I was wondering if the Euler buckling method is simply theoretical or

In summary: Buckling of bars, plates, and shells In summary, the Euler buckling method is accurate in a real world scenrio, but it is not accurate for structures like thin walled tubes, plates, or shells.
  • #1
roanoar
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I was wondering if the Euler buckling method is simply theoretical or actually accurate in the real world. I am asking this both for complex structures and a simply compressed rod or beam.

Thanks
 
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  • #2


Hey Roanoar,

You asked a good question. As long as your column meets the numerous assumptions made in deriving the Euler buckling equations, then yes, this analysis method is accurate in a real world scenrio. I have studied buckling for about 2 years now and if you are interested in more information, I would be happy to assist you.

Also, http://books.google.com/books?id=Uz...resnum=3&ved=0CCkQ6AEwAg#v=onepage&q&f=false" is a great reference for you if you want to read (what I consider) the best book on buckling.

Hope all this helps and thanks for the question,

jrw66
 
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  • #3


It kind of depends what your interest is.

If you are a researcher studying actual failure by buckling then no, Euler is too simple for the real world.

If you are a designer, designing to codes, then the anti buckling requirements of most codes are based on Euler. So in that sense, in the real world, a code design is (hopefully) a safe design and probably uses Euler.

Remember that Euler is based upon a static load. Buckling induced by dynamic or periodic loads require different treatment.
 
  • #4


Thanks both of you very much.

jrw66- I can usually understand these things better upon working it out a little bit. So "made" a little bar with circular cross sections on the ends. It is .2m long and the diameter is .01m. So I found the equation Fcr=[pi^2*(Modulus of Elasticity)*(second moment of inertia)]/(kL)^2.
I am pretending the beam is structural steel so my E=2*10^11 Pa. I calculated the second moment of inertia to be I=pi*(diameter)^4/64=pi*(.01^-8)/64. I also used k=.5 because the beam has two fixed ends. The equation came out to
Fcr=[(pi^3)*(2*10^11)*(.01^-8)]/[(64)*(.5*.2)^2]=96894.6146N.

I hate to ask you to do calculations but I am just curious if my procedure is correct and if this would indeed be the force which would cause such a bar to buckle. Thanks.

Studiot-You said that Euler's only works with static loads but not periodic. If I added 100N on linearly over the period of a second would that be periodic or static?
 
  • #5


By static loads I mean those that are only loaded / unloaded a few times. A compression memeber in say an aircraft wing subject to continual fluttering will be subject to many load cycles. Yes one second is plenty slow wnough.

However for structural steel your slenderness ratio 0.2/0.005 = 40 is below the usual criterion (100) for applying Euler. So the critical stress will be the proportional limit.

A note to calculate the slenderness ratio this equals the effective length divided by the least radius of gyration of the section (=r/2 for circular) times a factor for end conditions. This factor is 1 for a hinge at each end, 0.5 for both ends fixed, 0.7 for one end fixed and one hinged, and 2 for one end free and one end fixed (flagpole)
 
  • #6


Thank you, you really have been a lot of help in having me understand buckling. You guys have already answered my question but if you're interested in responding please do... I was just wondering if Euler's Buckling still holds under thermal stress? From the readings I've done it seems like yes it does. The thermal force will be F=(coefficient of thermal expansion)*(modulus of elasticity)*(temperature change)*(cross sectional area). Theoretically I am thinking that by setting this equal to the buckling force I can calculate what temperature change will buckle it. But i am thinking that the expansion caused by temperature increases my change the buckling force due to something like a change in the cross sectional area. Will Euler's hold true to predict this temperature or will it be inaccurate.
 
  • #7


Things do buckle under thermal stresses, which can be quite large.

This sort of problem is more often seen in thin walled tubes, plates or shells where a more complicated analysis is appropriate when in plane forces are applied. With a plate there are usually three dimensions to consider. Euler is meant for columns and struts which are reduced to line beam ( 2 dimensional) analyses.

jrw66 has provided one reference.

The classics are
Timoshenko- Theory of plates and Shells
Southwell - theory of Elasticity
 

1. What is the Euler buckling method?

The Euler buckling method is a mathematical formula used to predict the critical load at which a slender structural element, such as a column or beam, will buckle or collapse under compressive stress. It was developed by Swiss mathematician Leonhard Euler in the 18th century.

2. Is the Euler buckling method only theoretical?

While the Euler buckling method is a theoretical approach, it has been extensively validated through experiments and is widely used in engineering design and analysis. However, it is important to note that it may not accurately predict the behavior of complex or non-ideal structures.

3. How is the Euler buckling method used in engineering?

The Euler buckling method is used to determine the maximum load a structural element can withstand before it buckles. This information is crucial in designing safe and efficient structures, such as buildings, bridges, and aircraft components.

4. Can the Euler buckling method be applied to all types of structures?

The Euler buckling method is most applicable to slender structures that are subjected to axial compression loads. It may not accurately predict the behavior of structures with complex geometries or those subjected to combined loading conditions.

5. Are there any limitations to the Euler buckling method?

While the Euler buckling method is a useful tool in structural analysis, it has its limitations. It assumes that the structural element is perfectly straight, homogeneous, and has a constant cross-section. It also does not take into account the effects of imperfections or material properties that may vary along the length of the element.

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