Cantilever beam: cubic stiffness question

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SUMMARY

The discussion centers on the analysis of a cantilever beam's stiffness under varying loads. For small forces, the maximum deflection is expressed as δ = (P l³) / (3 E I), leading to an equivalent stiffness of K_eq = (3 E I) / (l³). However, for large forces and deflections, the equivalent stiffness exhibits cubic relationships with deflection. Participants seek references to derive the cubic force-deflection relationship, emphasizing the need to move beyond linear theory due to significant displacements.

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  • Understanding of cantilever beam mechanics
  • Familiarity with static equilibrium principles
  • Knowledge of material properties such as Young's modulus (E) and moment of inertia (I)
  • Basic differential equations related to beam deflection
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Structural engineers, mechanical engineers, and students studying advanced mechanics of materials who are interested in the behavior of cantilever beams under varying loads.

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Hello.

Supose that we have a cantilever beam.
For a small force P applied at the free side of the beam, we can find an expression for the maximum deflection:

\delta=\frac{P l^3}{3 E I}

If we want to use this beam as a string, we can find its equivalent stiffnes noting that P=K_{eq} \delta, so

K_{eq} = \frac{3 E I}{l^3}

In the case of large forces (and large deflections), it is known that the equivalent stiffness will have cubic powers of the deflection. Does anyone know a good reference on how to find the expression for this new relation force versus deflection with the cubic terms?
 
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Do you mean the equations for the vibration of a cantilever?

EI{\left( {\frac{{{\partial ^3}y}}{{\partial {x^3}}}} \right)_{x = L}} = - P\left( {\frac{{{\partial ^2}y}}{{\partial {t^2}}}} \right)

EI{\left( {\frac{{{\partial ^2}y}}{{\partial {x^2}}}} \right)_{x = L}} = 0
 
No, it is a static case where the displacement is large enough to invalidade the linear theory, which permits us to find the traditional deflection and equivalent stiffness expressions.
 

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