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#1
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![]() Alan Baker wrote: In article . com, wrote: Jose wrote: The hovering spacecraft has zero horizontal and vertical momentum. It has weight, directed downwards. The engine accelerates mass downward producing an upward force equal in magnitude and opposite in direction to the weight of the spacecraft. This imparts an acceleration to the spacecraft equal in magnitude and opposite in direction from the local acceleration due to gravity. The flying wing has some horizontal momentum which is secondary here, How much? and zero vertical momentum. It also has weight, directed downwards. The wing accelerates mass downward (mass it finds in the air molecules) producing an upward force equal in magnitude and opposite in direction to the weight of the wing (and its presumably attached aircraft. It does so by finding air in front of it, flinging it downwards and forwards (which causes the air in front to try to get out of the way by rising). In the steady state, one can measure high pressure below and low pressure above, but this is just the macroscopic manifestation of the greater number of molecular collisions below, and the lesser number of collisions above. That's what pressure is - we have both agreed on this. The greater number of collisions below imparts an acceleration to the aircraft equal in magnitude and opposite in direction from the local acceleration due to gravity. I agree that lift is a force, exerted on the aircraft by the air, which in steady level flight is equal in magnitude and opposite in direction to the weight of the aircraft. Energy is 'pumped' into the air by the plane. There is no need for a net momentum exchange between the airplane and the air in order for energy to be exchanged or for forces to be applied. Indeed, in those last two paragraphs above, you make no mention of momentum. BTW, I was wrong to invoke conservation of momentum. Momentum is conserved in elastic collisions, like the collision between a cue ball and the eight ball. Momentum is not conserved in inelastic collisions, like the collision between a cue ball and a nerf ball. You are incorrect. Momentum is *always* conserved. How is momentum conserved when a cue ball hits a nerf ball? Roll the airplane into a 90 degree bank. The weight is now orthogonal to the lift. As teh airplane falls, it banks even though there is no Earth 'under' the belly. Why? Because the wings are exerting a force on the air and the air consequently experiences a change in momentum. Yes, both the airplane and the air experience a net change in momentum when the aircraft climbs, descends, or banks. In level flight at constant speed the aircraft has constant horzontal and zero vertical momentum. The air exerts a force on the wings. In level flight, this force is countered by an equal and opposite force exerted on the aircraft by the gravitational attraction of the earth. Without that countering force, the aircraft would accelerate upward. That's what an unbalanced force *does*. Yes, no question about weight being balanced by lift. But the wings also exert a force on the air (Newton, remember: for every force there is an equal and opposite, etc., etc.). That force is not countered by *anything*. Hence, the air is accelerated downward; a continuous stream of air receives an constant change in momentum. If the air has a net increase in downward momentum, how is momentum conserved. F = ma; that's the way we normally see it presented. This equation relates force, mass and acceleration. It assumes a constant force acting on a constant mass will produce a constant acceleration, and the mass will start moving faster and faster. But there is an equally valid presentation of that equation; one which is more useful for examining what happens with an aircraft moving through the air: F = md/t^2; force is equal to mass, times distance, divided by the time squared. If you keep velocity and time squared together, you get acceleration of course, but there's no rule that says you have to. In fact, the rules of equations say exactly the opposite: that an equation is equally valid regardless of the way you group multiplications and divisions. So: F = m/t * v/t; the force is equal to the rate of mass per unit time, multiplied by the distance per unit time. What that says is that if you change the velocity of a given mass flow (air) by a given velocity, then you will get a given force. Yes, Force is the time rate of change of momentum. In other words, an aircraft passing through the air will cause a portion of that air to be disturbed downward. Because the aircraft is moving forward a constant speed, it imparts a downward velocity to certain mass of air each unit of time. The air starts moving downward with a certain velocity. I don't deny that downflow occurs. The pont is that downflow is a consequence of lift, not the cause of lift, and it is balanced by upflow, (albeit a more diffuse flow) otherwise the upper atmosphere would run out of air. Once you understand this, you understand why induced drag is less at hight speeds than low. Go twice as fast, and you encounter twice as much air in any unit time, and thus only need to impart a velocity to it that is half as much. But because the kinetic energy involved is proportional to mass and proportional to the *square* of velocity. Twice as much mass doubles its contribution to energy lost, but half the velocity *quarters* its contribution; giving an overall kinetic energy lost to induced drag of half as much when going twice as fast. Interesting. -- FF |
#2
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How is momentum conserved when a cue ball hits a nerf ball?
The vector sum, before and after, is identical. The vectors themselves are different (kinetic energy is converted to heat and such) but looking at both balls, or even looking at a cue ball and a glue ball, the center of gravity moves with the same velocity before and after. If the air has a net increase in downward momentum, how is momentum conserved. ....by the air's eventual collision with the earth. Momentum is similarly conserved when an object merely falls. The momentum gained by the falling object is cancelled by the momentum acquired by the earth rising up to meet it. In the case of "mysterious phantom gravity" not associated with the earth, momentum is not conserved, it disappears into the phantom gravity. This is one of the reasons why phantom gravity is not experimentally supported. If you ignore the earth, you are in the same position. I don't deny that downflow occurs. The pont is that downflow is a consequence of lift, not the cause of lift, and it is balanced by upflow, (albeit a more diffuse flow) otherwise the upper atmosphere would run out of air. If there were no earth for the smooshed-together air to crowd up against, the upper atmosphere =would= run out of air. Jose -- Money: what you need when you run out of brains. for Email, make the obvious change in the address. |
#3
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![]() Jose wrote: How is momentum conserved when a cue ball hits a nerf ball? The vector sum, before and after, is identical. The vectors themselves are different (kinetic energy is converted to heat and such) but looking at both balls, or even looking at a cue ball and a glue ball, the center of gravity moves with the same velocity before and after. Perhaps you are not familiar with nerf balls. Nerf balls are foam rubber. When a cue ball hits a nerf ball (sufficiently large) nerf ball it stops and the nerf ball just quivers a bit. The center of mas quits moving. The kinetic energy of the cue ball has been converted to heat. Energy is conserved, momentum is not. If the air has a net increase in downward momentum, how is momentum conserved. ...by the air's eventual collision with the earth. How is it conserved at the air/airplane collison? -- FF |
#4
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Perhaps you are not familiar with nerf balls. Nerf balls are foam
rubber. When a cue ball hits a nerf ball (sufficiently large) nerf ball it stops and the nerf ball just quivers a bit. The center of mas quits moving. The kinetic energy of the cue ball has been converted to heat. Energy is conserved, momentum is not. There is more to that. If this collision occurs in outer space, I guarantee you that the center of mass will =not= quit moving. On a pool table, friction with the table is involved, (as is to some extent rolling moment). The nerf ball starts its quiver in the direction the cue ball was going. If there is not enough force in the quiver to break starting friction, then the momentum gets imparted to the table (and the entire earth, which has no problem absorbing it). Jose -- Money: what you need when you run out of brains. for Email, make the obvious change in the address. |
#5
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![]() Jose wrote: Perhaps you are not familiar with nerf balls. Nerf balls are foam rubber. When a cue ball hits a nerf ball (sufficiently large) nerf ball it stops and the nerf ball just quivers a bit. The center of mas quits moving. The kinetic energy of the cue ball has been converted to heat. Energy is conserved, momentum is not. There is more to that. If this collision occurs in outer space, I guarantee you that the center of mass will =not= quit moving. But it will not move in a manner that conserves momentum. -- FF |
#6
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#8
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If the air has a net increase in downward momentum, how is
momentum conserved. ...by the air's eventual collision with the earth. How is it conserved at the air/airplane collison? (sorry, should have added this to the prevous post) It is conserved because the wing gets pushed (back) up when the air molecule gets pushed down. Jose -- Money: what you need when you run out of brains. for Email, make the obvious change in the address. |
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