What is Equivalent Stiffness of a Beam?

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Discussion Overview

The discussion revolves around the concept of equivalent stiffness of a beam, particularly focusing on cantilever beams under applied loads and moments. Participants explore the relationship between beam deflection, slope, and the interpretation of equivalent stiffness in terms of linear springs.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Mathematical reasoning

Main Points Raised

  • One participant defines equivalent stiffness as the stiffness of a linear spring that deflects the same amount under the same load, specifically for a cantilever beam with a load P and deflection δ.
  • Another participant clarifies that θ represents the local slope at the free end of the beam, and that the relationship between slope and displacement depends on the beam's length, independent of E or I.
  • A later reply confirms that knowing the moment at a location allows for the calculation of the slope of the beam at that point due to the moment.
  • Further contributions explain that the cantilever tip rotational stiffness is equivalent to a linear torsional spring with a spring constant kθ = E*I/L, and that the tip transverse deflection stiffness is equivalent to a linear translational spring with k = 2*E*I/L².

Areas of Agreement / Disagreement

Participants generally agree on the definitions and relationships regarding equivalent stiffness, local slope, and deflection, but there is ongoing exploration of the implications and calculations involved.

Contextual Notes

The discussion includes assumptions about beam properties and the geometrical relationships that may not be fully resolved, particularly regarding the dependence on beam length and the effects of applied moments.

boeing_737
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Hi all,

I am trying to understand the concept of equivalent stiffness of a beam. As I see it, the equivalent stiffness is the stiffness of a linear spring that would deflect the same amount under the same load. For a cantilever beam with a load P and a deflection \delta at the free end, if we just look at the deflection of the free end, and somehow lump the stiffness and elastic properties of the beam into the term k_{eq}, it's motion will be the same as a linear spring with stiffness k_{eq} when the same load P is applied to the spring.

My vibrations textbook mentions the k_{eq} for a cantilever with a moment applied to the free end as \frac{EI}{L}. Assuming that the spring being considered is a linear torsional spring, how do we interpret this? I am thinking it goes something like - 'The equivalent stiffness of a cantilever beam with a moment at the free end is the stiffness of a linear torsional spring that would coil by an angle say \theta when the same moment is applied to it.' Now, is \theta the same as the tip deflection \delta or is it the local slope at the free end ie \theta \approx \tan(\theta) = \frac{dy}{dx}

Thanks a lot for the help!

PS - Any suggestions for books that explain the equivalent stiffness concept well?
 
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\theta is the local slope at the free end.

Of course there is also a displacement at the free end, which you can find from the fact that the curvature of the beam is constant. The geometrical relationship between the slope and the displacement at the free end will depend on the length of the beam, but not on E or I.
 
AlephZero said:
\theta is the local slope at the free end.

Of course there is also a displacement at the free end, which you can find from the fact that the curvature of the beam is constant. The geometrical relationship between the slope and the displacement at the free end will depend on the length of the beam, but not on E or I.

Sorry for the late response.

Thanks for clarifying that. Also, does that mean that if we know the moment acting at a location x, we can calculate the slope of the curved beam at that point due to the moment?
 
boeing_737: Regarding post 3, yes, it does. Regarding post 1, you have a cantilever having an applied tip moment, M. As AlephZero mentioned, the cantilever tip rotational stiffness is equivalent to a linear torsional spring at the cantilever tip having spring constant ktheta = E*I/L. The cantilever tip slope is theta = M/ktheta.

Also, the cantilever tip transverse deflection stiffness is equivalent to a linear translational spring at the cantilever tip having spring constant k = 2*E*I/L^2. The cantilever tip transverse deflection is delta = M/k.
 

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