MAxwell reciprocal theorem and symmetric stiffness matrix

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SUMMARY

The discussion centers on the application of Maxwell's reciprocal theorem, which asserts that the stiffness matrix is symmetric (k12 = k21, kij = kji) for elastic materials undergoing small displacements. Despite this, the author observes that their assembled stiffness matrix remains symmetric even in geometric non-linear problems involving beam elements, specifically a cantilever beam with an end moment. This raises questions about the conditions under which symmetry is maintained in non-linear structural behavior.

PREREQUISITES
  • Understanding of Maxwell's reciprocal theorem
  • Knowledge of stiffness matrices in structural analysis
  • Familiarity with geometric non-linear analysis
  • Experience with beam elements in finite element modeling
NEXT STEPS
  • Explore the implications of Maxwell's reciprocal theorem in non-linear structural analysis
  • Investigate the properties of stiffness matrices in finite element methods
  • Learn about the behavior of cantilever beams under various loading conditions
  • Examine case studies involving geometric non-linear problems in structural engineering
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Structural engineers, researchers in finite element analysis, and students studying non-linear mechanics will benefit from this discussion.

svishal03
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As per Maxwell reciprocal theorem, it is valid only for elastic materials and structures indergoing small displacements.That is k12 = k21, kij = kji hence stiffness matrix is symmetric.

Howbver, I just have been going through MY OWN written programs for geometric non linear problems and I observe that stiffness matrix (assembled stiffness matrix) is well symmetric.

How can stiffness matrix be symmmetric for non linear behaviour of structures?
 
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Perhaps if you posted an example?

What elements do you have in your matrix?

kij is just a constant and therefore linear.
 
I have beam elements in my matrix. It is a cantilever beema with end moment.
 

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