Stepped Pulley: Angular and Linear Acceleration

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SUMMARY

The discussion focuses on calculating the angular acceleration of a stepped pulley system with a moment of inertia (I) of 2.0 kg*m², connected to two masses of 1.0 kg and 2.0 kg via strings attached to radii of 20 cm and 50 cm, respectively. The user seeks clarity on the relationship between angular speed (ω), angular acceleration (α), and linear acceleration (a), specifically how to apply the equations τ = Iα and v = rω. The conversation emphasizes the importance of using Newton's second law (F = ma) for each mass and the relationship between linear and angular quantities.

PREREQUISITES
  • Understanding of rotational dynamics, specifically the concepts of torque (τ) and moment of inertia (I).
  • Familiarity with Newton's second law (F = ma) and its application to both linear and rotational motion.
  • Knowledge of the relationship between linear and angular quantities (v = rω, a = rα).
  • Basic proficiency in using LaTeX for formatting equations in discussions.
NEXT STEPS
  • Study the derivation and application of the equations τ = Iα and F = ma in rotational systems.
  • Explore the conservation of angular momentum and its implications in pulley systems.
  • Learn how to effectively use LaTeX for presenting physics equations clearly.
  • Investigate the effects of friction in pulley systems and how it alters angular acceleration calculations.
USEFUL FOR

Students and educators in physics, mechanical engineers, and anyone interested in understanding the dynamics of pulley systems and rotational motion.

robert6774
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A stepped pulley is essentially a system of connected cocentric disks that have different radii. A stepped pulley (I= 2.0 kg*m^2) is placed on a frictionless axle and then strings are attached to two radii of 20 and 50 cm. The other ends of the strings are attached to a 2.0 and 1.0 kg mass respectively. Determine the angular acceleration of the pulley and the linear accelerations of the two masses.

I= 2.0 kg*m^2
r1= 50 cm
r2= 20 cm
m1= 1.0 kg
m2= 2.0 kg
w1= 0
w2= ?

I think I'm confusing the concept of the pulley starting at rest (so w1= 0) and the final angular speed (w2) of the rotating pulley with the fact that there are two different radii to be used in the same equation for the same pulley.

I'm pretty sure v= rw will come into play at some point but I need to find the angular speed in order to find the angular acceleration. And where the heck does time fit into all this?

I've also considered finding the linear accelerations and working the other way around but again I'm not sure how to look at this.

I've winged a couple ideas using the conservation of angular momentum and the conservation of angular kinetic energy but it doesn't make sense. Where do I start and how do look at/approach this problem?
 
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Thank you tiny-tim for your help. I've just figured out how to use the Latex symbols, that should make my equations easier to read. The other Latex stuff is a bit more complicated, don't know if I'll need it.
 

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