Here three blocks A, B and C are connected with strings and pulleys as shown in figure. The constraint relation between the acceleration of masses A, B, and C can be formulated as?
+ 2 + = 0
Take the ceiling as reference Now assume the distance of block A is yA, B is yB and C is yC
Now we can say that yA + 2yB + yC = l0 where l0 is the length of the string. Assume acceleration of blocks A, B and C as shown and differentiate once with respect to time
dyAdt=−vA & dyBdt=−vB as length is decreasing by the assumed acceleration
-vA - 2vB + vC = 0 (dl0dt=0 as l0 is constant) differentiating again. -aA - 2aB + aC = 0 ⇒ aC = (aA + 2aB) But C is going down while A & B are going up so aC = - (aA + 2aB)
Alternate solution I Let us assume that masses A and B would go up by distance xA and xB, respectively. This length of the string will slack as length (ab+cd) above the pulley P. Thus the block B will go up by a distance xB as shown in figure. Thus we have
(ab + cd) + xA = -xC or 2xB + xA = - xC (-ve sign due to sign convention)
Differentiating with respect to time, we get 2vB + vA = -vC ...(i)
Differentiating again with respect to time, 2aB + aA = -aC ...(ii)
Equations (i) and (ii) are the constraint relations for motion of masses A, B, and C.
Alternate solution II: Displacement of pulley is average displacement of both sides
Pulley 0 = xA−x12
= XA = X1
For Pulley z
XB=x2−x12
2XB+X1=X2
x2 = xC
xC = 2xB + xA
∵ x2 is up and xC is down so with sign
xC = -(2xB + xA)
⇒ xA + 2xB + xC = 0
⇒ vA + 2vB + vC = 0
⇒ aA + 2aB + aC = 0