In: Physics
, on a hill. Dr. L., Jimmie and Kepler (Total mass = MT ) are all on a massless sled together. They are on a hill that is at an angle of θ above horizontal… Ok. Now we know Dr. L. is lazy. This is the third problem he’s reused… Assume they start from rest and that there is no friction between the sled and hill. a.) How fast will the sled be going when it reaches the bottom of the hill. --- Now assume there’s friction between the sled and hill. The coefficient of kinetic friction is µK. b.) Draw a free body diagram of the sled. c.) What is the force of friction acting on the sled? d.) Now use energy and determine the final velocity of the sled with friction. Is it less than it was before? Good! It better be.
Okay, the problem statement is incomplete...but i understand that sled is moving down on a slope.
The hill has some vertical height (h) ......The slope has a length L
Then to find h , you can use trigonometry
h = L*sin
Then using conservation of energy
mgh = 1/2mv2
gh = v2 / 2
v = sqrt (2gh)
where v is the speed of sled at the bottom of the hill.
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Now, we must consider friction
Here is the free body diagram
where Fk is the force of kinetic friction and it acts in the opposite direction of motion.
Force of friction
Fk = ukN
Fk = ukmgcos
Now, work done by friction = ukmgcos* L
where L is length of slope
so,
finally
equating the initial and final energy, we get
mgh + ukmgcos* L = 1/2mv2
gh + ukgcos* L = 1/2v2
2 (gh + ukgcos* L) = v2
v = sqrt (2gh + 2ukgcos L)