/*! 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 10 A high-powered laser beam \((\la... [FREE SOLUTION] | 91Ó°ÊÓ

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A high-powered laser beam \((\lambda=600 \mathrm{~nm})\) with a beam diameter of \(10 \mathrm{~cm}\) is aimed at the Moon, \(3.8 \times 10^{5} \mathrm{~km}\) distant. The beam spreads only because of diffraction. The angular location of the edge of the central diffraction disk (see Eq. 36-12) is given by $$ \sin \theta=\frac{1.22 \lambda}{d} $$ where \(d\) is the diameter of the beam aperture. What is the diameter of the central diffraction disk on the Moon's surface?

Short Answer

Expert verified
The diameter of the central diffraction disk on the Moon is approximately 5560 meters.

Step by step solution

01

Understand the Given Data

We are given the wavelength of the laser \( \lambda = 600 \text{ nm} = 600 \times 10^{-9} \text{ meters} \), the beam diameter \( d = 10 \text{ cm} = 0.1 \text{ meters} \), and the distance to the Moon \( L = 3.8 \times 10^8 \text{ meters} \).
02

Calculate the Angular Width

Using the formula for the angular location of the edge of the central diffraction disk, \( \sin \theta=\frac{1.22 \lambda}{d} \), we can calculate the angular width \( \theta \). Substituting the values, \( \sin \theta = \frac{1.22 \times 600 \times 10^{-9}}{0.1} \approx 7.32 \times 10^{-6} \).
03

Calculate the Angle

To find \( \theta \), we use the fact that for small angles, \( \theta \approx \sin \theta \), so \( \theta \approx 7.32 \times 10^{-6} \text{ radians} \).
04

Find the Diameter of the Central Diffraction Disk

The diameter \( D \) of the central diffraction disk on the Moon's surface can be found using \( D = 2L \theta \). Substituting the values, \( D = 2 \times 3.8 \times 10^8 \times 7.32 \times 10^{-6} \approx 5560 \text{ meters} \).

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Key Concepts

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

Diffraction Disk
When light encounters an obstacle or passes through a small opening, it bends slightly around it. This bending of waves is called diffraction. A diffraction disk, or Airy disk, is a pattern that emerges due to this phenomenon. It is the bright central spot you see when light from a point source like a laser passes through a circular aperture. The size of the diffraction disk is influenced by the wavelength of the light and the aperture size.
To visualize this, imagine shining a flashlight through a small hole onto a wall. The light makes a circular pattern. Similarly, the laser beam aimed at the Moon creates a diffraction disk on its surface. The size of this central disk can be calculated based on the properties of the beam such as its wavelength and aperture diameter. This understanding is crucial in optical physics to control and predict light behavior in experiments and applications.
Laser Beam
A laser beam is a focused stream of coherent light, meaning the light waves are in phase with each other. This coherence makes laser beams incredibly effective for precision tasks like cutting, measuring distances, or pointing to objects in space. Lasers emit light in a continuous narrow beam that can travel long distances without significant spreading. This property is greatly admired in optical physics.
However, even though the beam is focused, diffraction causes it to spread slightly. The degree of this spread depends on factors such as the initial beam diameter and the wavelength of light being used. In the exercise, the high-powered laser beam has a wavelength of 600 nm and a diameter of 10 cm. This setup, although highly focused, will still experience spreading due to diffraction as it travels to the Moon.
Optical Physics
Optical physics is the study of light and its interactions with matter. It encompasses various phenomena including reflection, refraction, and diffraction. Understanding these concepts is crucial in designing optical systems such as telescopes, microscopes, and laser technologies. The focus is often on how light behaves under different conditions and how it can be manipulated to achieve desired outcomes.
The exercise involving the laser beam and its diffraction disk on the Moon is a quintessential example of optical physics at play. It demonstrates the importance of knowing how light behaves over long distances and through different media. Such knowledge is vital for applications in astronomy, telecommunications, and even in developing optical instruments for scientific research.
Diffraction Angle
The diffraction angle is a measure of how much a beam, like that of a laser, spreads due to the impact of diffraction. The angle (\( \theta \)) is calculated using the formula \( \sin \theta = \frac{1.22 \lambda}{d} \) where \(\lambda\) is the wavelength of the light and \(d\) is the diameter of the beam aperture. This formula originates from the study of circular apertures and their effect on wave propagation.
In the exercise, this angle helps determine the size of the diffraction disk on the Moon. The small angle approximation \( \theta \approx \sin \theta \) helps simplify calculations when \(\theta\) is only a few degrees. This simplicity enables more accurate predictions and efficient planning in fields like astronomy, where knowing the extent of light spread is critical for tasks like aiming lasers at distant targets.

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Most popular questions from this chapter

In the subshell \(\ell=4\), (a) what is the greatest (most positive) \(m_{\ell}\) value, (b) how many states are available with the greatest \(m_{\ell}\) value, and (c) what is the total number of states available in the subshell?

For a helium atom in its ground state, what are quantum numbers \(\left(n, \ell, m_{\ell}\right.\), and \(m_{s}\) ) for the (a) spin-up electron and (b) spin-down electron?

The active medium in a particular laser that generates laser light at a wavelength of \(694 \mathrm{~nm}\) is \(6.00 \mathrm{~cm}\) long and \(1.00 \mathrm{~cm}\) in diameter. (a) Treat the medium as an optical resonance cavity analogous to a closed organ pipe. How many standing-wave nodes are there along the laser axis? (b) By what amount \(\Delta f\) would the beam frequency have to shift to increase this number by one? (c) Show that \(\Delta f\) is just the inverse of the travel time of laser light for one round trip back and forth along the laser axis. (d) What is the corresponding fractional frequency shift \(\Delta f / f ?\) The appropriate index of refraction of the lasing medium (a ruby crystal) is \(1.75\).

Show that a moving electron cannot spontaneously change into an x-ray photon in free space. A third body (atom or nucleus) must be present. Why is it needed? (Hint: Examine the conservation of energy and momentum.)

An electron is in a state with \(n=4\). What are (a) the number of possible values of \(\ell\), (b) the number of possible values of \(m_{\ell}\), (c) the number of possible values of \(m_{s}\), (d) the number of states in the \(n=4\) shell, and (e) the number of subshells in the \(n=4\) shell?

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