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by msandford
4035 days ago
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If you're dealing with bridges or buildings then you're right of course, you don't stress anything and you just let the stress dissipate through various movements. But thermal stresses are very small, for "normal" steel it's 13e-6 per degree C. If you figure that the temperature variations in CA aren't going to be more than say 40C (and that's probably too much) then you're looking at 520e-6 or basically 5e-4. As far as strain goes, that's not a terribly big number at less than 0.1% especially considering that most of the stress/strain graphs will go up to 10% or more and the first 1% are usually WELL within the linear elastic region. That means that you're talking about doing perhaps only using a few ksi of the steel's strength for the thermal effects. |
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ΔL=αΔtL; ΔL/L=αΔt; ϵ=ΔL/L; ϵ=αΔt; E=f/ϵ; f=ϵ/E; so f=αΔtE
ΔL = change in length due to temperature
L = restrained length
f = stress that arises due to full restraint
E = Young’s modulus
ϵ= strain
α= coefficient of linear thermal expansion
Using AASHTO numbers for structural steel:
f= 6.5x10^-6 (1/F)* 100 F * 29000 ksi = 18.85 ksi
That's a big chunk of the elastic 50 ksi range, and it's greater than a good portion of the allowable ranges from the table on page 41 of this PDF [1]. As you might already seem to know, AASHTO doesn't consider temperature loading for fatigue limit states, and in the Strength limit states it considers the force effects to be halved. (Though the displacement effects are multiplied by 1.2) Regardless, fully restraining these things at their ends doesn't seem like a good idea. Am I missing something in what you're talking about? Yes, the strain is low but fatigue generally works in terms of stresses.
[1] http://downloads.transportation.org/LRFDUS-6-Errata.pdf