Fourier Series of part of 1 Sinusoid.
Cuthbert Nyack
If a part f(t) between T1 and T2 of a sinusoid with frequency w is used to find the Fourier series of the
sinusoid, would the calculation give a spectrum containing only
1 line at w?
The Fourier Series coefficients are given by:-
As the following applet shows, the "correct" result is only
obtained if w = 2p/T is a multiple of the
fundamental frequency 2p/(T2 - T1).
ie w = nwf or 2p/T =
n2p/(T2 - T1) or
(T2 - T1) = nT.
This is a consequence of the Fourier Series calculation assuming
a periodic signal. If a periodic signal is constructed by adding
f(t ± n(T2 - T1)) to f(t), then the correct spectrum is
obtained if the constructed periodic signal is identical to
the sinusoid. In the applet below the correct result is
obtained when the green f(t) and yellow f(t - (T2 - T1)) plots join
smoothly at the boundary.
Fn = 1 shows the effect for T1, T2 and
w.
Fn = 2 to 9 show special cases where (T2 - T1) contains an
integral number of periods.
In these cases the spectrum
consists of a single line at the frequency of the sinusoid.
For Fn = 7, w = 6 and the white text
is showing that c(10) has magnitude 1.0000 and frequency 6.0011.
(The accuracy is limited by the resolution of T1 and T2).
Fn = 10 to 13 show special cases where (T2 - T1) contains an
odd number of half periods.
In these cases the spectrum
does not contain a component at the frequency of the sinusoid.
For Fn = 13, w = 5.7 and the white text
is showing that
the largest components in the spectrum are
c(6) with magnitude 0.6556 and frequency 5.2578 and
c(7) with magnitude 0.61949 and frequency 6.1342.
Fn = 14 and 24 shows what happens as the number of periods
increases from 7 to 8 with
w
kept constant at 6.0 and T2 is varied.
Fn = 25 and 35 shows what happens as the number of periods
increases from 7 to 8 with
T1, T2
kept constant at 0.01 and 7.34 and w is varied.
This effect is more familiar with the DFT but is a feature of any
discrete frequency(or assumed periodic) transform. There is no
sampling here. When sampling is introduced the spectrum
becomes periodic.
Return to main page
Return to page index
COPYRIGHT © 2007,2012 Cuthbert Nyack.