Postulates of STR: Light Speed Constant in All Inertial Frames

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In summary, the speed of light is constant in all inertial frames of reference, as defined by the postulates of special relativity. In a thought experiment involving an observer at rest and a spaceship traveling at the speed of light, the observer measures the speed of light to be 3x10^8 m/s. However, due to the effects of time dilation, the astronaut on the spaceship also measures the speed of light to be 3x10^8 m/s, even though he is traveling at a high velocity relative to the observer. This is because the speed of light is always measured to be the same, regardless of the frame of reference. This concept is known as "relativistic velocity addition" and is a key principle
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manimaran1605
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The speed of light is constant in all inertial frames of reference

Imagine a thought experiment, an observer at rest sending a light pulse towards a spaceship, he measures the speed of light to be 3x10^8 m/s, now assume that the spaceship also travels at the speed of light and an astronaut in spaceship also measures the speed of light pulse is 3x10^8 m/s.
my question is according to him both him and light travels at the same speed so actually he could measure the speed of light to be zero (i.e, light pulse is at rest) right?, but according to postulates of special relativity the astronaut also measures the speed of light to be 3x10^8 m/s, how?
 
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Google for "relativistic velocity addition" - speeds do not add the way you're assuming, although the effect is too small to notice in anything in our daily existence.

Also, in the interests of being precise... Your example is physically impossible because no spaceship (or any other massive object) can move at the speed of light. However, we can fix your example just by saying that the spaceship is traveling at, say, 99% of the speed of light and then your question is good.
 
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  • #3
manimaran1605 said:
The speed of light is constant in all inertial frames of reference

Imagine a thought experiment, an observer at rest sending a light pulse towards a spaceship, he measures the speed of light to be 3x10^8 m/s,
Have you thought about how the observer can actually measure the speed of the light pulse that he sent out? Please describe in detail exactly what you have in mind.

manimaran1605 said:
now assume that the spaceship also travels at the speed of light and an astronaut in spaceship also measures the speed of light pulse is 3x10^8 m/s.
As Nugatory pointed, the astronaunt cannot travel at the speed of light, but assuming he is traveling at some lesser speed, how does he measure the speed of the same light pulse?

manimaran1605 said:
my question is according to him both him and light travels at the same speed so actually he could measure the speed of light to be zero (i.e, light pulse is at rest) right?, but according to postulates of special relativity the astronaut also measures the speed of light to be 3x10^8 m/s, how?
That's not an accurate statement of the postulate according to Einstein. Can you look it up and see the difference?
 
  • #4
manimaran1605 said:
my question is according to him both him and light travels at the same speed so actually he could measure the speed of light to be zero (i.e, light pulse is at rest) right?, but according to postulates of special relativity the astronaut also measures the speed of light to be 3x10^8 m/s, how?

Say you are at "rest" in the lab frame and the astronaut is traveling in the "primed" frame at .99c, as Nugatory suggested. If you in the lab frame read the same time on your clock as you read on the astronaut's clock, then you'd be right, it would appear as if the astronaut would read the speed the light to be very close to zero. However, you in the lab frame do not read the same time on both clocks. The astronauts clock according to your frame is running much, much, slower. So slow, in fact, the the very small velocity difference in the speed of light versus the astronauts speed that you observe in the lab frame is actually observed to be exactly the speed of light, c, as observed by the astronaut, whose perception of the transit of time is much slower than yours as measured from your lab frame.
 
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DiracPool said:
Say you are at "rest" in the lab frame and the astronaut is traveling in the "primed" frame at .99c, as Nugatory suggested.
I don't think you meant what you said. I think you meant you are at "rest" in the lab frame and the astronaut is traveling in the lab frame at .99c. You could then say that the astronaut is at "rest" in the "primed" frame and you are traveling at -0.99c in the "primed" frame. Isn't that what you mean?

DiracPool said:
If you in the lab frame read the same time on your clock as you read on the astronaut's clock, then you'd be right, it would appear as if the astronaut would read the speed the light to be very close to zero. However, you in the lab frame do not read the same time on both clocks. The astronauts clock according to your frame is running much, much, slower. So slow, in fact, the the very small velocity difference in the speed of light versus the astronauts speed that you observe in the lab frame is actually observed to be exactly the speed of light, c, as observed by the astronaut, whose perception of the transit of time is much slower than yours as measured from your lab frame.
Here is a spacetime diagram for the lab frame showing you as the thick blue line at rest and the astronaut in red traveling at 0.99c. The light pulse that you send out at time zero is shown as the thin blue line. The dots mark off 1 second increments of time. Notice how the astronaut's clock is running about seven times slower than yours:

attachment.php?attachmentid=72448&stc=1&d=1409058951.png

Now we use the Lorentz Transformation process to transform to the "primed" frame in which the astronaut is at rest and you are traveling at -0.99c but the light pulse is still traveling at c:

attachment.php?attachmentid=72449&stc=1&d=1409058951.png

Notice how in the "primed" frame, it is your clock that is running seven times slower than the astronaut's.

I think it is important for the OP to understand that neither observer is actually measuring the speed of light to be c, rather the speed of light is defined to be c "in all inertial frames of reference".
 

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1. What are the postulates of Special Theory of Relativity?

The postulates of Special Theory of Relativity (STR) are:
1. The laws of physics are the same in all inertial frames of reference.
2. The speed of light in a vacuum is the same for all observers, regardless of their relative motion.

2. How does STR explain the constancy of the speed of light?

According to STR, the speed of light is a fundamental constant in the universe. It is the same for all observers, regardless of their relative motion. This is because the laws of physics, including the laws of electromagnetism, are the same in all inertial frames. This means that the speed of light must be constant in order to satisfy this postulate.

3. What is the significance of the postulate of light speed constancy in all inertial frames?

The postulate of light speed constancy is crucial in understanding the principles of STR. It implies that the speed of light is the maximum speed at which any object or information can travel in the universe. This has profound implications for our understanding of space and time, and has been confirmed by numerous experiments.

4. Can the postulates of STR be verified experimentally?

Yes, the postulates of STR have been extensively tested and verified through various experiments. One of the most famous experiments is the Michelson-Morley experiment, which showed that the speed of light is constant regardless of the direction of the observer's motion. Additionally, many modern technologies, such as GPS, rely on the principles of STR and its postulates.

5. Are the postulates of STR applicable in all situations?

The postulates of STR are applicable in situations where the laws of physics are not affected by acceleration or gravity. This means that they are valid in inertial frames of reference, where there is no acceleration or gravitational force acting on the observer. In situations where these conditions do not hold, more complex theories, such as General Theory of Relativity, are needed to accurately describe the behavior of objects in the universe.

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