Lorentz Fitzgerald contraction

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SUMMARY

The Lorentz-Fitzgerald contraction hypothesis does not contradict classical motion of rigid bodies, as classical rigid bodies do not exist in the framework of relativity. In special relativity (SR), a rigid body is defined as retaining its shape in its instantaneous rest frame, while the concept of Born rigidity applies specifically to scenarios involving proper acceleration. A Born rigid geodesic congruence can exist in Minkowski spacetime, characterized by zero expansion and shear, but the conditions for achieving Born rigidity are significantly more restrictive than in classical Newtonian physics.

PREREQUISITES
  • Understanding of special relativity (SR) principles
  • Familiarity with the concept of Born rigidity
  • Knowledge of Minkowski spacetime
  • Basic grasp of the Herglotz-Noether theorem
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  • Research the implications of Born rigidity in special relativity
  • Study the Herglotz-Noether theorem and its relevance to rigid body motion
  • Explore the differences between classical and relativistic definitions of motion
  • Examine the concept of geodesic congruences in Minkowski spacetime
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Physicists, students of relativity, and anyone interested in the foundational concepts of motion and rigidity in the context of special relativity.

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Does the lorentz fitzgerald contraction hypothesis contradicts the classical motion of rigid body?
I am not sure but i think it doesn't contradicts the classical motion of rigid body.
 
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There is no such thing as a classically rigid body in relativity. Google and search here for "Born rigidity" for more.
 
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Nugatory said:
There is no such thing as a classically rigid body in relativity. Google and search here for "Born rigidity" for more.
Born rigidity only applies when proper acceleration is involved it has absolutely nothing to do with relative motion without proper acceleration.
 
MeJennifer said:
Born rigidity only applies when proper acceleration is involved

This is not correct. It is perfectly possible to have a Born rigid geodesic congruence. The simplest example is a congruence of parallel inertial worldlines in Minkowski spacetime.
 
PeterDonis said:
This is not correct. It is perfectly possible to have a Born rigid geodesic congruence. The simplest example is a congruence of parallel inertial worldlines in Minkowski spacetime.
Ok then, what is the difference between a Born rigid and a non Born rigid congruence of parallel intertial worldlines in Minkowski spacetime?

If there is no acceleration it is totally useless to talk about something being Born rigid.
 
MeJennifer said:
what is the difference between a Born rigid and a non Born rigid congruence of parallel intertial worldlines in Minkowski spacetime?

The first one exists and the second one doesn't. Every congruence of parallel inertial worldlines in Minkowski spacetime is Born rigid.
 
"Does the lorentz fitzgerald contraction hypothesis contradicts the classical motion of rigid body?"
The classical definition of a rigid body, that it retains its shape when moving, is contradicted by special relativity. An SR definition of a rigid body is that it retains its shape in its instantaneous rest system, even while moving. You could look at
arXiv:1105.3899.
 
clem said:
"Does the lorentz fitzgerald contraction hypothesis contradicts the classical motion of rigid body?"
The classical definition of a rigid body, that it retains its shape when moving, is contradicted by special relativity. An SR definition of a rigid body is that it retains its shape in its instantaneous rest system, even while moving. You could look at
arXiv:1105.3899.
What is your definition of moving?

In SR there is no such thing as absolute movement, all movement is relative.
What is not relative is proper acceleration.
 
clem said:
An SR definition of a rigid body is that it retains its shape in its instantaneous rest system, even while moving.

This isn't a good definition as it stands, since, as MeJennifer points out, "moving" has no absolute meaning in relativity.

In relativity, there is no such thing as a "rigid body" in the classical sense, because internal forces between different parts of an object are not instantaneous; they can only be transmitted at the speed of light. The best that can be done in relativity is Born rigidity. The technical definition of Born rigidity is that the congruence of worldlines that describes the body (one worldline for each point in the body) must have zero expansion and shear. Heuristically, this means the distances between different parts of the body are constant. However, the conditions under which this is even possible are quite restrictive, much more so than in Newtonian physics, because of the Herglotz-Noether theorem (which you can look up for more info).
 

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