Lorent's time transformation Feynman 15-6 simultaneity

In summary, Feynman discusses the failure of simultaneity at a distance using Lorentz's transformation of time. When a man synchronizes two clocks on a moving spaceship in system S', an observer in system S notes that the clocks are not synchronized due to the difference in their velocities. The question is asked if the clocks are synchronized in S', to which the answer is yes, but not in S. This concept is known as the relativity of simultaneity and is a difficult concept in special relativity. Once understood, other concepts become easier.
  • #1
nitai108
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Feynman makes an example (15-6 in his lectures) about failure of simultaneity at a distance, using the Lorentz's transformation of time.
A man moving in a spaceship (system S') synchronizes two clocks, placing them at each end of the ship, by a light signal sent from the middle of the ship, and he assumes the clocks are synchronized. An observer in system S reasons that since the ship is moving forward the clock in the front is running away from the signal, and the one in the back is moving toward the signal, therefore the signal reached the rear clock first, and they are not synchronized.

My question is, in the system S' are the clock synchronized? In S the are not synchronized, is this correct?
If the light travels at the same velocity they should be synchronized in S', and because the clocks travel at the same velocity in the spaceship they should read the same time in the S system (but they don't because they are separated by a distance x, which modifies the time transformation in the Lorentz's transformation, is this correct?).
 
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  • #2
nitai108 said:
My question is, in the system S' are the clock synchronized? In S the are not synchronized, is this correct?
Yes, and yes. The clocks are synchronized in S' but not in S. This is the relativity of simultaneity, and it is the most difficult concept in SR. Once you get this one down, the rest are easy.
 
  • #3
Thanks!
 

1. What is Lorentz's time transformation?

Lorentz's time transformation is a mathematical formula developed by Dutch physicist Hendrik Lorentz in the late 19th century. It describes how time and space coordinates change for an observer in one frame of reference when viewed from another frame of reference moving at a constant velocity.

2. What is Feynman's 15-6 simultaneity?

Feynman's 15-6 simultaneity refers to a thought experiment proposed by American physicist Richard Feynman in his book "The Feynman Lectures on Physics." It involves two observers moving at different velocities and their perception of simultaneous events. This experiment demonstrates the principles of Lorentz's time transformation.

3. Why is Lorentz's time transformation important?

Lorentz's time transformation is important because it is a fundamental concept in special relativity, which explains how time and space are relative to the observer's frame of reference. It has been verified through numerous experiments and is essential for understanding the behavior of objects moving at high speeds.

4. How does Lorentz's time transformation relate to Einstein's theory of relativity?

Lorentz's time transformation is a key component of Einstein's theory of relativity. It was initially developed by Lorentz to explain the experimental results of the Michelson-Morley experiment, which led Einstein to develop his theory of special relativity. Lorentz's time transformation is used to calculate the effects of time dilation and length contraction in special relativity.

5. Can Lorentz's time transformation be applied to everyday life?

Yes, Lorentz's time transformation can be applied to everyday life. It is used in various fields, including astronomy, particle physics, and engineering, to accurately describe the behavior of objects moving at high speeds. It also has practical applications, such as in the design of GPS systems, which rely on the principles of special relativity to function accurately.

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