Amplitude and Vibrations in Springs

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SUMMARY

The discussion focuses on the analysis of a mass-spring system undergoing simple harmonic motion (SHM) with specific parameters: an amplitude of 0.13m, mass of 85g, and a spring constant of 55N/m. The maximum elastic potential energy (Ee) is calculated to be 0.46J. The speed of the mass at a position of 7.4cm from the equilibrium point is determined to be approximately 2.78m/s, while the maximum speed is calculated to be 3.3m/s using energy conservation principles. The participants emphasize the importance of energy equations in solving for speed at various positions.

PREREQUISITES
  • Understanding of simple harmonic motion (SHM)
  • Familiarity with energy conservation principles in mechanical systems
  • Knowledge of elastic potential energy (Ee) and kinetic energy (Ek) equations
  • Ability to manipulate equations involving mass, spring constant, and displacement
NEXT STEPS
  • Study the derivation and application of the equations for elastic potential energy (Ee = ½k(Δx)²) and kinetic energy (Ek = ½mv²)
  • Learn about the relationship between amplitude, maximum speed, and energy in SHM
  • Explore the concept of damping in oscillatory systems and its effects on amplitude and energy
  • Investigate the use of energy conservation to solve complex SHM problems
USEFUL FOR

Students studying physics, particularly those focusing on mechanics and oscillatory motion, as well as educators seeking to enhance their understanding of energy conservation in mass-spring systems.

RoyceB
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Homework Statement


The amplitude of vibration of a mass on a horizontal spring experiencing SHM is = 0.13m. The mass is 85g and the force constant is 55N/m. a) What is the maximum elastic potential energy of the system. b) Find the speed of the mass when it's position is x = 7.4cm from the equilibrium point. c) What is it's maximum speed?

A = 0.13m
m = 0.085Kg
k = 55N/m
Δx = 0.074m

Homework Equations


Ee = ½k(Δx)2
Ek = ½mv2
Fx = -kΔx
T = 2π√(m/k)
Fc = mv2 / A[/B]

The Attempt at a Solution



a)

For this I simply used the Ee equation and solved for it. I used 0.13m as the amplitude as I figured this is the furthest the spring could stretch out.
Ee = ½k(Δx)2[/B]
Ee = ½55N/m(0.13)2
Ee = 0.46J

b)

This one I solved for T, used the force equation and the Fc equation to solve for speed.

T = 2π√(m/k)
T = 2π√(0.086/55)
T = 0.25s

Fx = -kΔx
Fx = -55(0.074)
Fx = 4.07N

Fc = mv2 / A
Fc = (0.086)v2 / 0.13
v = 2.5m/s

c) I am kind of lost and thought of making Ee = Ek but would like some assistance.

Also if you could proof check my answers and tell me any errors as I assume my entire b) part maybe wrong.
 
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Your answer for b is a bit off. Probably rounding errors. You could retain more digits during the calculation, but I would solve it using energy. How much elastic PE is lost in going from max extension to 7.4cm.?
RoyceB said:
Fc = (0.086)v2 / 0.13
v = 2.5m/s

c) I am kind of lost and thought of making Ee = Ek but would like some assistance.
If you mean that the max of the one equals the max of the other, yes. Can you turn that into an equation for the max speed?
 
haruspex said:
Your answer for b is a bit off. Probably rounding errors. You could retain more digits during the calculation, but I would solve it using energy. How much elastic PE is lost in going from max extension to 7.4cm.?

If you mean that the max of the one equals the max of the other, yes. Can you turn that into an equation for the max speed?

Well for b what if I made Ee = Ek' + Ee' and if Ee on the left side is equilibrium then the it could equal and I could move the other one over and solve for that point. Basically making Ek = Ee.

For c if it is at it's furthest point and highest speed could it be Ee = Ek but at a greater distance for x, like the 0.13m?
 
RoyceB said:
Well for b what if I made Ee = Ek' + Ee' and if Ee on the left side is equilibrium then the it could equal and I could move the other one over and solve for that point. Basically making Ek = Ee.

For c if it is at it's furthest point and highest speed could it be Ee = Ek but at a greater distance for x, like the 0.13m?
Since you have not defined exactly what you mean by those different energies, I cannot be sure whether you have that right.
It cannot be both at its furthest point and highest speed. When the one is max the other is min. Maybe that's not what you meant.

How about you just post attempts using what you wrote?
 
So for c I decided at it's highest speed, Ee could equal 0 and for the other side I have Ee at it's highest and Ek = 0 so I ended up with.
Ee = Ek
½mv2 = ½k(Δx)2
½(0.085)v2 = ½(0.13)2(55)
v = 3.3m/s

b)

I made Ee + Ek = Ee' + Ek' and for the beginning I had it equal zero for both when it is not moving so I ended up with.
0 = Ee' + Ek'

Ee = -Ek
½mv2 = ½k(Δx)2
½(0.085)v2 = ½(55)(Δ0.074)2
v = 1.88m/s

Is that what you mean and it is similar for both of determining the energies.
 
Actually how about this for it.

a)
Ee = 0.46J

b)

Ee + Ek = Ee (max)
Ee (max) - Ee (at x = 0.074m) = Ek
½(55)(0.13)2 - ½(55)(0.074)2 = ½(0.085)(v2)
v = 2.78m/s

c)

Ek = Et
½mv2 = Et
½(0.085)(v2) = 0.46J
v = 3.3m/s
 
RoyceB said:
Actually how about this for it.

a)
Ee = 0.46J

b)

Ee + Ek = Ee (max)
Ee (max) - Ee (at x = 0.074m) = Ek
½(55)(0.13)2 - ½(55)(0.074)2 = ½(0.085)(v2)
v = 2.78m/s

c)

Ek = Et
½mv2 = Et
½(0.085)(v2) = 0.46J
v = 3.3m/s
Looks good.
 

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