Time differentiation and
integration of Fourier Transform
(Cand.
Real.
Integration
(divide with iw) is the opposite, thus time differentiation and time
integration are examples of high-pass and low-pass filters respectively. The
geology of the seismic structure can by means of certain velocity functions
differentiate or integrate a seismic wavelet. Differentiation emphasizes the high frequencies over the low
and integration the low over the high. In general the locations of a
Fig.1.gives
an example of the Ricker wavelet 50 Hz centerfrequency - original (a),
differentiated (b) and integrated(c).



Fig.1. a)original
b)Differentiated c)Integrated wavelet


Fig.2. a)reflectivity convolved with original
b)Differentiated
Differentiation
is accomplished on the reflectivity series fig.2 convolved with the
differentiated Ricker wavelet. It is an analog with using a high-pass filter on
the series. In this way the geologic structure can act as a filter.
Differentiation of a seismic trace is straightforward and easy to visualize.
Integration is more complicated to visualize. In order to understand what
division by iw means, suppose a seismic trace is composed of a time-invariant
source wavelet that is convolved with a
reflectivity function, a generally-accepted good first approximation. If
this trace is convolved with a unit step function generated by:
UnitstepFuction
= Table [1,Length[seismicTrace]]
Then the
result is the same as you would get if an integrated source wavelet left the
source and was reflected from those same reflection coefficients.

Fig.3. a)reflectivity convolved with original and the
result convolved with unit step. b) reflectivity convolved with integrated
wavelet. We got the same result as a).