Guess we're all fine so let's get down to business shall we?
Problem:
A box of mass m is placed on a frictionless incline at an angle
\theta to the horizontal. The box is connected by a light, inextensible rope over a frictionless pulley at the top of the incline to a hanging mass M.- At time t=0, the system is released from rest.
- Assume the rope does not slip on the pulley.
- The incline and pulley apparatus are fixed.
Question:
What is the acceleration of the box just after release?
(i know the image looks weird, but it's AI generated and I hope you get the idea)
1,000 sats paid
Given:
m\thetaMIand radiusR(to be included for rotational effects)t=0a.T_1andT_2respectively.T_1 \neq T_2.\alphaof the pulley relates to linear accelerationaby:\tauon pulley is caused by difference in tensions:m a = m g \sin \theta - T_1M a = M g - T_2T_2 - T_1 = \frac{I}{R^2} aaon right:I = 0, this reduces to a simpler formula:M = m, implying infinite acceleration—showing the importance of pulley inertia.)I, the denominator increases, reducing acceleration. :)sin(\theta) \times 9.81 \frac{m}{s^2}