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No, you are right, there is no infinite force. The force exerted on the fly is directly proportional to the gradient of that line.
As for the false-model of the fly and bus as indestructible, non-deformable particles, well that is true also.
So how about if I now say that the graph is for one atom at the front of the fly, and one atom at the front of the bus. Now, you can deform atoms, you can wrench them apart and bond them together. But not at 50mph. So some constituent part of the fly will obey the rule of that graph. Doesn't really matter if the head being crushed cushions the blow to the body. For the body of the fly, the graph will be a slightly different shape. In fact, because of this effect, the 'corners' of the graph should be slightly rounded. But this doesn't matter, it should still go through zero, whatever it's shape.
As the first part of the fly, the first atomic surface, interacts with the first surface of the screen, it experiences a force. The force accelerates the fly, from -2 to +50 mph. And as it does so the velocity of the fly (or one of it's constituent parts) must at some time be zero. You cannot accelerate from -2 to 50 without going through zero. An acceleration can be very, very sudden, but never instantaneous.
I could, given enough data and a supercomputer, draw graphs of every single velocity of every single atom in that fly. Some of them would not obey that graph at all, as bits of fly zoom out into the atmosphere. Some of them would obey it closely, and these are the ones which at some time reach a velocity of zero.
Steve Dubplate: How could the fly, or any part of it, change direction instantaneously? It must take time, hence the graph having a slope.
The thing with instantaneous force being used to show that the orbits of planets are elliptic is also correct. This is just plain calculus. (Though in those days it was very new...) The derivation, as I've learnt it (I think this is the right one) does the math using 'real' (ie. big, measurable intervals) of time, velocity, angle and therefore acceleration, and shows that as the interval in time approaches zero, an expression can be given for the force acting on the body at that instant.
Taking this back to the fly, I can do the same thing with my graph. I can take the derivative of that graph, ie. it's gradient, and I will get a constant value, from which I can work out the force. That is the force exerted at any one instant on the fly. But if I exert that force over 'zero time', I cannot accelerate the fly. |
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