00:01
Here in this given problem, this is the rough inclined plane which is inclined at an angle of 37 degree with the horizontal.
00:12
Means this angle theta, this is given to be 37 degree out of the two blocks.
00:24
The first block of mass m1 where m1 is 50 kg that is kept over the inclined plane and another block that is hanging with the help of a thread, a light string.
00:42
The string is passing over a pulley, massless frictionless pulley.
00:47
Its mass m2 where this m2 is 100 kg.
00:56
Its weight m2g acting vertically down, tension t in the string.
01:02
Weight of the first block m1g that is also acting vertically down.
01:08
Its two components, first component perpendicular to the inclined plane that is m1g cos theta and another component along the inclined plane m1g sin theta.
01:24
Normal reaction of the inclined plane over the first block n which using newton's third law of motion that should be equal to m1g cos theta.
01:39
As this block will be falling down suppose with an acceleration a, so 50 kg block that will be moving up and the two points over the inclined plane a and b.
01:56
Coefficient of kinetic friction 0 .250, the gap between the two points a and b, this is ab is equal to 20 .0 meter.
02:08
First of all using free body diagram of the hanging block for which m2g should be more, m2 that is 100 kg.
02:32
So 100g -t, this net force should be equal to mass of the block 100 kg with its multiplied by the acceleration and that is using newton's second law of motion.
02:47
This is equation number 1.
02:49
Then using free body diagram of the block kept over the inclined plane, free body diagram of 50 kg block.
03:07
As it is moving up, so tension t will be more.
03:11
Then m1g sin theta means for m1 this is 50g sin 37 degree minus force of friction acting backward fk and that should be equal to m1 into a means 50a...