Hooke's law from first principles

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Hooke's law can be derived from first principles through an understanding of interatomic forces, specifically the balance between electrostatic attraction and Pauli repulsion. The energy around an equilibrium position can be expressed using a Taylor series, leading to the formulation of Hooke's law. While electrostatic models alone may not suffice due to limitations like Earnshaw's theorem, incorporating Pauli repulsion provides a viable explanation for atomic spacing in solids. Quantum mechanics explains Pauli repulsion, but classical mechanics can also account for nuclear electrostatic repulsion. Overall, the discussion highlights the interplay between quantum and classical models in understanding elasticity.
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Following a discussion in this forum, I have a question: Is it possible to derive Hooke's law from first principles?

I think a purely electrostatic model is not adequate: Earnshaw theorem would imply there's no "relaxed" position. Also, electrostatic forces get weaker with increasing distance, the opposite trend of spring forces.

Is my reasoning correct? Have I overlooked something? Is it possible to create a purely electrostatic model of elasticity?
 
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Absolutely. In solids, atoms sit at an energy minimum (specifically, electrostatic attraction balanced by Pauli repulsion) that governs interatomic spacing. The energy values E(x_0+\Delta x) around any minimum at x_0 can be expanded as a Taylor series,

E(x_0+\Delta x)=E(x_0)+\frac{\partial E(x_0)}{\partial x}\Delta x+\frac{1}{2}\frac{\partial^2 E(x_0)}{\partial x^2}(\Delta x)^2+\dots\approx \frac{1}{2}\frac{\partial E(x_0)}{\partial x}(\Delta x)^2

which is Hooke's Law where k=\partial^2 E(x_0)/\partial^2 x (taking E(x_0) as our energy reference and noting that \partial E(x_0)/\partial x is zero because we're at an energy minimum). Does this answer your question?
 
You Taylor series reminded me we may model spring forces with nearly any kind of forces - since Hooke's law is linear, many forces will fit it for suficiently small displacements.

So there's something that avoids the consequences of Earnshaw's theorem- Pauli Repulsion.
Is Pauli Repulsion explained with quantum mechanics? Or is there a way of modelling this repulsion using only classical mechanics?
 
Pauli repulsion is indeed explained with QM. And on the classical side, nuclear electrostatic repulsion may play a part too in controlling equilibrium atomic spacing, though I don't know offhand to what extent.

These effects are often modeled empirically with a repulsion term (e.g., in the http://en.wikipedia.org/wiki/Lennard-Jones_potential" ).
 
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