/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 43 The angle of incidence of a ligh... [FREE SOLUTION] | 91Ó°ÊÓ

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The angle of incidence of a light beam onto a reflecting surface is continuously variable. The reflected ray is found to be completely polarized when the angle of incidence is \(48.0^{\circ} .\) What is the index of refraction of the reflecting material?

Short Answer

Expert verified
The index of refraction of the reflecting material is approximately \(1.11\).

Step by step solution

01

Identify the given

The given is the Brewster's angle i.e., the angle of incidence, which is \(48.0^{\circ}\).
02

Apply Brewster's Law

Brewster's law gives the relationship between the angle of incidence and the refractive index of the material as \(n = tan θ_{B}\), where \(n\) is the refractive index and \(θ_{B}\) is the Brewster's angle.
03

Calculation using trigonometry function

Substitute the given Brewster's angle into the equation and calculate the result. In this case, \(n = tan (48.0^{\circ})\).
04

Calculating index of refraction

After using our calculator to compute the tangent of \(48.0^{\circ}\), we get \(1.11\). Therefore, the index of refraction of the reflecting material is \(1.11\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Brewster's Law
Imagine you're wearing sunglasses on a sunny day, and you notice that certain reflections disappear when you tilt your head. This is connected to an important concept in physics known as Brewster's Law. Brewster's Law helps us understand why at a certain angle—the aptly named Brewster's angle—light reflecting off a surface can become completely polarized.

What exactly does this mean? When light reaches the boundary between two materials (like air and glass), a specific angle of incidence will cause the reflected light to be entirely plane polarized. This critical angle depends on the inherent properties of the materials involved, specifically their indices of refraction. Mathematically, Brewster's Law is defined as \( n = \tan(\theta_B) \), where \( n \) is the index of refraction of the material and \( \theta_B \) represents the Brewster's angle.

When you're dealing with problems involving Brewster's Law, remember, it's more than just plugging numbers into a formula. Understanding Brewster's Law can give insights into many practical applications ranging from designing anti-reflective coatings to enhancing the contrast in photography.
Angle of Incidence
When we talk about the angle of incidence, we're referring to the specific angle at which a wave—in this case, light—hits a surface. This isn't just any angle; it's measured from the normal, an imaginary line that's perpendicular to the surface at the point of contact.

Why is the angle of incidence so crucial? In physics, the behavior of light as it encounters different materials highly depends on this angle. The law of reflection states that the angle of incidence is equal to the angle of reflection, which you might have seen when light bounces off a mirror. However, when it comes to Brewster's angle, the reflected light behaves differently, displaying full polarization.

The concept of the angle of incidence isn't limited to reflection. It's also a key player in refraction—the bending of light as it passes into a different medium—where it influences the refractive angle and is tied to Snell's Law, another fundamental law in optics.
Polarization of Light

Understanding Polarization

Light waves can vibrate in many directions. When these waves are restricted to vibrate in a single direction, we say that the light is polarized. This concept is easier to visualize if you imagine light waves as a series of oscillating strings, lying on a variety of planes. Polarization aligns these planes, so they oscillate uniformly.

Real-world Applications

The polarization of light is pivotal in numerous technologies we use every day. For instance, 3D movies exploit polarization to create the illusion of depth, and photographers use polarizing filters to reduce glare and enhance contrasts.

Polarization doesn't just have human-engineered applications; it's also useful in the natural world. Some animals, such as bees, use polarized light for navigation. As you can see, the concept of polarization permeates both the natural and technological aspects of our lives, illustrating its immense significance in our understanding of light.
Trigonometry in Physics
Trigonometry, the branch of mathematics dealing with angles and sides of triangles, has a powerful application in physics, particularly in understanding wave behaviors like reflection and refraction.

When solving problems involving Brewster's angle, we often use the trigonometric function tangent, denoted as \( \tan \). To find the index of refraction relative to a medium's Brewster's angle, as in the textbook exercise, we use the formula \( n = \tan(\theta_B) \). Here, \( \theta_B \) is the Brewster's angle, and \( n \) is what we're solving for—the index of refraction.

Trigonometry is essential in translating the angles and distances we observe into precise information about the properties of materials and the nature of light waves. It's a fundamental tool in a physicist's toolkit that allows us to model and predict the behavior of physical phenomena, cementing its status as an indispensable part of science education.

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Most popular questions from this chapter

How much diffraction spreading does a light beam undergo? One quantitative answer is the full width at half maximum of the central maximum of the single- slit Fraunhofer diffraction pattern. You can evaluate this angle of spreading in this problem and in the next. (a) In Equation \(38.4,\) define \(\beta / 2=\phi\) and show that, at the point where \(I=0.5 I_{\max },\) we must have \(\sin \phi=\phi / \sqrt{2} .\) (b) Let \(y_{1}=\sin \phi\) and \(y_{2}=\phi / \sqrt{2} .\) Plot \(y_{1}\) and \(y_{2}\) on the same set of axes over a range from \(\phi=1\) rad to \(\phi=\pi / 2\) rad. Determine \(\phi\) from the point of intersection of the two curves. (c) Then show that, if the fraction \(\lambda / a\) is not large, the angular full width at half maximum of the central diffraction maximum is \(\Delta \theta=0.886 \lambda / a\)

Light from a helium-neon laser \((\lambda=632.8 \mathrm{nm})\) is incident on a single slit. What is the maximum width of the slit for which no diffraction minima are observed?

You are vacationing in a Wonderland populated by friendly elves and a cannibalistic Cyclops that devours physics students. The elves and the Cyclops look precisely alike (everyone wears loose jeans and sweatshirts) except that each elf has two eyes, about \(10.0 \mathrm{cm}\) apart, and the Cyclops-you guessed it-has only one eye of about the same size as an elf's. The elves and the Cyclops are constantly at war with each other, so they rarely sleep and all have red eyes, predominantly reflecting light with a wavelength of \(660 \mathrm{nm} .\) From what maximum distance can you distinguish between a friendly elf and the predatory Cyclops? The air in Wonderland is always clear. Dilated with fear, your pupils have a diameter of \(7.00 \mathrm{mm}\)

Unpolarized light passes through two polaroid sheets. The axis of the first is vertical, and that of the second is at \(30.0^{\circ}\) to the vertical. What fraction of the incident light is transmitted?

A grating with 250 grooves/mm is used with an incandescent light source. Assume the visible spectrum to range in wavelength from 400 to 700 nm. In how many orders can one see (a) the entire visible spectrum and (b) the shortwavelength region?

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