Answer:
τext =(M*R*g)*(m₂ - m₁) / (m₁ + m₂)
The wheel is rotating clockwise. Its vector direction is - k which is perpendicular to the plane of the wheel.
Step-by-step explanation:
Given info
m₁ = mass of block 1
m₂ = mass of block 2
m₁ < m₂
M = Mass of the wheel
R = Radius of the wheel
I = Moment of inertia of the wheel = M*R²
We assume that the wheel is rotating clockwise since m₁ < m₂
In order to get an expression for the net external torque acting on the system we can apply the following equation
τext = I*α
where α is the angular acceleration of the wheel which can be found as follows
at = R*α ⇒ α = at / R
then we have to compute the acceleration of the system (at), using the Newton's 2nd Law
Block 1:
∑Fy = m₁*at (↑+) ⇒ T - m₁*g = m₁*at (I)
Block 2:
∑Fy = m₂*at (↓+) ⇒ - T + m₂*g = m₂*at (II)
If we apply
(I) + (II) ⇒ at = g*(m₂ - m₁) / (m₁ + m₂)
Now, we get α:
α = at / R = (g*(m₂ - m₁) / (m₁ + m₂)) / R
⇒ α = (g / R)*(m₂ - m₁) / (m₁ + m₂)
Finally
τext = I*α = (M*R²)*((g / R)*(m₂ - m₁) / (m₁ + m₂))
⇒ τext =(M*R*g)*(m₂ - m₁) / (m₁ + m₂)
The wheel is rotating clockwise. Its vector direction is - k which is perpendicular to the plane of the wheel.