The tautochrone is the curve in which a ball, positioned anywhere on the curve, will take the same time to arrive at its lowest point.

In a physical model where uniform gravity is the only force acting on the ball, the tautochrone curve is a *cycloid *(the curve described by a fixed point in a rolling circle), as correctly proven by Huygens in 1673 [BOYDE] using pure geometric arguments. We are going to present two different ways to arrive at this result.

## A wild guess.

Let be the curve of interest and consider any partition of it (finite or infinite) in points such that is the highest point in the partition, the second highest and so on. Let be a ball positioned at point of the partition. Assume is the highest point of the curve, as in the figure. Further, every ball arrives at the lowest point at time .

We also have the following equalities:

The very first observation one can come up with is that the acceleration function must be non-negative and strictly decreasing. We are ready to make a wild guess.

Let and two balls positioned on the curve with such that:

One way to impose and to arrive at the lowest point at the same time is to write:

So we have that the distance traversed by will always be times the distance traversed by . Since both balls start with zero speed, we can also derive the expression of its acceleration:

It is reasonable to guess that the ball’s acceleration will depend on its position on the curve. Let’s assume we can write the equation for the acceleration in terms of the -coordinate

where is a weight function. The simplest possibility for is a constant

Substituting with the actually acceleration function of our model

Derivating both sides

Then we have the following separable differential equation

Using the identity

Finally,

We still have to find an equation for .

From equation (1):

Integrating on both sides

In summary

the equation of a cycloid.

A different source of inspiration could come from harmonic oscillations. For small angles, the movement of a pendulum can be modeled as

where is the length of the chord. The solution is given by

where is the amplitude, i.e., the maximum angle the pendulum forms with the vertical axis. Notice the period of the harmonic pendulum does not depend on the amplitude. This is exactly the property we want for the tautochrone. Hence, the solution of the differential equation:

is a tautochrone curve.

## Derivation with no guesses.

Although correct, the given solution may not satisfy everyone. It was more a guess than a derivation. In particular, we are not able to ask if there exists a different solution from a cycloid or not.

Consider the model in the next figure. A ball is positioned on curve at height . Define

From the principle of conservation of energy we know that:

Therefore, the time for a ball positioned at height is given by:

We want that the time a ball takes to arrive at the lowest point is independently of its starting height. Therefore . We can solve the problem by applying the Laplace Transform.

where . The Laplace Transform of is easily computed.

By using the substitution one derives

The last integral can be computed and gives the value . Therefore,

Hence,

By observing .

And now it rests to us to solve the differential equation:

Using the substitution .

## Further Readings

**[1] – Boyce, W.E. and DiPrima, R. C. Elementary Differential Equations.
[2]**–

**Ballard**, Joel.The simple harmonic pendulum. [Link].

**[3]**–

**Tee**, Garry J. Isochrones and brachistochrones. [Link]