erobz
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Yeah, I agree (I think we all do now) that is the reality of an accelerating cart. If a wall is moving at constant velocity it will have displacement ## \delta x \approx v \delta t##. If the wall is accelerating at constant ##a##, then it has displacement ## \delta x \approx v \delta t + \frac{1}{2}a (\delta t)^2 ##. So, presumably more work will be done on the particle per unit ## \delta t ## in the case where the wall is accelerating assuming ##\delta t## doesn't strongly depend on ##a##.user079622 said:Cart that accelerate, in front produce force on air particle, particle with same force push back on the cart.
This additional force dont exist in constant velocity case.
Isnt it?
The devil here is in the details of the unsteady terms I crossed out in post no 225. You can work on the equations I provided (with now some hopefully sensible examples), make some different assumptions and pull the levers. That will be the same thing I am doing. Perhaps start with a constant velocity control volume and try to make some assumptions about the flow-mass acceleration inside it and see what happens to the equations.
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