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To visually examine sunspots through a telescope, astronomers have to reduce the intensity of the sunlight to avoid harming their retinas. They accomplish this intensity reduction by mounting two linear polarizers on the telescope. The second polarizer has a polarizing angle of \(110.6^{\circ}\) relative to the horizontal. If the astronomers want to reduce the intensity of the sunlight by a factor of \(0.7645,\) what polarizing angle should the first polarizer have with the horizontal? Assume that this angle is smaller than that of the second polarizer.

Short Answer

Expert verified
Answer: The polarizing angle of the first polarizer with the horizontal is approximately 81 degrees.

Step by step solution

01

Find the angle between the polarizers

As per Malus' Law, we know that \(I = I_{0}cos^2(\theta)\). Given the desired intensity reduction factor (\(0.7645\)), we can write: \(I = 0.7645 I_{0}\) and \(0.7645 = cos^2(\theta)\) Now, we have to find the angle \(\theta\) between the first and second polarizer.
02

Solve for the angle between the polarizers

Now let's solve for \(\theta\): \(0.7645 = cos^2(\theta)\), so \(cos(\theta) = \pm\sqrt{0.7645}\) Since angles between \(0\) and \(180^{\circ}\) have cosine values between \(1\) and \(-1\), we just take the positive square root value: \(cos(\theta) ≈ 0.874\) To find the angle \(\theta\), we can use the inverse cosine function: \(\theta ≈ cos^{-1}(0.874) ≈ 29.6^{\circ}\)
03

Find the polarizing angle of the first polarizer

We are given the polarizing angle of the second polarizer as \(110.6^{\circ}\), and we have found the angle between the first polarizer and the second polarizer to be \(29.6^{\circ}\). To find the polarizing angle of the first polarizer, we can subtract the angle between the polarizers from the second polarizer's angle: \(\text{Polarizing angle of first polarizer }= 110.6^{\circ} - 29.6^{\circ}\)
04

Calculate the polarizing angle of the first polarizer

Now let's perform the subtraction: \(\text{Polarizing angle of first polarizer }= 110.6^{\circ} - 29.6^{\circ} ≈ 81^{\circ}\) So, the polarizing angle of the first polarizer with the horizontal should be approximately \(81^{\circ}\).

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Key Concepts

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

Malus' Law
Malus' Law plays a critical role in understanding light intensity and polarization. It states that the intensity (\(I\)) of polarized light after passing through a polarizing filter is directly proportional to the square of the cosine of the angle (\( \theta \-\theta\theta\theta\theta ) between the light's initial polarization direction and the axis of the filter.

Let's say we have an incident light beam with an initial intensity of \(I_0\). After passing through the polarizer oriented at angle \(theta\) to the light's polarization direction, the intensity gets reduced to \(I = I_0 cos^2(theta)\).

If a second polarizer is introduced into the path of the polarized light coming from the first polarizer, and it's set at an angle \(theta\) relative to the first, we can apply Malus' Law again to determine the resulting intensity. This principle is used in various applications like photography, LCD displays, and, as in our example, safely observing sunspots through a telescope.
Polarization of Light
The phenomenon of polarization of light refers to the direction in which the electric field of the light wave oscillates. Unpolarized sunlight has waves vibrating in all possible directions perpendicular to the direction of propagation. When this light passes through a polarizing filter, it emerges with waves oscillating in only one direction - it becomes polarized.

Types of Polarizers


There are several types of polarizers, but the most common are linear polarizers which allow light with a particular orientation of the electric field to pass through while blocking the other orientations. They create linearly polarized light, which has a single plane of oscillation.

When discussing sunspot observation, astronomers use linear polarizers to control the light intensity reaching the telescope. By rotating the polarizers at specific angles to each other, they can selectively reduce the brightness and prevent eye damage without losing the required detail in their observations.
Intensity Reduction
Intensity reduction is the process of decreasing the brightness of light, which is particularly important when observing the Sun to prevent damage to sensitive instruments or the human eye. Polarizers achieve intensity reduction by selectively filtering out light that does not align with their polarization axes.

By adjusting the angle between two polarizing filters, astronomers can achieve a specific reduction factor. In the textbook exercise, the goal was to reach an intensity reduction factor of \(0.7645\).

Understanding how intensity reduction works can also reveal why polarized sunglasses are effective in reducing glare. They allow for comfortable vision by blocking scattered, horizontally polarized light and only letting through light polarized in other directions. This same principle ensures astronomers can make detailed observations of the sun without risking their eyesight.

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Most popular questions from this chapter

What is the electric field amplitude of an electromagnetic wave whose magnetic field amplitude is \(5.00 \cdot 10^{-3} \mathrm{~T} ?\)

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In a polarized light experiment, a setup similar to the one in Figure 31.23 is used. Unpolarized light with intensity \(I_{0}\) is incident on polarizer 1\. Polarizers 1 and 3 are crossed (at a \(90^{\circ}\) angle), and their orientations are fixed during the experiment. Initially, polarizer 2 has its polarizing angle at \(45^{\circ} .\) Then, at time \(t=0,\) polarizer 2 starts to rotate with angular velocity \(\omega\) about the direction of propagation of light in a clockwise direction as viewed by an observer looking toward the light source. A photodiode is used to monitor the intensity of the light emerging from polarizer \(3 .\) a) Determine an expression for this intensity as a function of time. b) How would the expression from part (a) change if polarizer 2 were rotated about an axis parallel to the direction of propagation of the light but displaced by a distance \(d

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