Find all the accelerations of the 3 masses and the 1kg pulley

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SUMMARY

This discussion focuses on calculating the accelerations of three masses and a 1kg pulley in a tension system using d'Alembert's principle. The correct tensions were determined to be 33N for the big pulley rope and 12N for the 1kg pulley rope, assuming gravitational acceleration (g) is 10 m/s². The user, Paul, questions the simplification of the system by eliminating the 1kg pulley, which leads to an incorrect tension calculation of 10N. The response clarifies that internal parts of the system accelerate differently, making such simplifications invalid.

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paul_harris77
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Dear All

I have a question about tension in a mass system with pulleys.

vpc1vl.jpg


The question asks you to find all the accelerations of the 3 masses and the 1kg pulley. It also asks you to find the tensions in the ropes.

I have used d'Alembert's principle to do this and appear to have the correct answer for the tensions of 33N for the big pulley rope and 12N for the 1kg pulley rope (assuming g=10ms-2)

After doing this though, I am slightly confused. Surely the system could be simplified to the 3 kg mass on the left of the big pulley and a 4kg mass on the right hand side (eliminating the 1kg pulley). Then the tension in the remaining rope would be (4-3)g = 10N instead of 33N. Why is this not right?

Many thanks

Regards

Paul
 
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They 4kg mass you replace necessarily accelerates at one rate while the individual masses on the RHS are accelerating at different rates. They are not exerting the same reaction forces as their static weights so they don't "just add up".

Consider a third example of a simple pulley with two masses and a third mass on the right being dropped. It isn't appropriate to add in this third mass right? But why not?
 


paul_harris77 said:
Surely the system could be simplified to the 3 kg mass on the left of the big pulley and a 4kg mass on the right hand side (eliminating the 1kg pulley).
You can't replace a system with internal parts that accelerate differently with a single mass with a single acceleration. (Note that the force exerted on the 1 kg pulley by the hanging masses does not simply equal the weight of the hanging masses.)
 

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