slowerlower
New member
- Joined
- Oct 26, 2014
- Messages
- 2
The problem is: An object begins at rest at the origin. At time t=0, it begins to move with velocity v(t) = <1, cos(pi*t) - pi*sin(pi*t), sin(pi*t) + pi*t*cos(pi*t)>. At what time T, point, and acute angle does the object leave the sphere (x^2 + y^2 + z^2 = 50)?
So I'm thinking that the "velocity" indicates that the equation above is a derivative of the position function. That position function should be P(t) = <t, t*cos(pi*t), t*sin(pi*t)>. For what it's worth, the acceleration is v'(t) = <0, -pi(2sin(pi*t) + pi*t*cos(pi*t), pi(2cos(pi*t) - pi(2cos(pi*t) - pi*t*sin(pi*t)> (I think, it was a lot). I'm thinking the next step might be to plug in this Position function into the sphere somehow to solve for when it leaves the sphere, but I'm not sure. Any thoughts, even general ideas?
So I'm thinking that the "velocity" indicates that the equation above is a derivative of the position function. That position function should be P(t) = <t, t*cos(pi*t), t*sin(pi*t)>. For what it's worth, the acceleration is v'(t) = <0, -pi(2sin(pi*t) + pi*t*cos(pi*t), pi(2cos(pi*t) - pi(2cos(pi*t) - pi*t*sin(pi*t)> (I think, it was a lot). I'm thinking the next step might be to plug in this Position function into the sphere somehow to solve for when it leaves the sphere, but I'm not sure. Any thoughts, even general ideas?