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Circularly polarized light of intensity \(I_{0}\) is incident on a sandwich of three polaroids. The first and third polaroids are crossed, i.e., their easy axes are at 90 deg to one another. The middle polaroid makes an angle \(\theta\) with the axis of the first polaroid. Show that the output intensity is \(\frac{1}{2} I_{0} \cos ^{2} \theta \sin ^{2} \theta\)

Short Answer

Expert verified
The output intensity is given by \( \frac{1}{2} I_0 \cos^2 \theta \sin^2 \theta \).

Step by step solution

01

Understand Circular Polarization

Circularly polarized light has equal intensity components (\( I_0/2 \) for each component) along any two perpendicular directions in the plane perpendicular to the direction of propagation.
02

Apply First Polaroid

The first polaroid will let through only the component of light that is parallel to its axis. Since the light is circularly polarized, the intensity after the first polaroid is \( I_0/2 \), but the light becomes linearly polarized.
03

Apply Malus's Law for the Second Polaroid

The intensity of the light after passing the second polaroid (oriented at an angle \( \theta \) to the first polaroid) can be found using Malus's Law:\[ I = \left( \frac{I_0}{2} \right) \cos^2 \theta \]
04

Apply Third Polaroid

The third polaroid is crossed with the first, meaning it is also at an angle \( 90^\circ - \theta \) with the second polaroid. We apply Malus's Law again to account for this additional rotation:\[ I = \left( I_0 \cos^2(\theta) \right) \sin^2 \theta \]
05

Simplify Expression

Combine the results from the above steps:\[ I = \frac{1}{2} I_0 \cos^2 \theta \sin^2 \theta \]

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Key Concepts

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

Malus's Law
Malus's Law is a key principle in understanding how light intensity changes when it passes through a series of polarizers. It states that the intensity of polarized light after passing through a polarizer is given by the formula:
  • \(I = I_0 \cos^2 \theta \)
where \(I\) is the transmitted light intensity, \(I_0\) is the initial intensity, and \(\theta\) is the angle between the light's initial polarization direction and the axis of the polarizer.
This principle helps predict the behavior of light as it passes through multiple layers of polarizers with different orientations. It explains how the amount of light decreases depending on the angle, which is essential in calculating light intensity in experiments involving polarized light.
Understanding this concept allows you to solve problems involving multiple polarizers by sequentially applying the law at each step.
Polaroids
Polaroids are optical devices that filter light waves to allow only those oscillating in a specific direction to pass through. They are crucial for manipulating and analyzing polarized light.
These filters are made of materials that can absorb certain light wave orientations while permitting others to pass through.
When you place polaroids in a series, each polaroid affects the light further, either retaining its linear polarization or altering it based on alignment.
  • First Polaroid: Polarizes incoming light,
  • Middle Polaroid: Adjusts light polarization based on its angle,
  • Third Polaroid: Often at a crossing angle with the first to filter further.
By understanding how polaroids work, you can predict light behavior in setups where controlling light orientation and intensity is necessary, like in photography and displays.
Light Intensity
Light intensity refers to the power per unit area carried by a wave. In the context of polarized light and Malus's Law, we often express intensity in terms of how much light makes it through polaroids.
The initial intensity \(I_0\) represents the energy or brightness of the light before any filters affect it.
As light passes through a series of polaroids, the intensity is reduced depending on their orientation and alignment, guided by Malus's Law.
  • Initial Intensity \(I_0\): Before encountering any polaroid,
  • After First Polaroid: \(I_0/2\), as circularly polarized light gets partially absorbed,
  • Final Intensity: As calculated, given by \(\frac{1}{2} I_0 \cos^2 \theta \sin^2 \theta\).
This progressive reduction highlights how light's power diminishes with each stage, which is essential for understanding various optical applications.
Linear Polarization
Linear polarization is a state where the light waves oscillate in parallel planes. This concept is crucial when discussing polarized materials and how they affect light. In the process of analyzing polarized light:
  • Circularly polarized light becomes linearly polarized after passing through the first polaroid.
  • The alignment of the light waves becomes critical as they pass through additional polarizers.
  • Final outcomes, like light's intensity and direction, depend on the sequential realignment along the polaroids.
In an experiment or application involving polaroids, setting up these orientations properly can enhance technologies like LCD screens and camera lenses. Understanding linear polarization allows you to effectively tailor and apply light in various practical scenarios.

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Most popular questions from this chapter

Circularly polarized light of intensity \(I_{0}\) (intensity means energy fux per unit area per unit time; this is proportional to a photomultiplier's output current, for light at a given frequency) is incident on a single polaroid. Show that the output intensity (intensity of the light emerging from the rear of the polaroid) is \(\frac{1}{2} I_{0}\)

Linearly polarized light with polarization direction at angle \(\theta\) from \(\hat{x}\) is incident on a polaroid with easy axis along \(\hat{x} .\) The first polaroid is followed by a second polaroid with its easy axis along the direction of polarization of the original incident light. Show that if the input intensity is \(I_{0}\), the output intensity is \(I_{0} \cos ^{4} \theta\).

Colors in clear plastics. Find a piece of clear plastic with a glossy finish on both sides, - for example, a plastic icebox dish or other container. Look at specular reflection of the sky at angle of incidence 45 deg or so. Do you see colors? (Put dark cloth or paper underneath to reduce background.) To enhance the effect, hold a piece of polaroid in front of your eye. Explain the origin of the colors.

Look at a light bulb through a piece of polaroid. Is the light polarized? Now insert a piece of cellophane (or your quarter- or half-wave plate) between the light bulb and the polaroid. Now is the light polarized? Reflect the light from a silvery metal, like a table knife. Is the reflected light polarized?

Optical activity. Suppose you send linearly polarized light through a length \(L\) of Karo corn syrup and find that, for \(L=5 \mathrm{~cm}\), red light is rotated by 45 deg. Now reflect the light that has passed through the syrup from a mirror and send it back through the syrup, so that the total length is \(10 \mathrm{~cm}\). (If you do the experiment, make the angle of reflection not quite \(180 \mathrm{deg}\); then look at the "image light bulb" through both the "real syrup" and the "image syrup." As a control experiment, you can look through the "image syrup" alone by moving your head.) Question: After the two traversals, is the linear polarization at 0 or 90 deg to the original direction?

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