Special Theory of Relativity(discussion question)

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In summary: The answer is: In summary, according to the given equations, if you were on a spaceship moving away from Earth at .8C, there would be a change in your shoe size and mass as observed by an external observer on Earth. However, there would be no observable change in your own measurements as you would be in an inertial frame of reference. The concept of pulse is also relative and not affected by the movement of the spaceship.
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BatmanACC
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Homework Statement



If you were on a spaceship moving away from Earth at .8C, would you observe any change in your shoe size, mass, or your pulse? Would an observer from Earth note any change in these quantities?

Homework Equations



L = Lo[sqrroot(1-v2/c2)]

M = Mo/ sqrroot(1-v2/c2)

The Attempt at a Solution



Disregarding any logical flaws in the argument (that an observer can't view a pulse, he/she cannot see inside a spaceship unless it is transparent, etc)(although mass/pulse need only be recorded...). I'm not sure as to the answer. Now, shoe size as well as mass are different to both the observer and the captain of the spaceship. This is noted by the 2 given equations. So that is easy to explain.

Note: Although I say its easy to explain I may be wrong and if that is the case correct me :P. But it seems logical that both mass/length are relative to the observer and captain because M=moving mass which is not equal to Mo=rest mass and same for the length contraction. And the captain first observes his foot size and mass at rest (before spaceship takes off). Thus when he is moving the quantities should be different.

As for the pulse I don't have an equation to explain it...I'm going to take a stab in the dark and say there's a reason for that. That reason being that the captains pulse is relevant to his/her excitement level and not on any of the 4 dimensions. As such it should be the same for both the observer and captain.

Thanks for taking a look guys. Just wanted to make sure I got this right as I have a test first period tomorrow :).

Edit - Pulse is contingent on time. That was my mistake. Since the Observer experiences time dilation his view will be different from that of the captain. This correct>?

Edit - Assuming the spaceship is moving via the power of rockets and is simply not gliding in space than the Captain is in an inertial frame of reference. Thus, he experiences no time dilation and therefore notices change in nothing.

Sorry for the edits. Just more clearly thinking it out :P
 
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There is no observable change in any measuremnt of an object in your own frame of reference. If there was, it would violate the 2nd posulate, meaning there would be some method of determining an absolute frame of reference.
 
  • #3
I would respond to this question by explaining the concept of the Special Theory of Relativity. According to this theory, the laws of physics are the same for all observers in uniform motion and the speed of light is constant in all inertial frames of reference. This means that the observer on the spaceship and the observer on Earth will both measure the speed of light as c, regardless of their relative motion.

In terms of the specific question, the observer on the spaceship would not observe any change in their shoe size, mass, or pulse. This is because the equations for length contraction and time dilation, L = Lo[sqrt(1-v^2/c^2)] and t = to/sqrt(1-v^2/c^2), only apply to objects in motion relative to an observer. Since the observer on the spaceship is also in motion, they would not notice any change in these quantities.

On the other hand, the observer from Earth would note a change in these quantities. This is because the spaceship is moving at a high speed relative to the observer on Earth, and therefore the equations for length contraction and time dilation would apply. The observer on Earth would see the shoe size and mass of the person on the spaceship as smaller, and their pulse as slower, due to the effects of time dilation.

In conclusion, the Special Theory of Relativity explains that the perception of space and time is relative to the observer's frame of reference, and that the laws of physics are the same for all observers in uniform motion. This theory has been extensively tested and has been proven to accurately describe the behavior of objects in motion.
 

1. What is the Special Theory of Relativity?

The Special Theory of Relativity, also known as the Theory of Relativity, is a scientific theory proposed by Albert Einstein in 1905. It explains the relationship between space and time and how they are affected by the motion of objects.

2. How is the Special Theory of Relativity different from the Theory of General Relativity?

The Special Theory of Relativity focuses on the laws of physics in inertial frames of reference, while the Theory of General Relativity includes the effects of gravity and non-inertial frames of reference.

3. What are the key principles of the Special Theory of Relativity?

The key principles of the Special Theory of Relativity are the principle of relativity, which states that the laws of physics are the same for all observers in uniform motion, and the principle of the constancy of the speed of light, which states that the speed of light in a vacuum is the same for all observers regardless of their relative motion.

4. How does the Special Theory of Relativity impact our understanding of time and space?

The Special Theory of Relativity has revolutionized our understanding of time and space by showing that they are not absolute and can be affected by the motion of objects. It also proposes that time and space are interconnected and can be described as a four-dimensional continuum known as spacetime.

5. What are the practical applications of the Special Theory of Relativity?

The Special Theory of Relativity has several practical applications, including GPS technology, nuclear energy, and particle accelerators. It also helps us understand the behavior of objects at high speeds and in extreme conditions, such as near the speed of light or in the presence of strong gravitational fields.

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