- #1
mgsk
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Monkey and hunter -- forces, vectors
I'm currently supplementing my institutional education with some me-time study. I'm studying maths and physics A-levels (or, rather, A-level equivalent).
Yale University has an awesome "online courseware" which makes available to the public videos of lectures and study materials (problem sets, etc.). My problem refers to the problem set given for the Newton's Laws lectures, found here: problem set, solutions, specifically problem 8. The problem is quoted here:
I began with asking what are the positions for each object's motion. The monkey is easy. It's "x" position is unchanging, and so does not vary with time: [tex]x_m =d [/tex]; while it's "y" position is changing with time: [tex]y_m = h-\frac{1}{2} g t^2[/tex]. Next, and this is where my approach differs to that given in the solution, I define the components of the bullet. The bullet begins with some initial velocity [tex]v_0[/tex] in the horizontal direction, and so by my understanding of forces and Newtonian mechanics, this horizontal velocity is constant (ignoring air resistance), so that the bullet's "x" position is: [tex]x_b=v_0 t[/tex]; and like the monkey, the bullet's "y" position changes because of gravity: [tex]y_b=h-\frac{1}{2} g t^2[/tex].
My reasoning is then: for the bullet to hit the monkey, the bullet must travel a horizontal distance d in a time that is no greater than the time it takes the monkey to fall a distance h; and because I'm dealing with the horizontal distance, I can focus on the "horizontal" component of the bullet's trajectory. Thus, the time for the bullet to travel a distance d is: [tex]t_{b}=\frac{d}{v_0}[/tex]; and the time it takes for the monkey to reach the ground is (given by solving [tex]y_m=0[/tex] for t): [tex]t_m=\sqrt{\frac{2h}{g}}[/tex]. Then equating the two and solving for [tex]v_0[/tex]: [tex]v_0=\frac{d\sqrt{g}}{\sqrt{2h}}[/tex].
Can someone spot the error in my reasoning? Many thanks!
P.S. Sorry for the poor formatting. I'm not familiar with this forum's LaTeX tools.
Homework Statement
I'm currently supplementing my institutional education with some me-time study. I'm studying maths and physics A-levels (or, rather, A-level equivalent).
Yale University has an awesome "online courseware" which makes available to the public videos of lectures and study materials (problem sets, etc.). My problem refers to the problem set given for the Newton's Laws lectures, found here: problem set, solutions, specifically problem 8. The problem is quoted here:
A monkey is hanging from a height h and a person d meters away from the tree and on the ground, wants to zap it (in today's version with a tranquilizer gun and in the original version, a hunting rifle). He aims straight at the monkey and fires. This would of course work in the absence of gravity but show that it will work even in its presence provided the initial speed obeys [tex]\sqrt{\left ( d^2+h^2 \right ) \frac{g}{2h}}[/tex]. What does this requirement ensure? Given that this will also work if a pulse of laser light is used, what do you learn about light in a gravitational field?
Homework Equations
I began with asking what are the positions for each object's motion. The monkey is easy. It's "x" position is unchanging, and so does not vary with time: [tex]x_m =d [/tex]; while it's "y" position is changing with time: [tex]y_m = h-\frac{1}{2} g t^2[/tex]. Next, and this is where my approach differs to that given in the solution, I define the components of the bullet. The bullet begins with some initial velocity [tex]v_0[/tex] in the horizontal direction, and so by my understanding of forces and Newtonian mechanics, this horizontal velocity is constant (ignoring air resistance), so that the bullet's "x" position is: [tex]x_b=v_0 t[/tex]; and like the monkey, the bullet's "y" position changes because of gravity: [tex]y_b=h-\frac{1}{2} g t^2[/tex].
The Attempt at a Solution
My reasoning is then: for the bullet to hit the monkey, the bullet must travel a horizontal distance d in a time that is no greater than the time it takes the monkey to fall a distance h; and because I'm dealing with the horizontal distance, I can focus on the "horizontal" component of the bullet's trajectory. Thus, the time for the bullet to travel a distance d is: [tex]t_{b}=\frac{d}{v_0}[/tex]; and the time it takes for the monkey to reach the ground is (given by solving [tex]y_m=0[/tex] for t): [tex]t_m=\sqrt{\frac{2h}{g}}[/tex]. Then equating the two and solving for [tex]v_0[/tex]: [tex]v_0=\frac{d\sqrt{g}}{\sqrt{2h}}[/tex].
Can someone spot the error in my reasoning? Many thanks!
P.S. Sorry for the poor formatting. I'm not familiar with this forum's LaTeX tools.