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A spacecraft of the Trade Federation flies past the planet Coruscant at a speed of 0.600c. A scientist on Coruscant measures the length of the moving spacecraft to be 74.0 m. The spacecraft later lands on Coruscant, and the same scientist measures the length of the now stationary spacecraft. What value does she get?

Short Answer

Expert verified
The proper length of the spacecraft is 92.5 m.

Step by step solution

01

Understand the Lorentz Contraction

The measured length of a moving object contracts in the direction of motion due to special relativity. This phenomenon is known as Lorentz contraction. The formula to calculate the contracted length \( L \) is \( L = L_0 \sqrt{1 - v^2/c^2} \), where \( L_0 \) is the proper length, \( v \) is the velocity of the object, and \( c \) is the speed of light.
02

Identify the Given Values

We are given the velocity \( v = 0.600c \) and the contracted length \( L = 74.0 \text{ m} \). We need to find the proper length \( L_0 \) of the spacecraft when it is at rest.
03

Calculate the Proper Length

Rearrange the Lorentz contraction formula to solve for the proper length \( L_0 \). The formula becomes \( L_0 = \frac{L}{\sqrt{1 - v^2/c^2}} \). Substitute the known values: \( L = 74.0 \text{ m} \), \( v = 0.600c \), and \( c = 1 \) in terms of \( c \).
04

Compute the Denominator Term

Calculate \( 1 - v^2/c^2 \). Since \( v = 0.600c \), we have \( v^2 = (0.600c)^2 = 0.36c^2 \), so \( 1 - v^2/c^2 = 1 - 0.36 = 0.64 \).
05

Solve for the Proper Length \( L_0 \)

Using the adjusted formula \( L_0 = \frac{L}{\sqrt{0.64}} \), substitute \( L = 74.0 \text{ m} \) to find \( L_0 = \frac{74.0}{\sqrt{0.64}} \approx 74.0 \times \frac{5}{4} = 92.5 \text{ m} \).

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Key Concepts

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

Special Relativity
Special Relativity is a fundamental theory in physics developed by Albert Einstein. It describes the behavior of objects moving at speeds close to the speed of light, known as relativistic speeds. One of the key ideas of this theory is that the laws of physics are the same for all observers, regardless of their relative motion.
A critical outcome of this theory is the realization that time and space are interconnected into a single entity called spacetime. This means that time can slow down or speed up depending on an object's velocity relative to the observer, and similarly, distances can appear contracted.
Key concepts in Special Relativity include:
  • The constancy of the speed of light: The speed of light in a vacuum is the same for all observers, no matter their velocity.
  • Time dilation: Clock measurements can differ for observers moving relative to each other.
  • Length contraction: Physical lengths appear shorter in the direction of motion when viewed from different inertial frames.
Overall, Special Relativity introduces a novel way of understanding motion at high speeds, breaking away from classical Newtonian mechanics.
Proper Length
The concept of Proper Length is central in understanding how objects behave under Special Relativity. Proper Length is the length of an object as measured in the object's own rest frame, meaning it's the longest length one can measure for that object.
This is because when the object is not moving relative to the observer, the effects of relativistic movement, such as length contraction, do not apply.
For example, if a spacecraft is at rest relative to a planet, and measures 100 meters from front to back according to an onboard observer, that 100 meters is its Proper Length.
In the context of relativity, finding the Proper Length helps us understand how motion affects distances. When an object moves with a significant fraction of the speed of light relative to an observer, the observed length will be less than the Proper Length.
Calculating Proper Length is important for comparing how measurements of the same object can differ between different frames of reference, as demonstrated in the Lorentz contraction formula.
Length Contraction
Length Contraction is an intriguing phenomenon predicted by Einstein's theory of Special Relativity. When an object moves at a significant fraction of the speed of light relative to an observer, its length parallel to the direction of motion appears shorter to that observer.
This contraction is only detectable at relativistic speeds, which are generally much faster than everyday speeds here on Earth.
The mathematical expression to calculate the contracted length, also known as the Lorentz contraction, is: \[ L = L_0 \sqrt{1 - \frac{v^2}{c^2}} \] Where:
  • **\( L \)** is the contracted length viewed by the observer in motion.
  • **\( L_0 \)** is the Proper Length, or the length of the object in its rest frame.
  • **\( v \)** is the relative velocity of the object and the observer.
  • **\( c \)** is the speed of light.
Using this formula, one can determine how long an object appears to an observer witnessing it in motion. As speed increases closer to the speed of light, the observed length decreases, reaching much larger contraction as speeds approach \( c \). This concept was key to solving the exercise involving the spacecraft's observed length on the planet Coruscant.

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Most popular questions from this chapter

Electrons are accelerated through a potential difference of 750 kV, so that their kinetic energy is 7.50 \(\times\) 10\(^5\) eV. (a) What is the ratio of the speed \(v\) of an electron having this energy to the speed of light, \(c\)? (b) What would the speed be if it were computed from the principles of classical mechanics?

A cube of metal with sides of length \(a\) sits at rest in a frame \(S\) with one edge parallel to the \(x\)-axis. Therefore, in \(S\) the cube has volume \(a^3\). Frame \(S'\) moves along the \(x\)-axis with a speed \(u\). As measured by an observer in frame \(S'\), what is the volume of the metal cube?

Muons are unstable subatomic particles that decay to electrons with a mean lifetime of 2.2 \(\mu\)s. They are produced when cosmic rays bombard the upper atmosphere about 10 km above the earth's surface, and they travel very close to the speed of light. The problem we want to address is why we see any of them at the earth's surface. (a) What is the greatest distance a muon could travel during its 2.2 - \(\mu\)s lifetime? (b) According to your answer in part (a), it would seem that muons could never make it to the ground. But the 2.2- \(\mu\)s lifetime is measured in the frame of the muon, and muons are moving very fast. At a speed of 0.999c, what is the mean lifetime of a muon as measured by an observer at rest on the earth? How far would the muon travel in this time? Does this result explain why we find muons in cosmic rays? (c) From the point of view of the muon, it still lives for only 2.2 \(\mu\)s, so how does it make it to the ground? What is the thickness of the 10 km of atmosphere through which the muon must travel, as measured by the muon? Is it now clear how the muon is able to reach the ground?

Space pilot Mavis zips past Stanley at a constant speed relative to him of 0.800c. Mavis and Stanley start timers at zero when the front of Mavis's ship is directly above Stanley. When Mavis reads 5.00 s on her timer, she turns on a bright light under the front of her spaceship. (a) Use the Lorentz coordinate transformation derived in Example 37.6 to calculate x and t as measured by Stanley for the event of turning on the light. (b) Use the time dilation formula, Eq. (37.6), to calculate the time interval between the two events (the front of the spaceship passing overhead and turning on the light) as measured by Stanley. Compare to the value of \(t\) you calculated in part (a). (c) Multiply the time interval by Mavis's speed, both as measured by Stanley, to calculate the distance she has traveled as measured by him when the light turns on. Compare to the value of \(x\) you calculated in part (a).

As you have seen, relativistic calculations usually involve the quantity \(\gamma\). When \(\gamma\) is appreciably greater than 1, we must use relativistic formulas instead of Newtonian ones. For what speed \(v\) (in terms of \(c\)) is the value of \(\gamma\) (a) 1.0% greater than 1; (b) 10% greater than 1; (c) 100% greater than 1?

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