
William W. answered 06/11/19
Experienced Tutor and Retired Engineer
This problem should be split into two parts, what's happening in the x direction and what's happening in the y direction.
First, draw a sketch (including the coordinate plane we are going to use):
Then draw a free body diagram (since friction is not mentioned, we'll ignore friction). A free body diagram shows the object in question as a dot and then all the forces acting on it - in this case, the forces are gravity and the normal force (the force the ramp is putting on the block that keeps the block from falling through the ramp). However, as I mentioned, we will divide the problem into two parts, the x direction and the y direction, so, since gravity, Fg, is not aligned to either the x or the y direction, we will split it into it's vector components that do align with the x and y directions:
Using trigonometric ratios, we can find that sin(35°) = Fg-x/Fg or Fg-x = Fgsin(35°)
Since we know that the force of gravity equals the mass times the acceleration of gravity (g) and that g = 9.81 m/s2, Fg = (15)(9.81) = 147.15 N
Then Fg-x = (147.15)(sin(35°)) = 84.4 N
Since that's the force in the direction of the travel, that's the force that will be pulling Blocky down the hill, To find his acceleration, we use F = ma or a = F/m = 84.4/15 = 5.627 m/s2
Now, we use the kinematic equations to find his velocity using this acceleration. vf2 = vi2 + 2ax. We will assume he starts from rest (vi = 0) so vf2 = 02 + 2(5.627)(80) or .vf2 = 900.29 and, taking the square root, we get vf = 30.005 m/s or rounding to 2 significant figures, vf = 30 m/s
To get the time, we use a different kinematic equation: vf = vi + at
So 30.005 = 0 + 5.627t and, solving for t, we get t = 5.332 s, again, rounding to 2 significant figures, we get t = 5.3 s