The block of mass m₁ shown in figure (12-E2) is fastened to the spring and the block of mass m₂ is placed against it. (a) Find the compression of the spring in the equilibrium position. (b) The blocks are pushed a further distance (2/k)(m₁+m₂)g.sinθ against the spring and released. Find the position where the two blocks separate. (c) What is the common speed of the blocks at the time of separation?
Answers
Answered by
31
(a) Due to the gravitational force on the blocks that's will equal the spring force
So,
kx = (m1+m2)g sin theta
So,
x = (m1+m2)gsin theta/k
Now,
(b) The blocks are further pushed 2/k(m1+m2)g sin theta
So, Total compression = 3/k(m1+m2)g sin theta
That means that The amplitude of the SHM followed will be 2/k(m1+m2)g sin theta
And, after the total compression in the spring will become zero that is the spring comes to it's natural length , then the blocks will leave each other's contact.
(c) By work energy theorem,
Change in Kinetic Energy = Work done by all forces,
So,
1/2*(m1+m2)*v^2 = 1/2*k*x^2 - (m1+m2)gsin theta*x
Therefore,
1/2*(m1+m2)*v^2 = 1/2*k*(3/k(m1+m2)g sin theta)^2 - (m1+m2)g sin theta *(3/k (m1+m2) g sin theta)
So,
v = g sin theta * √(3/k(m1+m2)
Hope this helps you !
So,
kx = (m1+m2)g sin theta
So,
x = (m1+m2)gsin theta/k
Now,
(b) The blocks are further pushed 2/k(m1+m2)g sin theta
So, Total compression = 3/k(m1+m2)g sin theta
That means that The amplitude of the SHM followed will be 2/k(m1+m2)g sin theta
And, after the total compression in the spring will become zero that is the spring comes to it's natural length , then the blocks will leave each other's contact.
(c) By work energy theorem,
Change in Kinetic Energy = Work done by all forces,
So,
1/2*(m1+m2)*v^2 = 1/2*k*x^2 - (m1+m2)gsin theta*x
Therefore,
1/2*(m1+m2)*v^2 = 1/2*k*(3/k(m1+m2)g sin theta)^2 - (m1+m2)g sin theta *(3/k (m1+m2) g sin theta)
So,
v = g sin theta * √(3/k(m1+m2)
Hope this helps you !
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12
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