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Lorien Stable: Trainer's Notes Welcome. Enjoy. For discussion of this article, or any other topic, visit the Message Board. |
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Okay, let's consider the question. Say you're a rider of mass
m on a horse who is
h tall, and he bucks with a force of F. To reference the equations I'm using, go here: Constant-acceleration equations. If you're not interested in how I found it, just in the answer, then skip to the bottom ;) |
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The force F imparts a upwards velocity vbuck
(that is, you are suddenly flying upwards). You go upwards more and
more slowly, until gravity (g) has halted you at a height
h2 above the saddle. Then you go back down. You are essentially falling from a standstill at a height d. F=ma   -->   a=(vbuck-0)/tbuck F=m(vbuck/tbuck)   -->   vbuck = (F tbuck)/m 0=vbuck² + 2g h2   -->   h2=(vbuck)²/2g so:
You fall a distance d=h+h2. |
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Okay, now suppose you are on a horse who is merrily galloping along at a
speed v. This horse now bucks with a force F. For convenience, I am going to assume that air resistance doesn't make a difference in the short distance you're falling (it won't really), so v doesn't change. |
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The force F imparts the same upwards velocity
vbuck. However, instead of flying straight up, and
then falling from a standstill, you go up the same distance...you just
also go forwards a distance xup. Then, while you are
falling from a height d, you are continuing to move forward a
distance xdown. When you eventually hit the ground, you are falling down at the same speed as if the horse had been standing still...you are also falling *forward* at the speed the horse was running. You still fall a distance d=h+h2. |
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Okay, so this is the difference in the fall: one goes straight down, one
goes forward and down. The height of the fall is the same--the
time of the fall is the same. d=g (tfall)²/2 tfall = sqrt(2d/g) |