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Two distant galaxies are receding from Earth at \(0.75 c\) in opposite directions. How fast does an observer in one galaxy measure the other to be moving?

Short Answer

Expert verified
An observer in one galaxy would measure the other galaxy to be moving at approximately \(0.96c\).

Step by step solution

01

Identify the Knowns

In this exercise, the known values are the speed of the two galaxies with respect to Earth (\(v_1, v_2 = 0.75c\)) and the speed of light (\(c\)).
02

Apply the Relativistic Velocity Addition Formula

Plug those values into the relativistic velocity addition formula to find the observed speed of one galaxy relative to the other: \(v' = \frac{v_1 +v_2}{1 + \frac{v_1v_2}{c^2}} = \frac{0.75c + 0.75c}{1 + \frac{(0.75c)(0.75c)}{c^2}}\).
03

Calculation

Perform the calculation to find the observed speed: \(v' = \frac{1.5c}{1.5625} = 0.96c\) (approximately).

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Key Concepts

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

Speed of Light
Understanding the concept of the speed of light is essential when diving into relativistic physics. The speed of light in a vacuum, denoted as 'c', is approximately 299,792,458 meters per second. This value is significant because it represents the ultimate speed limit for any form of matter or information in the universe.

According to Einstein's theory of Special Relativity, nothing can travel faster than the speed of light. In everyday life, speeds approaching 'c' are unfathomable, but when studying cosmic phenomena, this limit becomes crucial. For example, when galaxies recede from Earth, they can do so at speeds that are significant fractions of 'c', which affects how we calculate their motion relative to one another.

While we use 'c' to describe the speed of light, in relativistic equations, we often see 'c' used to normalize other velocities. This practice allows us to express speeds as a fraction of the speed of light, simplifying comparisons to this cosmic speed limit.
Special Relativity
The theory of Special Relativity, developed by Albert Einstein, revolutionized our understanding of space, time, and motion. At its core, Special Relativity addresses how the laws of physics are the same for all non-accelerating observers and how the speed of light is constant in a vacuum, regardless of the motion of the light source or the observer.

Time Dilation and Length Contraction

As objects move closer to the speed of light, time dilation, where time appears to pass slower, and length contraction, where lengths appear to shorten, become noticeable. These effects are not due to the limitations of our measurement but are real consequences of the relative motion as described by the Special Relativity.

Relativistic Velocity Addition

A fascinating implication of Special Relativity is the way we calculate velocities. When dealing with speeds that are significant fractions of the speed of light, adding them is not as simple as in classical mechanics. We must use the relativistic velocity addition formula, which takes into account the limiting nature of the speed of light to ensure that the resulting velocity does not exceed 'c'.
Galactic Motion
Galactic motion refers to the movement of galaxies as they travel through space. The study of this motion is complex, owing to the vast distances and high speeds involved, combined with the influence of gravity exerted by massive objects like black holes and dark matter.

Observations of galactic motion provide essential insights into the structure and evolution of the Universe. One such observation is the discovery that galaxies are receding from one another, which supports the Big Bang theory and suggests that the Universe is expanding.

When studying the motion of galaxies, especially those receding at speeds comparable to the speed of light, we must take relativistic effects into account. The distances are so immense, and the speeds so great, that conventional Newtonian mechanics falls short. Instead, we turn to Special Relativity, which allows for the accurate description of such high-speed motion and is essential for understanding the workings of the Universe on the grandest scales.

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Most popular questions from this chapter

The length of an object be \(l\), in a reference frame \(S\). The length of this object \(l\), in another reference frame \(S\) varies due to the motion of the object with a different velocity in frame \(S\). The speed of the object in the reference frame taken is in terms of speed of light. The speed of the object in the reference frame is less than the speed of light \((v

You've been named captain of NASA's first interstellar mission since the Voyager robotic spacecraft. You board your spaceship, accelerate quickly to \(0.8 c,\) and cruise at constant speed toward Proxima Centauri, the closest star to our Sun. Proxima Centauri is 4 light-years distant as measured in the two stars' common rest frame. On the way, you conduct various medical experiments to determine the effects of a long space voyage on the human body. Taking your pulse, you find a. it's significantly slower than when you're on Earth. b. it's the same as when you're on Earth. c. it's significantly faster than when you're on Earth.

Find the speed of an electron with kinetic energy (a) 100 eV, (b) \(100 \mathrm{keV},\) (c) \(1 \mathrm{MeV},\) and (d) \(1 \mathrm{GeV} .\) Use suitable approximations where possible.

You're writing a galactic history involving two civilizations that evolve on opposite sides of a \(10^{5}\) -ly-diameter galaxy. In the galaxy's reference frame, civilization B launched its first spacecraft 50,000 years after civilization A. You and your readers, from a more advanced civilization, are traveling through the galaxy at \(0.99 c\) on a line from A to B. Which civilization do you record as having first achieved interstellar travel, and how much in advance of the other?

The rest energy of an electron is 511 keV. What's the approximate speed of an electron whose total energy is 1 GeV? (Note: No calculations needed!)

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