In the case of a flat function, all derivatives vanish at , i.e. for all . This means that a meaningful Taylor series expansion in a neighbourhood of is impossible. In the language of Taylor's theorem, the non-constant part of the function always lies in the remainder for all .
The function need not be flat at just one point. Trivially, constant functions on are flat everywhere. But there are also other, less trivial, examples.
Glaister, P. (December 1991), A Flat Function with Some Interesting Properties and an Application, The Mathematical Gazette, Vol. 75, No. 474, pp. 438–440, JSTOR3618627