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kalapuikko
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jepe said:Try this: http://www.aps.anl.gov/asd/me/Calculators/ElasticBeam2.html
It does not show any equations, but gives you quick result
ChaosKnight said:You can work out the solution analytically.
The first portion L2 of the beam is easy enough. You only have a shear force from the support to give moments. Get the moment equation, integrate it to get displacement as a function of x. Obtain also the moment M1 at the point where q starts, ie beginning of L1.
Next obtain the moment equation for length L1. Remember to add the moment M1 at the beginning of L1. Integrate this equation.
Now, the 1st equation tells you the displacement and gradient of the beam at the end of L2 and where L1 starts. This must be matched when you solve the 2nd equation for L1. Essentially this means solving for the constants after integrating twice.
After this you're done.
kalapuikko said:Thank you!
Can you help is the answer before solving constants something like in picture? And then, how do I solve constants? (F is force from support)
Well, in first equation I get atleast this..
v(0)=0 -> C2=0
ChaosKnight said:You've got the gist.
Since v=0 at x=0, C2 = 0
And using symmetry, dy/dx = 0 at x=(L1/2 + L2). Use this to solve for C3.
Now just equate the vertical displacements and gradients at the point where q starts to solve for your remaining constants. 2 unknown constants, 2 equations, and you're done.
kalapuikko said:Thank you!
Can you help is the answer before solving constants something like in picture? And then, how do I solve constants? (F is force from support)
Well, in first equation I get atleast this..
v(0)=0 -> C2=0
Nice...Mech_Engineer said:This post has sort of had me transfixed for a while, so I finally decided to try solving the probem using MathCAD. The answers I came up with seem to at least make sense, but as was mentioned before it is VERY easy to make one small mistake that follows you through to the end.
The final solution I came up with is:
[tex]\delta_{max}=\frac{qL^4+16qa^4}{384EI}[/tex]
This is the maximum deflection along the entire beam, which ends up in the middle due to the symmetric loading condition. Suffice to say it was a LOT of work to get there.
FredGarvin said:Nice...
Mech_Engineer said:This post has sort of had me transfixed for a while, so I finally decided to try solving the probem using MathCAD. The answers I came up with seem to at least make sense, but as was mentioned before it is VERY easy to make one small mistake that follows you through to the end.
The final solution I came up with is:
[tex]\delta_{max}=\frac{qL^4+16qa^4}{384EI}[/tex]
This is the maximum deflection along the entire beam, which ends up in the middle due to the symmetric loading condition. Suffice to say it was a LOT of work to get there.
kalapuikko said:Anyway, I think that equation that prex and mrMikee have found in thread http://www.eng-tips.com/viewthread.cfm?qid=158137&page=10 is more correct, maybe I shold buy/borrow Bloddgett and see how it´s evaluated.
kalapuikko said:I´m still working with the case of different EI in L2 and L1. I hope I get them with your help. Thank you!
kalapuikko said:I must say thoug, I don´t believe it´s correct. If a=0, you get qL^4/384EI which is five times smaller than known 5qL^4/384EI. Anyway, I think that equation that prex and mrMikee have found in thread http://www.eng-tips.com/viewthread.cfm?qid=158137&page=10 is more correct, maybe I shold buy/borrow Bloddgett and see how it´s evaluated.
kalapuikko said:I´m still working with the case of different EI in L2 and L1. I hope I get them with your help.
Mech_Engineer said:Yeah, I had noticed that discrepancy too. it turns out my boundary conditions weren't quite right. When I changed the last boundary condition from the slope being zero in the middle to the bending moment being defined in the middle, everything worked out.
[tex]\delta_{2}(x)=-\frac{qL^3x-6qLa^2x-2qLx^3+qa^4+6qa^2x^2+qx^4}{24EI}[/tex]
[tex]\delta_{max}=-\frac{5qL^4-24qL^2a^2+16qa^4}{384EI}[/tex]
Mech_Engineer said:Now THAT gets really ugly...
[tex]E_{1}[/tex] and [tex]I_{1}[/tex] are in section 1 (left hand side)
[tex]E_{2}[/tex] and [tex]I_{2}[/tex] are in section 2 (middle)
[tex]E_{3}[/tex] and [tex]I_{3}[/tex] are in section 3 (right hand side)
The beam deflection equation is a mathematical formula used to calculate the amount of deflection in a beam under a specific load. It takes into account the material properties of the beam, the type of support it has, and the applied load.
The beam deflection equation is derived using principles of mechanics, specifically the theory of elasticity. It involves solving differential equations to determine the deflection of a beam at various points along its length.
The accuracy of the beam deflection equation is influenced by several factors, including the assumptions made in its derivation, the type of loading applied, and the material properties of the beam. It is important to carefully consider these factors when using the equation in engineering applications.
No, the beam deflection equation is only valid for certain types of beams, including beams with constant cross-sections and straight edges. It is not applicable to curved or tapered beams, as well as beams with varying cross-sections.
Yes, there are limitations to using the beam deflection equation. It assumes that the beam is made of a homogeneous and isotropic material, and that it is under small deflections. It also does not take into account other factors such as shear and torsion, which may affect the behavior of the beam.