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Dynamic Data Analysis – v5.12.01 - © KAPPA 1988-2017

Chapter

3 – P ressure Transient Analysis (PTA)

- p72/743

Fig. 3.C.2 – Bourdet derivative, loglog plot

3.C.3

Bourdet Derivative & Infinite Acting Radial Flow (IARF)

When IARF occurs we have the approximation:

 

t

mp

 

sup '

Where m

is the slope of the semilog straight line. In the following the drawdown response is a

specific case of the multirate response, and the logarithm of time is the specific superposition

time for a drawdown. The derivative is therefore:

Derivative when IARF has been reached:

 

'

sup

'

m

t

d

pd

p



When IARF is reached, the derivative stabilized to a level equal to the slope of the semilog

straight line. This property was the main reason for the development of the derivative, as it is

easy and straight forward to identify IARF on the loglog plot, something which is virtually

impossible on the semilog plot. One can say that the derivative is a ‘magnifying glass’

of the

semilog behavior, conveniently placed on the same plot, used historically for type-curve

matching.

Combined with the early time unit slope during wellbore storage, the derivative provides an

immediate way to define the pressure and the time match on the loglog plot, just by

positioning a unit slope line on the wellbore storage regime and positioning the horizontal line

on the IARF response.

This alone would have made the Bourdet derivative a key diagnostic tool. The delightful

surprise was that the derivative could do much more, and that most well, reservoir and

boundary models carry a specific signature on the derivative response. It is this remarkable

combination that allowed the derivative to become

THE

diagnostic and matching tool in

Pressure Transient Analysis.