At the Long-baseline Interferometer Gravitationalwave Observatory (LIGO) facilities in Hanford, Washington, and Livingston, Louisiana, laser beams of wavelength \(550.0 \mathrm{nm}\) travel along perpendicular paths \(4.000 \mathrm{~km}\) long. Each beam is reflected along its path and back 100 times before the beams are combined and compared. If a gravitational wave increases the length of one path and decreases the other, each by 1.000 part in \(10^{21}\), what is the phase difference between the two beams as a result?

Short Answer

Expert verified
Answer: To find the phase difference, follow these steps: 1. Calculate the change in path length: ΔL = (1 part in \(10^{21}\)) × (4.000 km) 2. Convert the path length to meters: Original path length = 4000 m, Change in path length = ΔL × 4000 m 3. Calculate the total length traveled by a laser beam: L = 4000 m × 2 × 100 4. Determine the change in distance traveled by laser beams: ΔL_total = 2 × ΔL m 5. Compute the number of wavelengths in the original path: n = L divided by the wavelength 6. Calculate the phase difference: Δϕ = 2π × (total change in distance traveled divided by the wavelength) By using the given wavelength (550 nm) and the values calculated in the previous steps, you can find the phase difference between the two laser beams as a result of the gravitational wave.

Step by step solution

01

Calculate the change in length of the paths

To determine the change in the length of the paths due to the gravitational wave, we can use the given fraction (1 part in \(10^{21}\)) multiplied by the original length of the paths. ΔL = (1.000 part in \(10^{21}\)) × (4.000 km)
02

Convert the path length to meters

To make our calculations easier, we need to convert the path length from kilometers to meters. Original path length: 4.000 km × 1000 (m/km) = 4000 m Change in path length: ΔL m = ΔL × 4000 m
03

Calculate the total length traveled by a laser beam

Given that each laser beam is reflected along its path and back 100 times before combining and comparing them, we calculate the total distance traveled by multiplying the original path length by 2 (since each reflection covers the path twice) and then multiplying it by 100. Total length traveled (without gravitational wave): L = 4000 m × 2 × 100
04

Determine the change in distance traveled by laser beams due to gravitational wave

Since one path increases and the other decreases by the same amount, we calculate the change in distance traveled by one laser beam and multiply it by 2. Change in distance traveled: ΔL_total = 2 × ΔL m
05

Compute the number of wavelengths in the original path

Now, we calculate the number of wavelengths in the original path by dividing the total length traveled by the wavelength. Number of wavelengths: n = L divided by the wavelength
06

Calculate the phase difference

Using the equation for phase difference (Δϕ) and the given wavelength (550.0 nm), we can calculate the phase difference between the two beams as a result of the gravitational wave. Recall that the phase difference is given by: Δϕ = 2π × (total change in distance traveled divided by the wavelength) Converting the wavelength to meters for our calculation: Wavelength = 550.0 nm × \(10^{-9}\) (m/nm) = 550.0 × \(10^{-9}\) m Then plug in the values we calculated earlier and solve for the phase difference.

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!

Key Concepts

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

LIGO (Laser Interferometer Gravitational-Wave Observatory)
The Laser Interferometer Gravitational-Wave Observatory, commonly known as LIGO, is an engineering marvel tasked with the detection of gravitational waves. These elusive ripples in spacetime are generated by extraordinary cosmic events such as the collision of black holes or neutron stars.

LIGO operates two facilities in the United States—one in Hanford, Washington, and the other in Livingston, Louisiana. Both stations work in unison, using laser interferometry to measure minuscule changes in distance caused by passing gravitational waves. Each LIGO observatory features two arms arranged in an L-shape, each stretching about 4 kilometers long. Laser beams are bounced back and forth within these arms and are later combined to reveal any disturbances in their journey which could be indications of gravitational waves passing by.

As gravitational waves traverse the Earth, they stretch and compress space slightly but detectably. LIGO is designed to measure these minute changes in length on the order of a thousandth of the diameter of a proton, which is an incredibly small scale. This is equivalent to accurately measuring the distance to the nearest star outside our solar system (over 4 light-years away) to within the width of a human hair.
Interference of Light
Interference is a fundamental property of light that arises when two or more light waves overlap. It results in a pattern of alternating bright and dark bands, known as interference fringes. This phenomenon occurs because light behaves as a wave, with its crests and troughs either reinforcing or canceling each other out.

When light waves meet in phase—that is, when the crests and troughs align—they constructively interfere to create a bright fringe. Conversely, when they meet out of phase, with the crests of one wave meeting the troughs of another, they destructively interfere and darken the area. This behavior is central to LIGO's ability to detect gravitational waves, as the interference pattern of the laser beams can indicate the minute spatial distortions caused by these waves.

This principle is harnessed in a device known as an interferometer, which splits a single light source into two beams to travel different paths before recombining them. By analyzing the resulting interference pattern, scientists can detect variations in the path lengths that are far too small to measure with conventional tools.
Wavelength and Phase Difference
Wavelength is the distance between consecutive crests (or troughs) in a wave, which, for light, determines its color. In the context of LIGO, the wavelength of a laser beam is crucial as it sets the scale for measuring the tiny distance changes caused by gravitational waves.

Phase difference, on the other hand, is a way of expressing how 'in step' two waves are with each other. It's measured in radians, and when two waves are perfectly in sync (in phase), their phase difference is zero. A phase difference of \( \pi \) radians (or 180 degrees) means the waves are out of phase, leading to destructive interference.

In LIGO, detecting a gravitational wave involves looking for a shift in the interference pattern, which indicates a difference in the phase between the two laser beams. This phase difference arises because the gravitational wave stretches one arm and compresses the other, altering the distance each light beam travels, and hence, their phase relationship upon recombination. By using the wavelength of the laser light and the observed phase difference, scientists can calculate the infinitesimal changes in distance between the interferometer's mirrors, evidencing the presence of a gravitational wave.
Measurement of Gravitational Waves
Gravitational waves are measured by detecting the incredibly minor distortions they cause in the fabric of spacetime as they pass through Earth. In LIGO's interferometers, laser beams travel down the length of each arm and reflect back. The distance the lasers travel should be constant, but a gravitational wave will slightly lengthen one arm and shorten the other.

To put things in perspective, the changes in length we're talking about are smaller than 1/10,000th the width of a proton! It is precisely this change in length that causes a shift in the phase of the laser beams, resulting in a change in the interference pattern.

Detecting this requires exceptionally precise and accurate instruments. The mirrors at LIGO are some of the smoothest and most perfectly shaped in the world, and the instrument is isolated from all other environmental vibrations that could mask the signal of a gravitational wave. This requires complex systems for vibration isolation and laser stabilization, ensuring that only a genuine cosmic event can produce the appropriate signal in the LIGO detectors, confirming the presence of a gravitational wave and offering insights into the profound events that caused them.

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

34.35 Monochromatic blue light \((\lambda=449 \mathrm{nm})\) is beamed into a Michelson interferometer. How many fringes move by the screen when the movable mirror is moved a distance \(d=\) \(0.381 \mathrm{~mm} ?\)

Calculate and compare the angular resolutions of the Hubble Space Telescope (aperture diameter \(2.40 \mathrm{~m}\), wavelength \(450 . \mathrm{nm}\); illustrated in the text), the Keck Telescope (aperture diameter \(10.0 \mathrm{~m}\), wavelength \(450 . \mathrm{nm}\) ), and the Arecibo radio telescope (aperture diameter \(305 \mathrm{~m}\), wavelength \(0.210 \mathrm{~m}\) ). Assume that the resolution of each instrument is diffraction limited.

What is the largest slit width for which there are no minima when the wavelength of the incident light on the single slit is \(600 . \mathrm{nm} ?\)

The irradiance pattern observed in a two-slit interference-diffraction experiment is presented in the figure. The red line represents the actual intensity measured as a function of angle, while the green line represents the envelope of the interference patterns. a) Determine the slit width \(a\) in terms of the wavelength \(\lambda\) of the light used in the experiment. b) Determine the center-to-center slit separation \(d\) in terms of the wavelength \(\lambda\). c) Using the information in the graph, determine the ratio of slit width \(a\) to the center-to-center separation between the slits, \(d\). d) Can you calculate the wavelength of light, actual slit separation, and slit width?

When using a telescope with an objective of diameter \(12.0 \mathrm{~cm},\) how close can two features on the Moon be and still be resolved? Take the wavelength of light to be \(550 \mathrm{nm}\), near the center of the visible spectrum.

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