Question
a)
b) above the branch
As @SayedAbdul pointed out below, it's possible to use a quicker solution in part (b) than what's shown in the video due to the fortunate coincidence that the branch is halfway between the archer and the target. At this horizontal position the vertical component of the arrow's velocity is zero, in which case can be rearranged (substituting zero for ) as . Had the branch been in a different horizontal position, then the approach shown in the video would need to be used, or this quicker approach would need to be modified by finding the vertical component of velocity at the branch's horizontal position.
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This is College Physics Answers with Shaun Dychko. This archer fires an arrow at a target which is 75 meters away and the height of the target is the same as the launch height of the arrow, and we'll say that is y naught equals zero. The speed of the arrow is 35 meters per second and we don't know what the angle of launch is, but that's part A, is to figure that out. Now because we have this convenient fact that the launch height of the arrow is the same as the target, we are allowed to use this range formula. We can solve it for theta and then that will give us this angle of launch. So the range which is 75 meters, equals the initial velocity of the arrow which is 35 meters per second, times sine of two times the launch angle, all divided by the acceleration due to gravity. We will solve this for sine two theta first by multiplying both sides by g over v naught squared and g over v naught squared cancels on the right and it appears on the left multiplied by r. Then we'll switch the sides around so we have sine two theta equals rg over