Simple harmonic motion of an ideal spring

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SUMMARY

The discussion focuses on the dynamics of simple harmonic motion involving an ideal spring with a spring constant of k=25 N/m and a 1 kg mass. Participants explore the correct application of force equations, specifically F = -kx and F = mg - kx, to determine the maximum extension of the spring and the acceleration of the mass at that point. The correct angular frequency is established as ω = 5 rad/s, and the importance of defining the coordinate system and direction of forces is emphasized to avoid confusion in calculations.

PREREQUISITES
  • Understanding of simple harmonic motion principles
  • Familiarity with Hooke's Law (F = -kx)
  • Knowledge of gravitational force and its impact on oscillating systems
  • Ability to differentiate sinusoidal functions for velocity and acceleration
NEXT STEPS
  • Study the derivation of angular frequency in simple harmonic motion
  • Learn about energy conservation in oscillating systems, including potential and kinetic energy
  • Explore the effects of damping on simple harmonic motion
  • Investigate the relationship between mass, spring constant, and oscillation period
USEFUL FOR

Students studying physics, particularly those focusing on mechanics and oscillatory motion, as well as educators seeking to clarify concepts related to simple harmonic motion and spring dynamics.

  • #31


You have established where x=0 is. Thats fine. However, when you are doing energy questions, what is important is the change in energy, not the absolute value. Thus, can you find out the change in the energy potential? For gravitational potential energy, mass at the top definitely has more GPE than at bottom.

Question here is by how much? It you have already established x= 0, downwards as positive, how much change in GPE is there?

EDIT: For energy, you can conveniently use a new scale or your choice, since it is only the difference that matter.
 
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  • #32


i really don't know what values to use for x and y anymore... it seems as though now I am supposed to change my value for x. why would i start with a certain value for x and then change it halfway through the problem? That's not making any sense to me.
 
  • #33


Okay first up, what is the change height? Just the absolute value will do.
 
  • #34


change in height is 2A idk
 
  • #35


It is 2A. So the change in GPE is mg(2A). We know that the top has more GPE than bottom. And we also know that by conservation of energy, GPE is transformed to another kind of energy at the bottom. What is it?

Equate them together. Then you can find what g/A is.
 
  • #36


i get the equation kxi^2-kxf^2=mg(4A) so I am having the same problem again... if i plug in x=0 for one of the x values it cancels one of the potential energy equations...
 
  • #37


so then -k=mg/A
 
  • #38


You know initially there is no elastic potential energy. Why? Because there is no extension of the spring, x=0. But there is GPE of mg(2A). At the bottom, extension is maximum, EPE= 1/2 k (2A)^2. Does it make sense?

At the bottom, we can define GPE = 0, this can be done since energy is relative.
 
  • #39


We are now comparing absolute value in energy, so there shouldn't be any negative sign.
 
  • #40


yeah that makes sense but i was thinking about it as the spring is in motion... At the top it would be getting ready to "spring" back out... so i do think it would have elastic energy at the top as the spring is oscillating
 
  • #41


Also what is the value of x in the equation E=1/2mv2+1/2kx2
if i plug in zero at x=0 the equation becomes Zero? is it supposed to be?
 
  • #42


If x=0, then yes, there is no kinetic and elastic energy.
 
  • #43


Ok then say we had called the point of equillibrium zero... Then it would have elastic energy at the top.. How is that?
 
  • #44


It still wouldn't have any elastic energy. The x are talking about here is no longer position of the mass vertically.

The x we are talking about here in 1/2 k x^2 is the extension of the spring.

[STRIKE]Imagine if you were to call the centre point of your oscillation zero, the mass will still be accelerating at centre point! This is because, at centre of oscillation the spring is still stretched.[/STRIKE] EDIT: Mistake, at centre point there is no net acceleration, but there is still spring force exerted on mass.

x = -Acos wt + A, x is position. You can define this however you want.

But k=-kx and E = 1/2 kx^2, the x is extension, not position anymore, though there are times where it can be position.
 
  • #45


Just to clarify.. By extension you mean distance away from the center of oscillation?
 
  • #46


Nope. Amount of spring is stretch from its unstretched state.
 
  • #47


Ok so how would you go about calculating that?
 
  • #48


Well, the question will tell you that.

The oscillation is started by hanging and releasing a mass on an unstretched* spring. There you have it, that's your reference.
 
  • #49


Ok so when you hang a mass on the spring..and then let it go.. Theoretically isn't it supposed to rise back up to the original unstretched position? I have a hard time imagining it would do exactly that depending on the mass.
 
  • #50


Yes it will rise back up to the unstretched position, then go back down again.

I don't understand about the depending on mass part. What do you mean depend on mass? The period?
 
  • #51


no I mean if the mass is heavy enough(not so heavy that it deforms the spring)then it wouldn't quite rise back up to that same position..
 
  • #52


pb23me said:
no I mean if the mass is heavy enough(not so heavy that it deforms the spring)then it wouldn't quite rise back up to that same position..

If it doesn't then it's because the spring deformed.
 
  • #53


It will rise back up to the original position, disregarding any dissipative force like air drag, and damping.

Conservation of energy demands that i rise back to the original position.

Edit: mindscape beat me to it...
 
  • #54


thanx for all the help...appreciatcha!:approve:
 

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