N.B. A detailed on-line essay by S. Finch
was the starting point for this entry.
Let a piecewise smooth function 
 with only finitely many discontinuities (which are all jumps) be defined on 
 with Fourier Series
![\begin{displaymath}
S_n(f,x)={\textstyle{1\over 2}}a_0+\left\{{\sum_{k=1}^n [a_k\cos(kx)+b_k\sin(kx)]}\right\}.
\end{displaymath}](w_973.gif)  | 
(3) | 
 
Let a discontinuity be at 
, with
  | 
(4) | 
 
so
![\begin{displaymath}
D\equiv \left[{\,\lim_{x\to c^-} f(x)}\right]-\left[{\,\lim_{x\to c^+} f(x)}\right]>0.
\end{displaymath}](w_976.gif)  | 
(5) | 
 
Define
![\begin{displaymath}
\phi(c)={1\over 2} \left[{\,\lim_{x\to c^-} f(x)+\lim_{x\to c^+} f(x)}\right],
\end{displaymath}](w_977.gif)  | 
(6) | 
 
and let 
 be the first local minimum and 
 the first local maximum of 
 on either side of
.  Then
  | 
(7) | 
 
  | 
(8) | 
 
where
  | 
(9) | 
 
Here, 
 is the Sinc Function. The Fourier Series of 
 therefore does not
converge to 
 and 
 at the ends, but to 
 and 
. This phenomenon was observed by Wilbraham (1848) and
Gibbs (1899).  Although Wilbraham was the first to note the phenomenon, the constant 
 is frequently (and unfairly)
credited to Gibbs and known as the Gibbs Constant.  A related constant sometimes also called the Gibbs
Constant is
  | 
(10) | 
 
(Le Lionnais 1983).
References
Carslaw, H. S.  Introduction to the Theory of Fourier's Series and Integrals, 3rd ed.  New York: Dover, 1930.
Finch, S.  ``Favorite Mathematical Constants.''  http://www.mathsoft.com/asolve/constant/gibbs/gibbs.html
Le Lionnais, F.  Les nombres remarquables.  Paris: Hermann, pp. 36 and 43, 1983.
Zygmund, A. G.  Trigonometric Series 1, 2nd ed.  Cambridge, England: Cambridge University Press, 1959.
© 1996-9 Eric W. Weisstein 
1999-05-26