Conceptual Question About Vertical Spring System

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Homework Help Overview

The discussion revolves around a vertical spring system with a mass attached, exploring the dynamics of oscillation and equilibrium. Participants examine the relationships between gravitational force, spring force, and energy conservation in different scenarios of mass release and equilibrium positioning.

Discussion Character

  • Conceptual clarification, Assumption checking, Mixed

Approaches and Questions Raised

  • Participants discuss the implications of defining equilibrium points and the effects on force balance equations. Questions arise regarding the consistency of stretch in the spring under different conditions of release and lowering.

Discussion Status

There is an active exploration of the relationships between forces and energy in the system. Some participants provide insights into the energy equations and the effects of different release methods, while others seek clarification on the assumptions made regarding stretch and equilibrium.

Contextual Notes

Participants are navigating the complexities of energy conservation and force balance in the context of a spring-mass system, with specific attention to how different initial conditions affect the outcomes. The discussion reflects a mix of theoretical considerations and practical implications of the spring's behavior.

lvslugger36
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Suppose there is a spring with a mass m attached to it, and it is released from rest. It will oscillate, starting from a certain point y0, going back to equilibrium and then down to let's say y2. Let's say in the first case, I call y1 my x = 0 point for the spring. When it passes equilibrium, is it not true that mg = kx since the acceleration is zero? However, let's repeat the case for which i will call the equilibrium point the x=0 for the spring. Now, from energy we have: mgx = kx^2/2. This means that 2mg = kx. How can this be possible?
 
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lvslugger36 said:
Suppose there is a spring with a mass m attached to it, and it is released from rest. It will oscillate, starting from a certain point y0, going back to equilibrium and then down to let's say y2. Let's say in the first case, I call y1 my x = 0 point for the spring. When it passes equilibrium, is it not true that mg = kx since the acceleration is zero?
yes
However, let's repeat the case for which i will call the equilibrium point the x=0 for the spring. Now, from energy we have: mgx = kx^2/2. This means that 2mg = kx. How can this be possible?
You are mixing apples and oranges. For the 2nd case, the mass has kinetic energy at x= 0 (point y1). You are better off using the energy equations from the starting point y0. Then from the 2 'no speed' positions (at release and at the end point when the mass comes to a temporary stop), then mg(2x) = 1/2(k(2x)^2 , k = mg/x. Note that the stretch is double the stretch if the mass was slowly lowered to its final at rest position y1.
 
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Thanks for your help; that's brilliant. However, wouldn't the stretch be the same even if it was lowered? For the first equation: x = mg/k. For the one slowly lowered, since the forces are balanced once it reaches equilibrium, shouldn't the stretch be x = mg/k also?
 
lvslugger36 said:
However, wouldn't the stretch be the same even if it was lowered? For the first equation: x = mg/k. For the one slowly lowered, since the forces are balanced once it reaches equilibrium, shouldn't the stretch be x = mg/k also?
Yes. When it is slowly lowered with your hand applying an external force, then you release it once it reaches it's equilibrium position, the stretch is mg/k. Or, if it is damped due to friction, it will ultimately, after oscillating back and forth a few times, settle to that same point, x =mg/k.
 

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