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?
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?