Acceleration & Special Relativity: Explained

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SUMMARY

The discussion centers on the principles of Special Relativity (SR) and the implications of acceleration on relative motion. It clarifies that SR operates within inertial frames, which do not experience acceleration, and emphasizes that acceleration does not directly affect the Lorentz transformations, length contraction, or time dilation equations. The key distinction is that the person in the rocket experiences acceleration during their turnaround, while the person on Earth remains in an inertial frame. Understanding these concepts is crucial for grasping the nuances of SR.

PREREQUISITES
  • Understanding of Special Relativity principles
  • Familiarity with inertial and non-inertial frames
  • Basic knowledge of Lorentz transformations
  • Concept of acceleration and its effects in physics
NEXT STEPS
  • Study the Lorentz transformations in detail
  • Explore the concept of inertial frames versus non-inertial frames
  • Learn about General Relativity and its relation to gravitational effects
  • Investigate Gravitational Time Dilation and its mathematical implications
USEFUL FOR

Students of physics, educators teaching relativity, and anyone interested in the foundational concepts of Special Relativity and its applications in modern physics.

delsaber8
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So my question arises from the whole time dilation thought experiment where one person stays on Earth the other speeds off in a rocket at near light speed. Upon return of course the one in the rocket is younger, etc. The reason I bring this up is how do we determine who is actually moving, without an acceleration. I thought you need a force to determine the relative motion and since all the SR equations seem to only focus on velocity how do we know it isn't simply the Earth moving away from the rocket ship. I mean I'm sure something explains this, but I'm just slightly confused where and how it is incorporated. I also figure that I should add, my knowledge of special relativity is very elementary as I have never studied the theory in-depth.
 
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Someone had to turn around in order for them to compare times. The one turning around performed an acceleration.
 
Special Relativity does include consideration of acceleration. And the way you know you are accelerating is if there is a net force acting on you. So the guy in the rocket is the one who experiences the acceleration, while the guy back on Earth does not experience acceleration.

Chet
 
delsaber8 said:
So my question arises from the whole time dilation thought experiment where one person stays on Earth the other speeds off in a rocket at near light speed. Upon return of course the one in the rocket is younger, etc. The reason I bring this up is how do we determine who is actually moving, without an acceleration. I thought you need a force to determine the relative motion and since all the SR equations seem to only focus on velocity how do we know it isn't simply the Earth moving away from the rocket ship. I mean I'm sure something explains this, but I'm just slightly confused where and how it is incorporated. I also figure that I should add, my knowledge of special relativity is very elementary as I have never studied the theory in-depth.

Special relativity, like Newtonian mechanics, works only in inertial frames. Inertial frames, by definition, do not accelerate. A non-exhaustive but hopefully illuminating requirement for a frame to be inertial is that an accelerometer, placed at constant coordinates within the frame, reads zero.

The relative acceleration of any two inertial frames will be zero.

Acceleration does not enter directly into the Lorentz transform, length contraction, or time dilation, only the velocity is important.

So - the requirements for special relativity to work are basically similar to the requirements for Newtonian mechanics, except that if you want to take into account gravitational effects, you need to use General Relativity rather than special relativity. It is difficult to say when you can neglect GR effects unless you're able to compute them - as a rule of thumb, I'd suggest looking at some of the GR effects with simple formula (like Gravitational Time Dilation) to see if they are significant in the problem.

Acceleration isn't really an issue for SR, except for the part where SR requires that inertial frames do not accelerate.
 
pervect said:
Special relativity, like Newtonian mechanics, works only in inertial frames.

Just like you can do Newtonian mechanics by introducing time dependent coordinate systems by introduction of fictitious forces, you can do SR in coordinates that are not inertial. This is essentially equivalent to being able to describe a Euclidean space with curvilinear coordinates. The space is still Euclidean regardless of the coordinate representation, some things might be obscured by the non-linear coordinate system, but others may appear more tractable. If I use Rindler coordinates in Minkowski space, I am still doing SR. However, this goes beyond what you would typically encounter when studying SR.
 
In an inertial frame of reference (IFR), there are two fixed points, A and B, which share an entangled state $$ \frac{1}{\sqrt{2}}(|0>_A|1>_B+|1>_A|0>_B) $$ At point A, a measurement is made. The state then collapses to $$ |a>_A|b>_B, \{a,b\}=\{0,1\} $$ We assume that A has the state ##|a>_A## and B has ##|b>_B## simultaneously, i.e., when their synchronized clocks both read time T However, in other inertial frames, due to the relativity of simultaneity, the moment when B has ##|b>_B##...

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