Oscillating springs in relativistic time frame

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Homework Help Overview

The discussion revolves around the dynamics of two identical spring and mass oscillators in a relativistic context. Participants are tasked with calculating angular frequency, period, and analyzing the effects of relativistic transformations on the system as observed from different frames of reference.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the calculations of angular frequency and period for oscillators, and discuss the effects of damping on amplitude. There is confusion regarding how to transform the force law for the oscillators into a second observer's frame, with questions about inertia and stretch in that frame.

Discussion Status

Several participants are actively questioning the transformations needed for the spring's force law and the implications of relativistic effects on mass and displacement. There is an ongoing exploration of how to apply the concepts of length contraction and relativistic mass to the problem, with no clear consensus yet on the correct approach.

Contextual Notes

Participants express uncertainty about the transformation of forces and the treatment of non-uniform acceleration in the context of special relativity. There are references to specific equations and concepts that may require clarification or further exploration.

Samuelriesterer
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1. The problem statement, equations, and work done:

[A]
Two identical spring and mass oscillators are set in motion in perpendicular directions. The masses are each 4.0 kg and the spring constants are 196 N/m.

[1] Calculate the angular frequency and the period of the oscillators.

##\omega = \sqrt{\frac{k}{m}} = .143 rad/sec##

##T = \frac{2\pi}{\omega} = 43.938 s##

[2] The oscillators are damped such that the amplitude decreases by 20% in 140 seconds. Determine the coefficient in the damping force (b in F = -bv) and the time constant (τ) for the energy decay ( E= Eo e-t/τ)

##A_{\% decrease\hspace{1 mm}per\hspace{1 mm}cycle} = \frac{A_{total\hspace{1 mm}decrease} \hspace{1 mm}X\hspace{1 mm}time}{T} = \frac{.20 X 140 s}{43.938 s} = 63.726 \%##

##A = A_0 - A_{\%decrease\hspace{1 mm}per\hspace{1 mm}cycle} = A_0 e^{\frac{-bT}{2m}} →##

##1 - .63726 = 1\hspace{1 mm}X\hspace{1 mm}e^{\frac{-b(43.938 s)}{2(4 kg)}} →##

##b = .184636 kg/s##

##\tau = \frac{m}{b} = \frac{.18636 kg/s}{4 kg} = 21.66 s##

[3] A second observer passes at 0.6c, traveling in the direction one of the oscillators moves. Write the force law for the spring in the frame where one end is stationary (as in parts 1 and 2). Then transform this to the second observer's frame by finding the inertia and stretch in the second frame. Do this twice, once for each oscillator.

##F_{stationary\hspace{1 mm}reference} = ma = -k\Delta x##

<This is where I am confused. How to I convert this to second observer's frame by finding the inertia and stretch?>

[4] Using your force law in [3], derive the expressions for the angular frequency and the period of the oscillators in the second frame.

[5] Now compare the periods you calculated to the result of a time dilation calculation
 
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Samuelriesterer said:
<This is where I am confused. How to I convert this to second observer's frame by finding the inertia and stretch?>
I'm no expert on relativity, but I would guess the inertia would be increased according to the relativistic mass formula, and stretch reduced according to the distance contraction.
 
I think I get it. So Delta x would shrink due to the length dilation and k, which represents the inertia?, would expand; but what equation represents this k expansion?
 
Samuelriesterer said:
I think I get it. So Delta x would shrink due to the length dilation
contraction. Dilation would be lengthening, as in time dilation.
Samuelriesterer said:
k, which represents the inertia?, would expand
No, inertia means mass. m increases according to the usual equation. Use the spring equation to find how these x and m changes affect k.
 
Would it be:

##\vartriangle x’ = \frac{\vartriangle x}{\gamma}##
##m’ = \gamma \vartriangle x##
##k = \frac{m’ a}{\vartriangle x’}##
 
Samuelriesterer said:
Would it be:

##\vartriangle x’ = \frac{\vartriangle x}{\gamma}##
##m’ = \gamma \vartriangle x##
##k = \frac{m’ a}{\vartriangle x’}##

Aren't you supposed to use the transformations of forces for different IRF's?

##F'_x = ...##

##F'_y = ...##

As well as the length contraction formula.
 
Last edited:
PeroK said:
Aren't you supposed to use the transformations of forces
Probably. It says 'the force law' which suggests it's the ##F=k\Delta x## equation that's to be transformed. I was looking at ##ma = k\Delta x##.
Samuelriesterer said:
##m’ = \gamma \vartriangle x##
Shouldn't there be an m on the right, not an x?
 
haruspex said:
Probably. It says 'the force law' which suggests it's the ##F=k\Delta x## equation that's to be transformed. I was looking at ##ma = k\Delta x##.

Shouldn't there be an m on the right, not an x?

Oh yes, that was a mistake. An m on the right.
 
Can anybody shed some light on finding the inertia and stretch in the second frame.
 
  • #10
Samuelriesterer said:
Can anybody shed some light on finding the inertia and stretch in the second frame.
You wrote ##k = \frac{m’ a}{\vartriangle x’}## (I guess you meant ##k' = \frac{m’ a}{\vartriangle x’}##), but you also need to transform a.
You already posted an equation for transforming the extension. Do you have doubts about it?
 
  • #11
I have a lot of doubts about physics. But I didn't think you could transform non uniform acceleration..
 

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