The governing body, World Athletics, allows several slightly different shapes for a 400-metre track. The simplest lay-out consists of two semi-circles joined by straight lines. The radius of the semi-circles, measured to the inside edge of the track, is 36.5m. The straights are 84.39m long. We can easily check that these curves add up to a length of 400m, by computing \[ 2 \cdot \pi \cdot 36.5 + 2 \cdot 84.39 = 398.116\ldots \] Hang on… This is no mistake! The official distance is measured 30cm away from the inside edge of the track. If we take this into account, the radius of the semicircles increases to 36.8m, and we find \[ 2 \cdot \pi \cdot 36.8 + 2 \cdot 84.39 = 400.001\ldots \] Close enough, I suppose… I’ll just round everything to two decimal places from now on. Still, this means that if a runner manages to stay close to the inside edge, they may be able to complete a lap in less than 400m!
Where are the start lines?
The lanes on an athletics track are numbered 1 to 8 (or however many lanes there are), starting from the inside. To make a race fair to those running further from the inside of the bend, the starting positions in different lanes are staggered.
The width of a lane is 1.22m, or 4 feet. So while a bend in lane 1 is $36.80 \pi \approx 115.61$ metres long, the same bend in lane 2 has a length of $38.02 \pi \approx 119.44$ metres. Each time we move one lane further out, the bend gets longer by $1.22 \pi \approx 3.83$ metres. (I’m ignoring some weird technicalities here, concerning where exactly the official distance is measured in each lane.)
In a 200m race, where the athletes run one bend and one straight, the runner in lane 2 starts 3.83m ahead of the one in lane 1. In each lane further out, the start line is again 3.83m ahead of the start line in the previous lane. In the 400m, runners navigate both bends to complete one lap of the track, so the starts are staggered by twice the distance, 7.67m per lane.
In the 800m, the situation is a bit more complicated, because athletes are allowed to break out of their lane after the first bend. Their staggered start is similar to that of the 200m, but needs to be corrected to account for the distance from where the runners leave their lane to the inside of the next bend.
Why do laps get longer?
To compute that a lap gets longer by 7.67m each time we move a lane further out, we assumed that the track consists of straight lines and semi-circles. This is true for one of the standard track layouts, but World Athletics allows slightly different shapes as well. Luckily, the answer doesn’t change if the track is a different shape. As long as over the course of a lap we turn a total of $360^\circ$, then moving some distance $d$ outwards increases the length of lap by $2 \pi d$. However, if the track were a figure of eight, then we would turn just as much to the left as to the right, so there the net turning angle would be zero. This means that every lane would be exactly the same length, avoiding the need for a staggered start.
Curved start lines
In the longer distances (such as the 1500m, 5000m and 10,000m), runners are not bound to any specific lane. Does that mean that the start line should be a straight line perpendicular to the lanes? No! Because that would still put runners on the outside at a disadvantage: they would have to cover more distance in order to reach the inside edge of the track. To obtain the actual shape of the start line, first imagine winding a rope (shown in blue) around the inside edge of the bend.
Next, pull the end of the rope to the outside of the track, so that the rope starts unwinding, but remains taut. The curve traced by the endpoint of the rope is the start line (shown in orange). Since the length of the rope does not change, this guarantees that each runner will have exactly the same distance to cover.
The curve obtained this way is called the involute of the curve the rope was wrapped around. Because the start lines for the 5000m and 10,000m are positioned at the start of a semi-circular bend, their shape is that of the involute of a circle. If we continue drawing the involute of a circle beyond the width of the track, we get a spiral. If we draw several involutes on the same circle they have the satisfying property that the strips between them are of constant width.
Some other curves have aesthetically pleasing involutes. My favourite is the cardioid, whose involute is a cardioid that is three times as large and rotated by $180^\circ$. Here too, we could think of the involute as a start line. If you have to run from the blue cardioid to the cusp of the green shaded cardioid, without going into the shaded area, the distance you have to travel is independent of where on the blue cardioid you start!
Involute gears
As a sports fan I hate to admit it, but the most interesting application of the involute of a circle has nothing to do with athletics. It occurs in mechanical transmission. The teeth of gears are often made such that their sides are involutes of a circle. This leads to a smooth transmission of force between the two gears, which is not the case with other tooth shapes!
For example, consider a gear with angular teeth (shown in orange):
When two such gears engage, there will almost always be a a corner of one tooth driving the other gear (pink circles). This causes several issues. One issue is that the corners would wear down very quickly. Another is that there would be vibrations in the transmission, because the point of contact jumps all over the place as the gears rotate against each other:
In an involute gear (shown in blue), the sides of the teeth are involutes of a circle called the base circle (black):
The base circle is larger than the physical disk the teeth are mounted on. A few of its involutes are shown in red, matching the profile of the teeth. The force between two involute gears is always transmitted along the same line (pink), tangent to the base circles of both gears. The contact point (circled in pink) moves steadily along this line as the gears rotate.
You can imagine that the two gears are connected by a piece of string that is unwinding from one gear while winding onto the other gear. The relative motion of the string and one of the gears is exactly the same as the relative motion of the rope and the athletics track when we were marking out the 10,000m start line. But now we are in a frame of reference where, instead of moving the rope/string sideways to unwind it, we are rotating the track/gear and pulling the rope/string.
By imagining this string, we see that the torque is transmitted as if the two wheels were connected by a drive belt instead of having interlocking teeth. This implies that the gear ratio (the ratio of the angular velocities of both gears) stays exactly the same throughout the motion. In particular, there is no sudden jolt when the next corner of a tooth catches. Theoretically, the transmission is perfectly smooth.
The shape of the teeth of an involute gear depends on the size of the base circle of that gear, but not on the size of the gear we pair it with. The only things that need to be standardised are the ‘pitch’ (how far apart consecutive teeth are) and the ‘pressure angle’ (which relates to the distance between the base circles of two engaged gears). If we have a set of involute gears in various sizes, each with the same pitch and pressure angle, we can pair any two to build a smooth transmission.
With these benefits, it should come as no surprise that many of the gears you’ll find in real-world machines (or in a Lego set) are involute gears.
I wonder if somewhere in the world there is a big machine containing a gear with a base circle radius of 36.5m. Then you could bring this giant gear to an athletics track and perfectly align one of its teeth with the start line. Sadly, the largest gear I could find any concrete information about, though it weighs a whopping 73.5 tonnes, has a radius of less than 7m. So, if you manage to find a 36.5-metre gear to bring to your local running track, please remember to lift with your legs, not your back!
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