Simple Harmonic Motion and acceleration

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Discussion Overview

The discussion centers on the relationship between maximum acceleration, amplitude, and frequency in simple harmonic motion (SHM). Participants explore how changes in frequency affect amplitude and maximum acceleration, considering both theoretical implications and practical examples.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions whether amplitude (A) is inversely proportional to frequency squared, suggesting that doubling the frequency might reduce amplitude by a factor of 4, while holding maximum acceleration (amax) constant.
  • Another participant asserts that frequency, amplitude, and phase are independent quantities, indicating that changes in frequency do not necessitate a constant maximum acceleration.
  • A different viewpoint states that if frequency is doubled, maximum acceleration is quadrupled, implying a direct relationship between frequency squared and maximum acceleration.
  • Participants discuss a practical example involving a ruler suspended between supports, questioning how changes in support position that double frequency would affect amax and A according to the equation.
  • One participant introduces the concept of maximum spring potential energy conservation, suggesting that increasing stiffness (k) by moving supports closer would require a decrease in maximum displacement (xmax) to conserve energy.
  • There is a query about whether SHM equations can still apply in the context of the ruler example, indicating uncertainty about the applicability of SHM principles in modified conditions.
  • Another participant notes that the ratio amax/A would quadruple if frequency is doubled, but emphasizes that more information is needed to determine the specific relationship between amax and A.

Areas of Agreement / Disagreement

Participants express differing views on the relationships between frequency, amplitude, and maximum acceleration, with no consensus reached on how these variables interact under changing conditions.

Contextual Notes

Participants acknowledge that the discussion involves multiple models and interpretations of the equations governing SHM, as well as practical considerations that may affect the theoretical relationships.

Jimmy87
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Hi, I have a few questions relating to the equation for maximum acceleration for SHM:

amax = A (2 x pi x f)^2 where amax = max. acceleration, A = amplitude, f = frequency.

How are these variables supposed to be interpreted when you relate them to each other. For example, is A inversely proportional to the frequency squared as the equation implies? So, if you doubled the frequency, would the amplitude go down by a factor of 4? This reasoning would involve holding amax constant which itself depends on A so I'm not sure whether what I said is justified. What happens to the variables in the equation if you do increase the frequency?

Thanks for any help given!
 
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The frequency, amplitude and phase of an harmonic oscillator are independent quantities. They can vary from system to system and if the oscillator is free (no damping or driving force) they are fixed for ever. There is no reason why in you equation if, for example, you double the frequency the maximum acceleration should remain the same.
 
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Acceleration is proportional to A, and it is proportional to the square of the frequency, so if the frequency is doubled the maximum acceleration is quadrupled.

Chris
 
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Einj said:
The frequency, amplitude and phase of an harmonic oscillator are independent quantities. They can vary from system to system and if the oscillator is free (no damping or driving force) they are fixed for ever. There is no reason why in you equation if, for example, you double the frequency the maximum acceleration should remain the same.

Thanks for the replies. Take, for example, a ruler suspended between two supports. You hang a mass in the middle and set it oscillating. You can increase the frequency by moving the two supports closer (essentially making the ruler shorter). Say that you move the supports closer such that the frequency has doubled what would happen to amax and A in this situation according to the equation?
 
That is a different set of equations. The maximum spring potential energy is conserved even when you change the ruler. ##PE_{max}=\frac{1}{2}kx^2_{max}## where k is the spring constant for Hooke's law. When you move your supports, you stiffin the spring and k increases. That means ##x_{max}## has to decrease for energy to be conserved.

Chris
 
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kq6up said:
That is a different set of equations. The maximum spring potential energy is conserved even when you change the ruler. ##PE_{max}=\frac{1}{2}kx^2_{max}## where k is the spring constant for Hooke's law. When you move your supports, you stiffin the spring and k increases. That means ##x_{max}## has to decrease for energy to be conserved.

Chris

That's interesting, thank you. Can you still apply simple harmonic motion equations to this? Surely it is still undergoing simple harmonic motion is it not?
 
Jimmy87 said:
Thanks for the replies. Take, for example, a ruler suspended between two supports. You hang a mass in the middle and set it oscillating. You can increase the frequency by moving the two supports closer (essentially making the ruler shorter). Say that you move the supports closer such that the frequency has doubled what would happen to amax and A in this situation according to the equation?
According to the equation, the ratio amax/A would quadruple if the frequency is doubled. But more information is required before we could say whether amax quadrupled, or A was reduced by a factor of 4, or amax doubled while A was halved, etc.
 
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