Linear coefficient of thermal expansion

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SUMMARY

The coefficient of linear expansion (≡k) is defined by the relationship ΔL = LkΔT, where ΔL represents the change in length, L is the original length, and ΔT is the change in temperature. This definition is an approximation, as it does not account for the temperature dependence of k, which can lead to inaccuracies when calculating length changes. The discussion highlights that the Wikipedia article uses derivative notation for a more precise definition, indicating that the traditional interpretation with finite Δ's may not capture the full complexity of thermal expansion.

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Nathanael
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The "coefficient of linear expansion" (≡k) was defined in my book by the following relationship:
##\Delta L=Lk\Delta T##
Where L is length and T is temperature

I'm wondering, is this just an approximation? Because, if you were to increase the temperature by \Delta T and then calculate the new length, and then decrease the temperature by the same \Delta T and calculate the new length again, you would not get back to your original length.

Wouldn't the "symmetrical" definition of k be
##L_{f}=L_{0}e^{k\Delta T}##

This leads me to the question:
Is the reason they don't define it like this because the idea of 'linear thermal expansion' is not true to that degree of accuracy?
(In other words, finding the new length (to that accuracy) is not as simple as using a single constant?)
 
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Nathanael said:
not as simple as using a single constant?
It's temperature dependent, and generally so small that the dependence isn't measureable before things melt/decompose.
 
Nathanael said:
The "coefficient of linear expansion" (≡k) was defined in my book by the following relationship:
##\Delta L=Lk\Delta T##

That's only an approximation if we treat the \Delta's as finite, which is the traditional interpretation of \Delta's.

I notice the Wikipedia article defines the coefficient of linear expansion using the notation for derivatives. http://en.wikipedia.org/wiki/Thermal_expansion
 
Stephen Tashi said:
That's only an approximation if we treat the \Delta's as finite, which is the traditional interpretation of \Delta's.

I notice the Wikipedia article defines the coefficient of linear expansion using the notation for derivatives. http://en.wikipedia.org/wiki/Thermal_expansion

Thanks, I didn't see that. Everywhere I looked kept using \Delta L and \Delta T. Next time I'll be sure to check Wikipedia.
 
I think it was very perceptive of you to intuitively realize that it should, more precisely, be expressed differentially.

Chet
 
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