returns the number whose fifth power is 1. Because is odd, a value exists for negative arguments as well, so the domain is the whole real line. Even roots, by contrast, are defined only for .
A negative number has a real fifth root because multiplying a negative number five times leaves the sign negative, which is exactly what fails for a fourth root or a square root.
Needing to reach before the value reaches is a vivid measure of how slowly it grows.
Writing , the derivative is . The denominator is positive whenever , so the function increases everywhere. As we get , so the curve rises steeply through the origin and then flattens out on both sides.
The second derivative is .
| Range of | Concavity | |
|---|---|---|
| negative | concave down | |
| positive | concave up |
The derivative is undefined at the origin, but the bending genuinely does reverse there, so it counts as an inflection point with a vertical tangent.
Solving for gives , so the inverse is the quintic , and the two graphs are reflections of each other in the line . Where lies flat near the origin and shoots up far away, the fifth root stands up near the origin and lies down far away, exactly as a mirror image should.
It meets at and .
| Range of | Which is closer to zero |
|---|---|
At we have against . Higher roots flatten the graph further, tending in the limit toward a horizontal line at height for . The fourth root, meanwhile, cannot be drawn for at all.
Abel and Ruffini showed that the general quintic equation cannot be solved using arithmetic and radicals2, yet the simplest case, , is solved by a radical itself, and this function supplies that solution.
In physics the radius of a blast wave is given in terms of the energy, the time and the density as follows3.
Taylor famously used this one-fifth power law to deduce the yield of a nuclear test from nothing but published photographs.