Can we derive Hooke's law from the theory of elasticity? I know it is not a fundamental law and therefore can be derived from more basic considerations.


Yes, we can derive Hooke's Law from more basic continuum conditions, provided that the material be stable and at equilibrium, so that the strain energy is smoothly minimized with respect to the distance between atoms. (This energy is sometimes called the pair potential and is modeled using functions such as the Lennard-Jones potential.)

Consider just a pair of atoms. For slight positional deviations $\delta$ (corresponding to the small-strain assumption of linear elasticity) around the smooth energy minimum $E(0)$, the energy $E$, regardless of its true functional form, can be expanded using a Taylor series:


where the prime notation denotes derivatives with respect to position. Now let's set our energy reference to $E(0)=0$, note that $E^\prime(0)=0$ because we're at an energy minimum, and drop all but the very next term. This gives


which describes the energy of an idealized spring with spring constant $E^{\prime\prime}$ and displacement $\delta$; the derivative of this equation with respect to position provides the restoring force, which is

$$F(\delta)\approx E^{\prime\prime}(0)\delta.$$

Now define stress as $\sigma=F/A$ and engineering strain as $\epsilon=\delta/L$ and we have $$\sigma=\frac{LE^{\prime\prime}(0)}{A}\epsilon$$ or $$\sigma=Y\epsilon,$$

which is simple Hooke's Law for a corresponding elastic modulus $Y$.

  • $\begingroup$ You actually derived Hooke's law from Lennard-Jones potential and then you derived elasticity from Hooke's law. $\endgroup$
    – Diracology
    May 29 '18 at 18:53
  • 4
    $\begingroup$ I specifically noted that one does not need to use the Lennard-Jones potential or any specific potential; it's sufficient to assume that the substance is initially at a stable equilibrium. That's the beauty of a Taylor series expansion; it proves that every smooth minimum looks like a parabola from up close. A parabolic energy response is equivalent to a spring-like response. $\endgroup$ May 29 '18 at 18:59
  • $\begingroup$ That derivation works for materials that doesn't have any imperfections. Like perfect crystals. $\endgroup$
    – nicoguaro
    May 29 '18 at 19:10
  • 1
    $\begingroup$ It works pretty well until vacancies/impurities start to make up a fair fraction of the atomic volume fraction. Small amounts of imperfections in crystals generally have much more of an effect on strength than on stiffness. $\endgroup$ May 29 '18 at 19:36

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