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Complex Form of Fourier Series

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in the Figure below, and the amplitude and phase spectrum. ... whenever is integral so with the fourth, eighth, twelfth lines etc. are zero. ... – PowerPoint PPT presentation

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Title: Complex Form of Fourier Series


1
Complex Form of Fourier Series
For a real periodic function f(t) with period T,
fundamental frequency
where
is the complex amplitude spectrum.
2
The coefficients are related to those in the
other forms of the series by
Amplitude spectrum
Phase spectrum
3
Example Derive complex Fouries Series for the
rectangular form in the Figure below, and the
amplitude and phase spectrum.
4
Note that the plot is more complex than previous
examples of purely odd, or even functions.
5
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6
Where the sinc function is given by
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8
  • The harmonics are placed at intervals of 1/T,
    their envelop following the (modulus) of the sinc
    function. A zero amplitude occurs whenever
    is integral so with the
    fourth, eighth, twelfth lines etc. are zero.
    These zeros occurs at frequencies 1/t, 2/t , 3/t
    etc..
  • The repetition of the waveform produces lines
    every 1/T Hz and the envelope of the spectrum is
    determined by the shape of the waveform.
  • The term is a phase term dependent
    on the choice of origin and vanishes if the
    origin is in chosen in the center of a pulse. In
    general a shift of origin of ? in time produces a
    phase term of in the
    corresponding spectrum.

9
Useful deductions (i) For a given period T ,
the value of t determines the distribution of
power in the spectrum.
small t
1/t
1/T
large t
1/t
10
(ii) For a given value of pulse width t, the
period T similarly determines determines the
power distribution.
large T
small T
11
(iii) If we put Tt, we get a constant (d.c)
level. is then given by A sinc(n), so a
single spectral line of height A occurs at zero
frequency.
12
(iv) If we let the repetition period T become
very large, the line spacing 1/T become very
small. As T tends to infinity, the spacing tends
to zero and we get a continuous spectrum. This is
because f(t) becomes a finite energy signal if T
is infinite, and such signal have continuous
spectra.
13
(v) Suppose we make t small but keep the pulse
area A t constant. In the limit we get an impulse
of strength A t , and the spectrum will simply be
a set of lines of constants heights A/T.
14
(vi) Finally, it is clear tha a single impulse
will have a constant but continuous spectrum.
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