Geology Reference
In-Depth Information
Now consider a linear, continuous system with impulse response h ( t ). By defin-
ition of the impulse response, if the input is a Dirac delta function, δ( t ), then the
output of the system is h ( t ). The Fourier transform of the Dirac delta function, δ( t ),
is unity (2.260). Thus, for this input, the Fourier transform of the output from the
linear system is H ( f )
·
1, where H ( f ) is called the system function . Because the
system is linear, at a given frequency its output is proportional to the input at that
frequency. If the input is g( t ) with Fourier transform G ( f ), the Fourier transform of
the output is
H ( f )
·
G ( f ),
(2.307)
the product of the two Fourier transforms. Therefore, by (2.269), the output o ( t )is
the convolution
o ( t )
=
h (λ)g( t
λ) d λ.
(2.308)
−∞
The autocorrelation of the output at lag τ is then
T /2
1
T
φ oo (τ)
=
lim
T →∞
h (λ)g( t
λ) d λ
T /2
−∞
h )g ( t
τ λ ) d λ dt
·
−∞
h (λ) h gg + λ λ) d λ d λ .
=
(2.309)
−∞
−∞
If the Fourier transform of the autocorrelation, φ gg (τ), considered as a lag domain
function, is S gg ( f ), its Fourier integral representation is
S gg ( f ) e i f τ df .
φ gg (τ)
=
(2.310)
−∞
Thus,
h (λ) h ) S gg ( f ) e i f + λ λ) dfd λ d λ .
φ oo (τ)
=
(2.311)
−∞
−∞
−∞
The Fourier transform of the impulse response is
h ( t ) e i ft dt ,
H ( f )
=
(2.312)
−∞
and its conjugate is
H ( f )
h ( t ) e i ft dt .
=
(2.313)
−∞
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