Simple Harmonic Motion at Relativistic Speeds

Click For Summary
The discussion centers on the implications of applying Simple Harmonic Motion (SHM) principles at relativistic speeds. It highlights that the standard equations for SHM, such as acceleration being proportional to displacement, do not hold when velocities approach relativistic levels, leading to a different set of complex differential equations. The relativistic extension of SHM can be analyzed using Lagrangian mechanics, revealing that while motion remains bounded and periodic, it becomes anharmonic due to time dilation effects. The period of motion increases with amplitude, and curvature is more pronounced at turning points. Understanding these dynamics is crucial for accurately describing motion in relativistic contexts.
Washer101
Messages
1
Reaction score
0
On The Student Room I saw a couple of guys looking at whether the rules for Simple Harmonic Motion at non-relativistic speeds (e.g. a = -w2y and so on) would work if the maximum velocity of the particle hits relativistic speeds.

Many Thanks
W101
 
Physics news on Phys.org
No, you get a different set of differential equations whose non-linearity makes them difficult to solve. And that's all I know about it.
 
Washer101 said:
On The Student Room I saw a couple of guys looking at whether the rules for Simple Harmonic Motion at non-relativistic speeds (e.g. a = -w2y and so on) would work if the maximum velocity of the particle hits relativistic speeds.

Many Thanks
Have a look at
Relativistic (an)harmonic oscillator
Moreau, William; Easther, Richard; Neutze, Richard
American Journal of Physics, Volume 62, Issue 6, pp. 531-535 (1994).

The relativistic extension of one-dimensional simple harmonic motion is developed in the Lagrangian formalism. The relativistic equations of motion are derived and solved analytically. The motion with respect to proper time is analyzed in terms of an effective potential energy. While the motion remains bounded and periodic, the effect of time dilation along the world line is to cause it to become anharmonic with the period increasing with amplitude and the curvature concentrated at the turning points.
 
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##...

Similar threads

  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 7 ·
Replies
7
Views
4K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 20 ·
Replies
20
Views
2K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 14 ·
Replies
14
Views
2K
  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 11 ·
Replies
11
Views
3K
  • · Replies 17 ·
Replies
17
Views
3K