Calculating Tensions and Acceleration in Frictionless Pulley System

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SUMMARY

The discussion focuses on calculating tensions FT1 and FT2 and the acceleration of two weights (200 N and 300 N) in a frictionless pulley system. The key insight is that the acceleration of block B is half that of block A, which can be mathematically proven by analyzing the constraints of the string length. The relationship is established through the equation a_x + 2a_y = 0, where a_x is the acceleration of mass A and a_y is the acceleration of mass B. Practical experimentation with a piece of string is also suggested to visualize the concept.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Basic knowledge of pulley systems
  • Familiarity with calculus concepts, particularly derivatives
  • Ability to analyze forces and tensions in mechanical systems
NEXT STEPS
  • Study the principles of Newton's second law in detail
  • Explore advanced pulley system mechanics
  • Learn about tension calculations in multi-body systems
  • Experiment with physical models to understand string dynamics
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Physics students, mechanical engineers, and anyone interested in understanding dynamics in frictionless systems will benefit from this discussion.

Lamoid
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The weights of the objects are 200 N and 300 N. The pulleys are essentially frictionless and massless. P1 has a stationary axle but P2 is free to move up and down. Find the tensions FT1 and FT2 and the acceleration of each body.

Diagram I made in paint attached.

Now my problem is not that I can't get the right answer but that I don't understand why. It gives me a hint that the acceleration of block B is half (and in the opposite direction of course) that of block A and I cannot not figure out why that is. Can anyone explain it to me?

And yes, the diagram sucks but the A block is moving down, B is moving up.
 

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You can prove mathematically that the magnitude of the acceleration of A is twice that of B using the fact that the string length remains constant. Divide the string into three pieces: X (from mass A to P1), Y (from P1 to P2), Y (from P2 to the spot of rope at the height of P1). Thus the length of the rope is X + 2Y. Since the length can't change, take the derivative twice to find the acceleration constraint: a_x + 2a_y = 0. Make sense? (a_x is the acceleration of mass A; a_y is the acceleration of mass B)

But even better than proving it is to just play around with a piece of string and see how folding the string in half affects things.
 
Thank you very much! That's a neat calculus proof.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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