Fourier series: Difference between revisions
Jump to navigation
Jump to search
imported>Paul Wormer No edit summary |
imported>Paul Wormer No edit summary |
||
Line 13: | Line 13: | ||
In what sense it may be said that this series converges to ''f''(''x'') is a somewhat delicate question. However, physicists being less delicate than mathematicians in these matters, simply write | In what sense it may be said that this series converges to ''f''(''x'') is a somewhat delicate question. However, physicists being less delicate than mathematicians in these matters, simply write | ||
:<math>f(x) = \sum_{n=-\infty}^\infty c_n e^{2\pi inx/T},</math> | :<math>f(x) = \sum_{n=-\infty}^\infty c_n e^{2\pi inx/T},</math> | ||
and usually do not worry too much about the conditions to be imposed on the arbitrary function ''f''(''x'') for this expansion to converge to it. | and usually do not worry too much about the conditions to be imposed on the arbitrary function ''f''(''x'') of period ''T'' for this expansion to converge to it. |
Revision as of 08:42, 12 January 2010
In mathematics, the Fourier series, named after Joseph Fourier (1768—1830), of a complex-valued periodic function f of a real variable, is an infinite series
defined by
where T is the period of f.
In what sense it may be said that this series converges to f(x) is a somewhat delicate question. However, physicists being less delicate than mathematicians in these matters, simply write
and usually do not worry too much about the conditions to be imposed on the arbitrary function f(x) of period T for this expansion to converge to it.