constantly decreases with a rate of .
In the above pulley-mass system the massIf initially both the masses were equal to , then find the distance travelled by the mass in meters in assuming that the mass didn't reached the top end in those and .
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Since the mass m decreases at constant rate α = 0 . 0 1 g s − 1 and at the beginning m ( 0 ) = M , we can write:
m ( t ) = M − α t
The force on the system is:
F = ( M − m ( t ) ) g = ( M + m ( t ) ) x ¨ ⇒ x ¨ = M + m ( t ) ( M − m ( t ) ) g
x ¨ = 2 M − α t α g t , with boundary conditions x ( 0 ) = 0 and x ˙ ( 0 ) = 0
It's easy to integrate that expression twice in order to get x ( t ) :
x ( t ) = 2 α 2 α t ( 4 M − α t ) + 4 M lo g ( 2 M ) ( α t − 2 M ) + 4 M ( 2 M − α t ) lo g ( 2 M − α t ) g
Using the values provided in the text, we fine x ( 3 0 s ) = 0 . 2 2 5 m .