Conservation of energy - rocket hovering above moon

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Discussion Overview

The discussion revolves around the conservation of energy in the context of a rocket hovering above the moon. Participants explore the energy transformations involved when the rocket burns fuel to maintain its position, considering gravitational potential energy, chemical energy, and kinetic energy. The scope includes theoretical reasoning and conceptual clarification regarding energy conservation principles.

Discussion Character

  • Exploratory, Technical explanation, Conceptual clarification, Debate/contested

Main Points Raised

  • One participant outlines the initial and final energy states of the rocket and moon, questioning where the additional kinetic energy of the moon comes from if energy is conserved.
  • Another participant suggests that the exhaust from the rocket hitting the moon prevents it from moving towards the rocket, implying a loss of potential energy from the fuel.
  • A similar example of a helicopter hovering is presented, noting that the Earth would also move slightly towards the helicopter, although this effect is often ignored.
  • One participant reiterates the initial energy and final energy equations, emphasizing the need to account for the kinetic energy of both the rocket and moon, as well as the exhaust.
  • Concerns are raised about the assumption that gravitational potential energy remains constant, given that the mass of the rocket changes as fuel is burned.

Areas of Agreement / Disagreement

Participants express differing views on the implications of energy conservation in this scenario, with no consensus reached on how to account for the kinetic energy of the moon or the effects of the exhaust. The discussion remains unresolved regarding the additional terms needed in the energy equations.

Contextual Notes

Participants highlight the changing mass of the rocket and the potential energy associated with the fuel, indicating that assumptions about energy conservation may depend on these factors. The discussion also reflects on the complexities of analyzing energy transformations in a non-inertial frame.

bob900
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Suppose a rocket is hovering above the moon at a constant height, burning just enough propellant to stay at that height, and not move upwards or downwards.

Viewed from an inertial frame, we have. Initial energy (just before ignition) :

1. Gravitational potential energy between rocket and the moon = I1
2. Chemical energy stored in fuel = I2


Assume kinetic energies of rocket and moon are both 0 initially.

----

Final energy:

1. Gravitational potential energy between rocket and the moon = F1
2. Kinetic energy (or heat) of the burning propellant = F2
3. Kinetic energy of the rocket = F3
4. Kinetic energy of the moon (it is gravitationally accelerated towards the rocket) = F4

If there is to be conservation of energy, (I1+I2) should equal (F1+F2+F3+F4).

But I2 = F2 + F3, because chemical energy of the fuel is converted into kinetic energy of the rocket and of the propellant. And since the rocket is still hovering at the same distance from the moon, I1 = F1.

So where does the additional term, F4 come from? Is energy conserved?
 
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1,When the exhaust hits the surface of moon, it will prevent moon moving toward the rocket;
2,The mass of rocket continues to decrease, the lost part of fuel will lose its potential energy ;
3,Another better example similar:
A helicopter hovering aloft in the atmosphere of the Earth ,the airflow moving downwards will diffuse in the open air but not hit the surface of the earth.
It's sure the Earth will move towards the helicopter with a extremely tiny velocity.
Unfortunately analysts used to ignore this point.
 
Last edited:
bob900 said:
Suppose a rocket is hovering above the moon at a constant height, burning just enough propellant to stay at that height, and not move upwards or downwards.

Viewed from an inertial frame, we have. Initial energy (just before ignition) :

1. Gravitational potential energy between rocket and the moon = I1
2. Chemical energy stored in fuel = I2


Assume kinetic energies of rocket and moon are both 0 initially.

----

Final energy:

1. Gravitational potential energy between rocket and the moon = F1
2. Kinetic energy (or heat) of the burning propellant = F2
3. Kinetic energy of the rocket = F3
4. Kinetic energy of the moon (it is gravitationally accelerated towards the rocket) = F4

If there is to be conservation of energy, (I1+I2) should equal (F1+F2+F3+F4).

But I2 = F2 + F3, because chemical energy of the fuel is converted into kinetic energy of the rocket and of the propellant. And since the rocket is still hovering at the same distance from the moon, I1 = F1.

So where does the additional term, F4 come from? Is energy conserved?

If you manage to let the exhaust not hit the moon, then the kinetic energy of the moon comes from the fact that both the moon and the rocket start to move (the rocket is hovering at constant distance from the moon), so the kinetic energy of the exhaust will be less in the frame where the moon was initially at rest.
 
willem2 said:
If you manage to let the exhaust not hit the moon, then the kinetic energy of the moon comes from the fact that both the moon and the rocket start to move (the rocket is hovering at constant distance from the moon), so the kinetic energy of the exhaust will be less in the frame where the moon was initially at rest.

Right, viewed in the rest frame, both rocket and moon start to move with kinetic energies R and M respectively. There's also the kinetic energy of the exhaust, E.

After all the fuel has been burned, the Δkinetic energy = R+M+E, and Δpotential energy = -C where C is the potential energy of the fuel at the start. So by conservation of energy,

R+M+E = C (1)

But... Since the exhaust doesn't hit the moon, C is converted into only R and E, so

C = R+E (2)

So there's a contradiction, between (1) and (2). Seems like there should be an additional term on the right hand side of (1), equal to M. But where does it come from?
 
bob900 said:
I1 = F1.
This is wrong. The mass of the rocket has changed.
 

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