Find length of spring A in equilibrium position

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SUMMARY

The discussion focuses on determining the length of spring A (LA2) in its equilibrium position when a piston, supported by two springs (A and B), is released from a pinned state. The spring constants are kA = 3,859 N/m and kB = 3,090 N/m, with natural lengths LA0 = 0.03 m and LB0 = 0.1 m. The lengths of the springs when pinned are LA1 = 0.1 m and LB1 = 0.1 m. The equilibrium position can be found using the elastic energy constitutive relation and the first law of thermodynamics, simplifying the problem to a force balance due to the vacuum condition.

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  • Understanding of elastic energy and spring constants
  • Knowledge of the first law of thermodynamics
  • Familiarity with force balance concepts in physics
  • Basic principles of equilibrium in mechanical systems
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  • Study the application of the elastic energy constitutive relation in mechanical systems
  • Learn about force balance calculations in equilibrium scenarios
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ally2106
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As shown in Figure Q1a, a frictionless, massless, piston, supported by two springs, A and B, is held by a pin in a vacuum inside a rigid-walled container. The properties of the springs are: spring constants kA = 3,859 and kB = 3,090 (in N/m), natural lengths LA0 = 0.03 and LB0 = 0.1 (in m). When the piston is pinned to the wall, the lengths of the springs are LA1 = 0.1 and LB1 = 0.1 (in m), respectively. Both springs possesses dissipative properties so that after the pin is pulled, the piston eventually comes to rest at an equilibrium position. Find the length of spring A in this equilibrium position (LA2) in units of m.

Equations so far:
Models:
Elastic Energy Constituitive Relation: (E2 - E1) = (k/2)(x22 - x12)

First Law of thermodynamics: (E2 - E1) = (Q1-2) - (W1-2)
Second Law of thermodynamics...

Don't really know where to start? Help appreciated
 
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Hello Ally, welcome to PF :smile: !

You bring in thermodynamics, but is that really intended for this exercise ? I don't see any other given than "vacuum" , so I must assume that applies to both volume A and volume B. And then the exercise becomes a simple force balance.
 

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