# Proof 37: Elastic potential energy

In a spring that is elongated/compressed the distance $\Delta L=L_\text{end}-L_\text{relaxed}$, an elastic force (due to Hooke’s law) $F_\text{elastic}=k\Delta L$ is pushing/pulling on the surroundings in order to return the spring to its relaxed size. That force can thus supply energy to, or do work on, the surroundings; this energy was stored in it as elastic potential energy $U_\text{elastic}$. So, if we can find the work that can be done via the work formula, $W=Fd$, then we have the stored elastic potential energy.

Since the relaxed length is the situation of zero energy stored, let’s place our coordinate system at that point. Then $L_\text{relaxed}=0$, and the elongation/compression is $\Delta L=L_\text{end}-\cancel{L_\text{relaxed}}=L_\text{end}$.

The work formula $W=F_\text{elastic}\underbrace{\,\Delta L}_d$ has to be calculated during a very, very tiny moment, because the elastic force changes as we go. And then all those small portions of work must be added together. Such a tiny moment only gives a tiny displacement, so instead of $\Delta L$, let’s symbolise it $\mathrm dL$: $W=F_\text{elastic}\mathrm d L$. And we’ll sum them all up with an integral:

$$W=\int F_\text{elastic}\mathrm d L=\int kL\,\mathrm d L=\frac12 kL^2$$

The final $L$ value equals the final $L_\text{end}$, which was equal to $\Delta L$. So, we’ll swap $\Delta L$ back in instead of $L$. And finally, we’ll remember that the work that was found here is stored as elastic potential energy $U_\text{elastic}$ before being released. So:

$$U_\text{elastic}=\frac12 k\,\Delta L^2\qquad\blacksquare$$

## Proof 31: Elastic-collision speed “conservation”

We call a collision elastic if the total kinetic energy is conserved (same before as after the collision) and there are no other energies involved.…

## Proof 35: Kinetic energy

Linear version of kinetic energy A spaceship in outer space starts its rocket engines to propel itself forwards with a rocket force. That force does…

## Proof 36: Gravitational potential energy

Small falling object due to weight A flower pot falls down from a window sill due to gravity. This i because gravity does work $W_g$…

## Proof 32: Momentum conservation law

The moment conservation law and Newton’s 3rd law as well as the idea of impulse seem equivalent (they all describe impacts/collisions). And in fact the…

## Proof 14: Motion equations

In motion along a path, $a$ is acceleration, $v_0$ and $v$ are initial and final (current) speed, and $t_0$ and $t$ are initial and final…