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Hi,
I have two very different suggestions for understanding this class of
problems.
1. Use the basic ideas of general relativity in which the "natural",
force-free path in the presence of gravity is falling. Then, if the
rocket is hovering, it is actually accelerating upward. ( This is a
very simplified explanation. )
2. Consider two aircarts connected by a spring. The track runs from
left to right and the spring is initially stretched so the carts would
pull toward each other. If one holds the left cart so that it is
stationary in the lab frame, the right cart accelerates toward it. Now
replace the person holding the left cart with a rocket that keeps the
left cart stationary in the lab frame. (This would require a controller
on the rocket the adjusts the thrust constantly.) The right cart
accelerates to the left and thus gains momentum, balancing the
conservation of momentum equation.
One catch with this type of problem is correctly apply Newton's Third
law to gravity between two masses, but replace gravity with a spring and
the action and reaction become at least somewhat clearer.
Thanks
Roger Haar
U of AZ Physics
Jack Uretsky wrote:
The change in momentum of the gas after it leaves the rocket cannot, at_______________________________________________
leasst in first order, have any effect on the rocket. I don't understand
your remark after the "but".
Regards,
Jack
On Mon, 24 Jul 2006, Marc "Zeke" Kossover wrote:
--- Jack Uretsky <jlu@hep.anl.gov> wrote:
The answer toThis is what I originally thought (and the student, too)
what is getting
upward momentum is, simply, the earth. The added
downward momentum from
the gas is from the gravitational attraction of the
each.
but it leaves out the fact that the rocket does get some
positive momentum as well. The rocket end up upwards from
it's original position, even though it remains the same
distance from the planet.
I advocate keeping it simple and accompanying theSure, but he was wondering about momentum conservation. And
answer with a
diagram showing the gas, the earth, the mutual forces
acting on each, and
nothing else.
I think that he was leading me towards asking the more
vexing question about momentum conservation in a plane with
level flight.
Marc "Zeke" Kossover
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