Conservation of Energy and Angular Momentum in Inverse Cube Force Problems

In summary, this problem asks for an equation that explains the motion of a particle as a function of time, given an impulse given in the opposite direction to the particle's velocity. The equation that is given is a first-order equation that concerns the angular momentum of the particle.
  • #1
Spanky1996
7
0

Homework Statement


I'm given a force law is [tex] F = \frac{-k}{r^3} [/tex] and that initially, the particle is in a circular orbit the particle is given an impulse parallel and in the opposite direction to its velocity find the distance from the center for the particle as a function of time.

Homework Equations



I started with the first integral of motion. We know the energy is conserved because this is central force motion (also know angular momentum is conserved).

The Attempt at a Solution



After taking the time derivative of the first integral of motion I get: [tex] r^3*\frac{dr^2}{dt^2} = \frac{L^2-mk}{m} [/tex]

I'd then have to solve that and I'd technically have my answer I think? I guess I'd have to analyze its form and figure out what it's doing when it's going slower than a certain threshold to find it's motion after the impulse is given? Is there possibly a simpler way to approach this problem? Thanks.
 
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  • #2
Hello and welcome to PF!
Spanky1996 said:
After taking the time derivative of the first integral of motion I get: [tex] r^3*\frac{dr^2}{dt^2} = \frac{L^2-mk}{m} [/tex]
Can you show the steps you used to arrive at this? Note that the units don't match for the left and right sides of the equation. Does ##L## represent angular momentum? Did you mean to write ##\frac{d^2r}{dt^2}## instead of ##\frac{dr^2}{dt^2}##?
 
  • #3
Oops yes, that is the 2nd time derivative of r(t)

[tex] E = \frac{1}{2}m(\frac{dr}{dt})^2+\frac{L^2}{2mr^2}-\frac{k}{2r^2} [/tex]

take the time derivative of this equation and that is how I got the expression from my previous post. L is the angular momentum, yes.
 
  • #4
Spanky1996 said:
the energy is conserved
So what equation does that give you?
Spanky1996 said:
After taking the time derivative
Why would you do that? That's going in the wrong direction. You want to integrate again.
 
  • #5
Spanky1996 said:
Oops yes, that is the 2nd time derivative of r(t)

[tex] E = \frac{1}{2}m(\frac{dr}{dt})^2+\frac{L^2}{2mr^2}-\frac{k}{2r^2} [/tex]

take the time derivative of this equation and that is how I got the expression from my previous post. L is the angular momentum, yes.
OK. If you take the time derivative of this, you will not quite get what you wrote for the right hand side of your equation in the first post. L2/m does not have the correct units.

But, rather than taking the time derivative of the energy equation, try working with the equation itself. You should be able to manipulate it so that you can integrate it. [as pointed out by haruspex]
 
  • #6
The equation it gives me is the one just above your post I believe.

I suppose you're right I maybe should not take the time derivative. I guess E can be found with the initial conditions. [tex] E = \frac{L^2}{2mr_o^2}-\frac{k}{2r_o^2} [/tex]

from there I have a first-order equation I suppose.
 
  • #7
Spanky1996 said:
I suppose you're right I maybe should not take the time derivative. I guess E can be found with the initial conditions. [tex] E = \frac{L^2}{2mr_o^2}-\frac{k}{2r_o^2} [/tex]

from there I have a first-order equation I suppose.
Yes
 
  • #8
So, TSny and Haruspex I think I've got this one figured out. What if the radial velocity at time = 0 isn't 0? What if the particle is given some type of kick outward or inward? Would I then want to turn it into a 2nd order D.E. so I could take that initial condition into account? Or is there a better way?
 
  • #9
Spanky1996 said:
So, TSny and Haruspex I think I've got this one figured out. What if the radial velocity at time = 0 isn't 0? What if the particle is given some type of kick outward or inward? Would I then want to turn it into a 2nd order D.E. so I could take that initial condition into account? Or is there a better way?
I don't think it would change things much. You would just need to account for an adjustment in the angular momentum. Unless I'm overlooking something.
 
  • #10
TSny said:
I don't think it would change things much. You would just need to account for an adjustment in the angular momentum. Unless I'm overlooking something.
If the impulse was purely radial the angular momentum wouldn't change right? Shoot, have I done something wrong with the original problem since the angular momentum would change? I plugged it into the integral and treated as a constant. I'm not sure if there is a mistake there or not now...
 
  • #11
Spanky1996 said:
have I done something wrong with the original problem since the angular momentum would change?
Hard to say without seeing your work. You are not given the size of the impulse.
Note that it says opposite to velocity direction. It ought to add that the result is reduced speed. This is important in the nature of the solution.
 

1. What is the Inverse Cube Force Law?

The Inverse Cube Force Law is a physical law that describes the relationship between the magnitude of a force and the distance between two objects. It states that the force between two objects is inversely proportional to the cube of the distance between them.

2. How is the Inverse Cube Force Law different from the Inverse Square Force Law?

The Inverse Cube Force Law is similar to the Inverse Square Force Law, but the former takes into account the three-dimensional nature of space. In the Inverse Square Force Law, the force decreases with the square of the distance, while in the Inverse Cube Force Law, it decreases with the cube of the distance.

3. What are some examples of the Inverse Cube Force Law?

Some examples of the Inverse Cube Force Law include the gravitational force between two objects, the electrostatic force between two charged particles, and the magnetic force between two magnetic dipoles.

4. How is the Inverse Cube Force Law derived?

The Inverse Cube Force Law is derived from the universal law of gravitation, which states that the force between two objects is directly proportional to the product of their masses and inversely proportional to the square of the distance between them. By accounting for the three-dimensional nature of space, the Inverse Cube Force Law can be derived.

5. What are the practical applications of the Inverse Cube Force Law?

The Inverse Cube Force Law is used in various fields of science and engineering, including astronomy, electromagnetism, and fluid dynamics. It helps us understand the behavior of objects in space and how forces act on them. It also aids in the design and development of technologies, such as satellites and spacecraft, that rely on the laws of gravity and electromagnetism.

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