Statics example from Meriam ( SI improper )

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    Example Si Statics
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SUMMARY

The discussion focuses on the concept of partial constraints in statics, specifically regarding the behavior of a blue rectangle constrained by three links. The first two links fix the position of point A, while the third diagonal link experiences variable tension due to potential rotation around point A. As highlighted by user @Baluncore, tension in link 3 can become infinite when its attachment points align with point A, similar to a taut rope scenario. This principle is practically applied in vehicle recovery situations, demonstrating the importance of understanding tension dynamics in real-world applications.

PREREQUISITES
  • Understanding of static equilibrium and constraints in mechanics
  • Familiarity with tension forces and their calculations
  • Knowledge of basic trigonometric functions, particularly the cosine function
  • Experience with practical applications of physics in real-world scenarios
NEXT STEPS
  • Study the principles of static equilibrium in mechanical systems
  • Learn about calculating tension in cables and ropes under various conditions
  • Explore the application of trigonometric functions in physics problems
  • Research practical techniques for vehicle recovery using tension principles
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This discussion is beneficial for engineering students, mechanics, and anyone interested in the practical applications of statics and tension in real-world scenarios, particularly in vehicle recovery techniques.

lakuzamalakuzam
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could not understand why it is partial constraints. Also, I don't understand how link works. Below here is what I am thinking i think it is totally wrong can someone explain what's wrong with my idea here.
1601627852528.png
 
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Welcome to PF.

The blue rectangle is not fully constrained by the three links within the frame. The position of A is fixed by the first two links, but the diagonal link 3 may be stretched as the body is rotated slightly about A.

The top of the cosine function at zero, is horizontal. Because the line from A to link 3 is straight, very high tension forces could be present in link 3 if the body was rotated slightly.
 
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As @Baluncore stated, the tension on link 3 goes to infinity when its attachment points are co-linear with point A. The situation is similar to a rope or chain stretched tight between two supports. Try calculating the tension when pushing on the center of the rope/chain span.

A practical use of the phenomena is retrieving a vehicle from a ditch.
Two people with a chain, a tree, and something to block the wheels, can pull the vehicle out. Providing there is a portion of the chain not being supported (by the ground):
  1. chain taught between tree and vehicle
  2. person 1 stands on the middle of the chain, deflecting it
  3. person 2 chocks the vehicle wheels so can't roll back down into the ditch
  4. person 1 steps off the chain and repeats from step (1)
Upon completion, they choose a different route. :olduhh:

Cheers,
Tom
 
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