When the blocks are released, what is the acceleration of the lighter block?
A 1.4 kg block and a 2.7 kg block are connected to opposite ends of a light rope that passes over a solid, frictionless pulley with a diameter of 25 cm and a mass of 0.72 kg. When the blocks are released, what is the acceleration of the lighter block?
Here’s what I’ve worked out so far:
- For the 1.4 kg block, the force equation is ( T_1 - m_1g = m_1a ).
- For the 2.7 kg block, the force equation is ( T_2 - m_2g = m_2a ).
- For the pulley, I believe the torque equation is ( \text{torque} = rF ), where ( F ) would be ( T_2 - T_1 ). This is then set equal to ( I\alpha ), or ( \frac{1}{2}mr^2 \cdot \frac{a}{r} ), since the pulley is a solid disk.
From here, I tried solving for ( a ) by rearranging the force equations to express ( T_1 ) and ( T_2 ), then substituting those values into the torque equation. However, my answer was incorrect, and I’m not sure where I’ve gone wrong.
Can someone help clarify my approach or point out any mistakes? Any guidance would be greatly appreciated!
2 Answers
m₁ = mass 1 = 1.4 kg
m₂ = mass 2 = 2.7 kg
m₃ = mass of the pulley = 0.72 kg
R = radius of the pulley = 0.25 m
g = accelerayion by gravity = 9.8 m/s²
First, you need to ‘choose’ a direction in which the system will accelerate. As m₂ is bigger than m₁, it seems logic to choose m₂ moving down, and m₁ moving up.
(Note: If you choose wrong, that’s not a problem. You will end up with a negative value for acceleration so you will know that the system moves in the other direction than the one you chose)
The forces acting on m₁ are:
* tensile force in the rope, pulling up
* force of gravity, pulling down
As m₁ is moving up, you know that the tensile force is bigger than the gravitational force. The net force on m₁ will be:
Fnet₁ = T₁ – m₁×g
By Newton’s second law, you can say:
T₁ – m₁×g = m₁×a
T₁ = m₁×g + m₁×a . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . equation 1
The forces acting on m₂ are:
* tensile force in the rope, pulling up
* force of gravity, pulling down
As m₂ is moving down, you know that the gravitational force is bigger than the tensile force. The net force on m₂ will be:
Fnet₂ = m₂×g – T₂
By Newton’s second law, you can say:
m₂×g – T₂ = m₂×a
T₂ = m₂×g – m₂×a . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . equation 2
The moment of inertia of the pulley (assuming it is a solid disk) is:
I = m₃×R²/2 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . equation 3
The equation for torque on the pulley is:
T₂×R – T₁×R = I×a/R
Rearranging this a bit, you get:
(T₂ – T₁)×R = I×a/R
T₂ – T₁ = I×a/R² . .. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . equation 4
Substituting equation 3 into equation 4, you get:
T₂ – T₁ = (m₃×R²/2)×a/R²
T₂ – T₁ = m₃×a/2 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . equation 5
(note how the radius R cancels out)
Now substituting equations 1 and 2 into equation 5, you get:
(m₂×g – m₂×a) – (m₁×g + m₁×a) = m₃×a/2
m₂×g – m₂×a – m₁×g – m₁×a = m₃×a/2
m₂×g – m₁×g = m₃×a/2 + m₂×a + m₁×a
(m₂ – m₁)×g = (m₃/2 + m₂ + m₁)×a
a = g × (m₂ – m₁) / (m₃/2 + m₂ + m₁)
And finally, entering the numbers, you get:
a = (9.8 m/s²) × [(2.7 kg) – (1.4 kg)] / [(0.72 kg)/2 + (2.7 kg) + (1.4 kg)]
a = 2.8565… m/s²
a = 2.9 m/s² (to 2 sf)
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