nair=1

sinθ=1.58sin14.45simθ=0.3942θ=23.2

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

In Fig. 33-42, unpolarized light is sent into a system of three polarizing sheets. The anglesθ1,θ2andθ3of the polarizing directions are measured counterclockwise from the positive direction of the yaxis (they are not drawn to scale). Anglesθ1and θ3are fixed, but angle θ2can be varied. Figure 33-43 gives the intensity of the light emerging from sheet 3 as a function of θ2. (The scale of the intensity axis is not indicated.) What percentage of the light’s initial intensity is transmitted by the system when θ2=30°?

Figure 33-74 shows a cylindrical resistor oflengthI,radius a, and resistivityr carrying current.i(a) Show that the Poyntingvector at the surface of the resistor is everywhere directed normal to the surface, as shown. (b) Show that the rate at which energy flows into the resistor through its cylindrical surface, calculated by integrating thePoynting vector over this surface, is equal to the rate at which thermal energy is produced: localid="1664201793898" SdA=i2R wherelocalid="1664201800300" dA is an element of the area on the cylindrical surface and localid="1664201803478" R is the resistance.

(a) Prove that a ray of light incident on the surface of a sheet of plate glass of thicknesstemerges from the opposite face parallel to its initial direction but displaced sideways, as in Fig. 33-69. (b) Show that, for small angles of incidence θ, this displacement is given byx=tθn-1n

where nis the index of refraction of the glass andθis measured in radians.

What is the wavelength of the electromagnetic wave emitted by the oscillator–antenna system of the following Fig. 33-3 ifL=0.253μHandC=25.0pF?

Question: In Fig. 33-64, a light ray in air is incident on a flat layer of material 2 that has an index of refraction n2=1.5 . Beneath material 2is material 3 with an index of refraction n3.The ray is incident on the air–material 2 interface at the Brewster angle for that interface. The ray of light refracted into material 3happens to be incident on the material 2-material 3 interface at the Brewster angle for that interface. What is the value of n3 ?

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free