Blocks and Massive Pulley with Friction

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Rotational Motion Intermediate rigid body dynamics

Source: High school physics (Chinese)

Problem

Two objects of mass $m_1$ and $m_2$ are connected by a string over a pulley as shown. Block $m_1$ hangs vertically, while block $m_2$ is on a horizontal surface with a coefficient of kinetic friction $\mu$. The pulley has a moment of inertia $I$ and a radius $r$. The string does not slip on the pulley.

  1. Find the acceleration $a$ of the system.
  2. Find the tensions $T_1$ and $T_2$ in the string.
P0646-problem-1

P0646-problem-1

$a = \frac{(m_1 - \mu m_2)g}{m_1 + m_2 + I/r^2}$ $T_1 = \frac{m_1 g(m_2(1+\mu) + I/r^2)}{m_1 + m_2 + I/r^2}$ $T_2 = \frac{m_2 g(m_1(1+\mu) + \mu I/r^2)}{m_1 + m_2 + I/r^2}$

Apply Newton's second law to each object and the pulley. Let the direction of motion (down for $m_1$, right for $m_2$) be positive.

For mass $m_1$:

$$m_1g - T_1 = m_1 a$$

For mass $m_2$, the friction force is $f_k = \mu N = \mu m_2 g$:

$$T_2 - \mu m_2 g = m_2 a$$

For the pulley, the net torque is $\tau = (T_1 - T_2)r$. Using $\tau = I\alpha$ and the no-slip condition $a = \alpha r$:

$$T_1 - T_2 = I \frac{a}{r^2}$$

To solve for $a$, isolate $T_1$ and $T_2$ from the first two equations and substitute into the third:

$$(m_1g - m_1 a) - (m_2 a + \mu m_2 g) = \frac{I}{r^2} a$$

Rearrange to solve for $a$:

$$m_1g - \mu m_2 g = a (m_1 + m_2 + \frac{I}{r^2})$$ $$a = \frac{(m_1 - \mu m_2)g}{m_1 + m_2 + I/r^2}$$

Substitute $a$ back into the equations for $T_1$ and $T_2$:

$$T_1 = m_1(g - a)$$ $$T_2 = m_2(a + \mu g)$$