Two masses over a pulley. Acceleration and tension in terms of the two masses.
The situation
Two masses m1>m2 are connected by a light inextensible string over a smooth, massless pulley. The system is released from rest. Find the acceleration and the tension in the string.
Setting up
Since the string is inextensible and the pulley is smooth (frictionless), both masses have the same magnitude of acceleration a. m1 (heavier) accelerates downward, m2 accelerates upward.
Taking downward as positive for m1 and upward as positive for m2:
For m1 (going down):
m1g−T=m1a...(1)
For m2 (going up):
T−m2g=m2a...(2)
Solving for acceleration
Add equations (1) and (2):
m1g−m2g=(m1+m2)a
a=m1+m2(m1−m2)g
Solving for tension
From equation (2): T=m2(g+a)
Substitute a:
T=m2(g+m1+m2(m1−m2)g)=m2g⋅m1+m2m1+m2+m1−m2=m2g⋅m1+m22m1
T=m1+m22m1m2g
Checking special cases
Equal masses (m1=m2=m):
a=0,T=mg
System stays at rest, tension equals the weight of either mass. Makes sense — balanced.
One mass much larger (m1≫m2):
a≈g,T≈2m2g
m1 falls nearly in free fall, m2 is accelerated upward at nearly g.
Tension is less than either weight
T=m1+m22m1m2g
Compare with m2g:
m2gT=m1+m22m1<2and>1 when m1>m2/...
More directly: T<m1g (since m1 accelerates downward — net force is downward, so T<m1g) and T>m2g (since m2 accelerates upward — net force is upward, so T>m2g).
m2g<T<m1g
Tension lies between the two weights. This is a useful check.
Historical note
The Atwood machine was invented by George Atwood in 1784 to verify Newton's Second Law experimentally. By using two nearly equal masses, the acceleration is much less than g, making it easy to measure with the instruments available at the time.
Remember
Always assign consistent positive directions before writing equations. For Atwood's machine: the direction of motion of $m_1$ is positive for $m_1$, and the direction of motion of $m_2$ is positive for $m_2$. Both bodies have acceleration of magnitude $a$ — the string constraint ensures this.