Big anaconda orbiting the planet

  • Thread starter Thread starter paul-g
  • Start date Start date
  • Tags Tags
    Planet
Click For Summary
SUMMARY

The discussion centers on the orbital mechanics of a hypothetical big anaconda orbiting the planet XYZ-123. The key question is whether the anaconda's orbit remains circular after it folds into a compact shape. The analysis suggests that angular momentum is conserved, leading to the conclusion that the anaconda will begin to move away from the planet, resulting in a non-circular orbit. The equations of motion and energy conservation principles are applied to support this conclusion.

PREREQUISITES
  • Understanding of angular momentum conservation
  • Familiarity with gravitational force equations
  • Knowledge of kinetic and potential energy in orbital mechanics
  • Basic proficiency in algebra and physics equations
NEXT STEPS
  • Study the principles of angular momentum in non-circular orbits
  • Learn about gravitational potential energy and its implications in orbital mechanics
  • Explore the effects of mass distribution on orbital paths
  • Investigate numerical methods for simulating orbital dynamics
USEFUL FOR

Students and enthusiasts of physics, particularly those interested in orbital mechanics and gravitational interactions in celestial bodies.

paul-g
Messages
14
Reaction score
0

Homework Statement


Big anaconda orbiting the planet XYZ-123 in a vertical position (along the radius of the planet and at a constant height). At some point, anaconda folded her in a small bundle. Is its orbit will be circular? He begins to recede from or approach the planet?


2. The attempt at a solution

I know that the anaconda was able to perform the action described in the command have to do some work. It seems to me that it would start by moving away from the planet, but I do not know how to prove it.
 
Physics news on Phys.org
Is angular momentum conserved?
 
There is no information about it, but I think yes.
 
Why not choose some numbers for an example and work out a figure for the angular momentum of the snake stretched out (so going from say, radius r1 to radius r2). Then determine at what radius the compact body would want to orbit with that same angular momentum. Compare this and that. :smile:
 
I thought to write it this way

E_{p}=-\frac{GMm}{r}

F=ma

\frac{GMm}{r^2}=\frac{mv^2}{r}

\frac{mv^2}{2}=\frac{GMm}{2r}

E_{k}=-\frac{E_{p}}{2}

E=E_{k}+E_{p}=\frac{GMm}{2r}-\frac{GMm}{r}

E=-\frac{GMm}{2r}



This applies to the circular orbit, but in our case:

E_{k}=E_{k_{1}}-W

E=E_{k_{1}}-W+E_{p}

How to prove that the orbit is not circular. This is enough? Snake gave up and will be circulated in the orbit of larger radius, or begin to move away from the planet?
 

Similar threads

Replies
1
Views
2K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 7 ·
Replies
7
Views
4K
  • · Replies 2 ·
Replies
2
Views
3K
Replies
6
Views
2K
Replies
1
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
Replies
8
Views
2K
Replies
15
Views
2K