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| Tags: angular, momentum |
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#1
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I'm sorry to bother you all with this question. I was just playing around
with a problem I found in a book. It is a simple problem where in a man sits on a stoll free to ratate without friction and is spun around while he holds two 3kg weights. we are given the moment of inertia of the man+stool, initial speed and the fact that the weights are 1m from the axis of rotation. The man then contracts his arms to 0.3m from the axis of rotation. Obviously the man will go faster because of this, but when I calculated the initial and final kinetic energies, they were VERY differant. Where did all that extra energy come from? Or did I calculate the energy wrong? |
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#2
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Timtro wrote: I'm sorry to bother you all with this question. I was just playing around with a problem I found in a book. It is a simple problem where in a man sits on a stoll free to ratate without friction and is spun around while he holds two 3kg weights. we are given the moment of inertia of the man+stool, initial speed and the fact that the weights are 1m from the axis of rotation. The man then contracts his arms to 0.3m from the axis of rotation. Obviously the man will go faster because of this, but when I calculated the initial and final kinetic energies, they were VERY differant. Where did all that extra energy come from? Or did I calculate the energy wrong? The man had to do work to reel in the weights. |
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#3
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Timtro wrote:
I'm sorry to bother you all with this question. I was just playing around with a problem I found in a book. It is a simple problem where in a man sits on a stoll free to ratate without friction and is spun around while he holds two 3kg weights. we are given the moment of inertia of the man+stool, initial speed and the fact that the weights are 1m from the axis of rotation. The man then contracts his arms to 0.3m from the axis of rotation. Obviously the man will go faster because of this, but when I calculated the initial and final kinetic energies, they were VERY differant. Where did all that extra energy come from? Or did I calculate the energy wrong? Angular Momentum http://scienceworld.wolfram.com/phys...rMomentum.html Look at equation (2) L is constant Kinetic Energy http://scienceworld.wolfram.com/phys...ticEnergy.html Look at equation (11) Total Energy is conserved, but Kinetic Energy is not |
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#5
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Centrifical force is converted to speed.
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#6
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"tj Frazir" wrote in message
... Centrifical.. .. .. no he wants an answer from someone with an education. |
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#7
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That much energy comes just from putting his arms in? It couldent possibly
take in the order of 100N to pull a couple of lousy 3kg weights into your sides could it? It seems to be the only explaination, certinly the first that I thought of, but I dismised it because it seemed so unreal. This is almost enough to get me into a bar, just to try it Wouldent I be the lifeof the party! hehe! "Richard" wrote in message ... Timtro wrote: I'm sorry to bother you all with this question. I was just playing around with a problem I found in a book. It is a simple problem where in a man sits on a stoll free to ratate without friction and is spun around while he holds two 3kg weights. we are given the moment of inertia of the man+stool, initial speed and the fact that the weights are 1m from the axis of rotation. The man then contracts his arms to 0.3m from the axis of rotation. Obviously the man will go faster because of this, but when I calculated the initial and final kinetic energies, they were VERY differant. Where did all that extra energy come from? Or did I calculate the energy wrong? The man had to do work to reel in the weights. |
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#8
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If i had to guess, i would say that the tip accelarates as a consequance of:
A: force provided by the jerk backwords to "snap" the whip/fly. B: I can picture it as being simolar to an angular rotation problem with th body rotating at one end. For example, placing a uniform rod with a pivot at one end, hanging from a ceeling. As a result of the angular motion when the system is released, the tip of the rod will accelerate faster than gravity. But the whip is not ridgid like a rod, and it is not simply under the influance of gravity. Also, the segments of the whip do not accelerate uniformly, this causes the whip to retard in such a way the the tip falls behind the midpoint in the whips trajectory (this is when tall towers begind to fall, they break apart). As the segments of the whip begin to reach full extension (starting near the hilt of the whip), the whips radius of rotation becomes smaller and smaller, and finally at the tip, when the radius is at its smallest, the energy reaches a maximum, and then the signature "snap" when the tip inverts and collides with itself. "Repeating Decimal" wrote in message ... in article , Richard at wrote on 10/25/03 5:05 PM: Timtro wrote: I'm sorry to bother you all with this question. I was just playing around with a problem I found in a book. It is a simple problem where in a man sits on a stoll free to ratate without friction and is spun around while he holds two 3kg weights. we are given the moment of inertia of the man+stool, initial speed and the fact that the weights are 1m from the axis of rotation. The man then contracts his arms to 0.3m from the axis of rotation. Obviously the man will go faster because of this, but when I calculated the initial and final kinetic energies, they were VERY differant. Where did all that extra energy come from? Or did I calculate the energy wrong? The man had to do work to reel in the weights. One of my pet interests is fly fishing and the cazsting required to put a fly out where you want it to go. The process is similar to that used in a whip. A heavy line, ususally tapered in thickness, is flicked out using arm motion. After the flick (cast) is completed, arm motion ceases. The line continues to travel. The speed of the tip can increast (in the case of a whip) close to the speed of sound. Often, the whip cracks or a fly gets flicked of the leader. How does the tip get speeded up? Aside from incidental losses to sound and the like, is mechanical energy conserved? Is momentum conserved? If not, where does extra momentum com from? If there is a discussion on the subject here, and if no one figures it out (an unlikely situation) I will reveal the mechanisms in a week or two. Bill |
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#9
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In article ers.com,
Timtro wrote: I'm sorry to bother you all with this question. I was just playing around with a problem I found in a book. It is a simple problem where in a man sits on a stoll free to ratate without friction and is spun around while he holds two 3kg weights. we are given the moment of inertia of the man+stool, initial speed and the fact that the weights are 1m from the axis of rotation. The man then contracts his arms to 0.3m from the axis of rotation. Obviously the man will go faster because of this, but when I calculated the initial and final kinetic energies, they were VERY differant. Where did all that extra energy come from? Or did I calculate the energy wrong? Did you recalculate the moment of inertia when the man changed the distribution of his masses? -- "Let us learn to dream, gentlemen, then perhaps we shall find the truth... But let us beware of publishing our dreams before they have been put to the proof by the waking understanding." -- Friedrich August Kekulé |
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#10
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"Timtro" wrote in message able.rogers.com... That much energy comes just from putting his arms in? It couldent possibly take in the order of 100N to pull a couple of lousy 3kg weights into your sides could it? There is something seriously wrong with your math. Energy is measured in Joules, not Newtons. Tom Davidson Richmond, VA |
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