Harmonic Oscillator - Mass With Initial Velocity

In summary, the conversation discusses the force equation for a harmonic oscillator with mass M, spring stiffness k, and displacement x. It is a simple second order differential equation with solutions involving sine and cosine. The initial conditions are then used to solve for A and B, which determine the specific solution for x(t). The equation could potentially be used to model the behavior of a bungee jumper at the end of the rope. However, factors such as gravity and the non-linearity of the bungee must be taken into account.
  • #1
Eugbug
21
0
For a harmonic oscillator with mass M, spring of stiffness k and displacement the force equation is:

-kx = Md2x/dt2

How do you handle the situation and work out a solution for x(t) when the mass has an initial velocity. E.g. a mass dropped onto the spring?
 
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  • #2
It's a pretty simple second order differential equation with sins and coss as it's solutions, you then just solve for x'(0) = initial velocity
 
  • #3
The first thing you do is to solve the DE in the general case, that is without specific initial conditions. You find
x = A cos [itex]\omega[/itex]t + B sin [itex]\omega[/itex]t

in which [itex]\omega[/itex] = [itex]\frac{force per unit x}{mass}[/itex]

and A and B are arbitrary constants. It is these whose values accommodate the initial conditions. So, suppose you knew that at t = 0, x = 0 and [itex]\frac{dx}{dt}[/itex] = v[itex]_{0}[/itex].

Substituting x = 0, t = 0 into the general solution gives

x = B sin [itex]\omega[/itex]t. [A = 0.]

So [itex]\frac{dx}{dt}[/itex] = B [itex]\omega[/itex] cos [itex]\omega[/itex]t

Now imposing [itex]\frac{dx}{dt}[/itex] = v[itex]_{0}[/itex] when t = 0

v[itex]_{0}[/itex] = B [itex]\omega[/itex] so B =[itex]\frac{v}{\omega}[/itex]

Putting in this value for B, we finally have

x = [itex]\frac{v}{\omega}[/itex] sin [itex]\omega[/itex]t.
 
  • #4
Thanks for the answer Philip!

I was reading a question about Bungee ropes last night on Webanswers and this equation could probably go some way towards modeling the behavior of a jumper when they have reached the end of the rope which then starts to stretch.
 
  • #5
Yes, it would be an excellent model. You've got to be careful over gravity, which displaces the equilibrium position below the point at which the bungee starts to stretch, but I doubt if this will cause too many problems for you.

And – not something to worry about yet – the bungee won't obey Hooke's law perfectly.
 

What is a harmonic oscillator?

A harmonic oscillator is a system that experiences a restoring force proportional to its displacement from its equilibrium position. It follows a sinusoidal pattern of motion and has a constant period, regardless of the amplitude of the oscillation.

What is the equation for a harmonic oscillator?

The equation for a harmonic oscillator is F = -kx, where F is the restoring force, k is the spring constant, and x is the displacement from equilibrium.

What is the significance of initial velocity in a harmonic oscillator?

The initial velocity in a harmonic oscillator determines the amplitude and phase of the oscillation. It also affects the total energy of the system.

How does mass affect a harmonic oscillator?

The mass of the system affects the period of the oscillation. A larger mass will result in a longer period, while a smaller mass will result in a shorter period. However, the amplitude and frequency of the oscillation will remain constant.

What is the relationship between potential and kinetic energy in a harmonic oscillator?

In a harmonic oscillator, the potential energy is at its maximum when the displacement is at its maximum, and the kinetic energy is at its maximum when the displacement is at its equilibrium position. As the mass oscillates, the potential and kinetic energies alternate, but the total energy remains constant.

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