00:01
So we give a block initial speed and the block starts moving up a slope.
00:06
And we know the kinetic coefficient for the slope.
00:11
And we want to know how far the block will get.
00:13
And if the block will slide back down once it gets the maximum value.
00:19
So first we can draw the free body diagram for this situation.
00:23
So we have the normal force following the slope.
00:27
So normal force, force of ground.
00:31
Gravity, fg, and then the friction that is opposing the direction of motion.
00:43
So this is theta, fk, normal force, and gravity.
00:49
In components we have the newton equation as kinetic friction plus mg sine of theta is equal to m a, and n is equal to m g cosine of theta.
01:03
We can combine both of this equation because we know so fk equals mu k n and we can substitute the normal force to get to give the acceleration is equal to g sine of theta plus mu kgg cosine of theta.
01:22
And now we need to solve for the kinematic equation to find the displacement.
01:29
So we solve for v square equals v0 square plus 2a delta x.
01:35
We want the situation where v to define a velocity 0 and we want to find delta x.
01:41
So delta x is equal to v0 squared divided by 2a.
01:51
And this gives us v0 square divided by 2 times g sine of theta plus mu kg full sign of theta.
02:08
And this is 1 .4 meters per second square 2 times 9 .8.
02:16
Times sine of 22 degrees plus 0 .7 full sign of 22 degrees...