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