Relativity and Lorentz Transformations

In summary, two spaceships, A and B, are traveling at 0.6 times the speed of light past each other. Clocks on both ships are synchronized and set to zero at the moment when A passes B. A light flashes at the front of ship A at this time. Using Lorentz transformation formulas, it can be determined that the reading of the clock at the rear of ship A when the light reaches it is 5.0*10^-8 seconds. The reading on the clock on ship B when the light reaches the rear of ship A, as observed by someone on ship B, can also be calculated using the same formulas.
  • #1
little neutrino
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Homework Statement


Spaceship A of length 30m travels at 0.6c past spaceship B. Clocks in frame S' of spaceship A and S of spaceship B are synchronised within their respective frames of reference and are set to zero, so that t' = t = 0 at the instant the front of spaceship A passes the rear of spaceship B located at x' = x = 0. At this time a light flashes at the front of spaceship A.

a. When the light flash reaches the rear of spaceship A, what is the reading of a clock there?
b. What is the reading on the clock on spaceship B when according to an observer on B, the flash reaches the rear of A?

Homework Equations


Lorentz transformation formulas

The Attempt at a Solution


a. From spaceship A's POV, it is stationary. It measures proper length. Thus time t1' = 30m / speed of light. Is this correct?

b. Using Lorentz transformation of time,
t = γ(t' + ux'/c2)

x1' = -30, u = 0.6c and t1' from answer in a, I got t1 = 5.0*10-8 s. Does this work?

Thanks!
 
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  • #2
little neutrino said:

Homework Statement


Spaceship A of length 30m travels at 0.6c past spaceship B. Clocks in frame S' of spaceship A and S of spaceship B are synchronised within their respective frames of reference and are set to zero, so that t' = t = 0 at the instant the front of spaceship A passes the rear of spaceship B located at x' = x = 0. At this time a light flashes at the front of spaceship A.

a. When the light flash reaches the rear of spaceship A, what is the reading of a clock there?
b. What is the reading on the clock on spaceship B when according to an observer on B, the flash reaches the rear of A?

Homework Equations


Lorentz transformation formulas

The Attempt at a Solution


a. From spaceship A's POV, it is stationary. It measures proper length. Thus time t1' = 30m / speed of light. Is this correct?

b. Using Lorentz transformation of time,
t = γ(t' + ux'/c2)

x1' = -30, u = 0.6c and t1' from answer in a, I got t1 = 5.0*10-8 s. Does this work?

Thanks!
Yes.
 
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1. What is the theory of relativity?

The theory of relativity, developed by Albert Einstein, is a fundamental concept in physics that describes the relationship between space and time. It states that the laws of physics are the same for all observers in uniform motion and that the speed of light is constant regardless of the observer's frame of reference.

2. What are Lorentz transformations?

Lorentz transformations are a set of equations that describe how measurements of space and time differ for two observers in relative motion. They are a key component of the theory of relativity and help explain the effects of time dilation and length contraction.

3. What is the difference between special and general relativity?

Special relativity deals with the relationship between space and time for objects moving at constant speeds, while general relativity also takes into account the effects of gravity. Special relativity is a more specific and simplified version of general relativity, which is a more comprehensive theory.

4. How do Lorentz transformations affect the concept of time?

Lorentz transformations show that time is not absolute and can appear to pass at different rates for different observers depending on their relative motion. This is known as time dilation and is a key principle of relativity.

5. What are some real-world applications of relativity and Lorentz transformations?

Relativity and Lorentz transformations have been extensively verified through numerous experiments and have practical applications in fields such as astrophysics, nuclear physics, and GPS technology. They also have implications for modern technologies such as particle accelerators and GPS satellites.

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