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

Chapte

r 2 – T heory

- p54/743

The principle of traditional real gas analysis is to replace the pressure by the pseudopressure

and interpret the data as if the fluid was slightly compressible.

However, there is an important shortcoming in this method. Although the equation looks the

same, it will only be linear as long as we can consider the diffusion term k/



c

t

constant. This

is valid as long as the average reservoir pressure does not substantially decrease which is a

reasonable assumption for a standard, relatively short, well test. In the case of extended tests

such as limit tests and production well tests, this may not be the case.

2.I.3.b

Normalized pseudopressures

The gas diffusion equation remains valid if we multiply the pseudopressures by a fixed

number. Because the unit and orders of value of the standard pseudopressures are not

intuitive, one possibility is to use normalized pseudopressures by selecting a reference

pressure p

ref

, with the condition:

Normalized pseudopressures:

 

 

 

ref

ref

Norm

pm

pm

p p m

Normalized pseudopressure at:

p

ref

:

 

ref

ref

Norm

p p m

The normalized pseudopressures have the dimension and unit of the pressure, it follows the

same diffusion equation and it coincides with the pressure at p

ref

:

Normalized pseudopressures:

) (

0002637

.0

) (

2

p m

c

k

t

p m

Norm

t

Norm

2.I.4

Non-Darcy flow

The diffusion equation used as the basis of the methodology in Dynamic Data Analysis is based

on three components: the conservation of mass, a PVT equation and Darcy’s law. We have

seen above that the gas PVT required some adjustments in the equations and the method:

pseudopressures, changing storage, material balance. In complement there are some cases,

and especially for gas, where the assumption of Darcy flow is invalid. Sections of the reservoir,

generally close to the well, will flow at such speed that turbulence will occur and have a strong

impact on the well response. We now need to add a turbulence component to the flow

equation, replacing Darcy’s law by a second degree equation, such as Forchheimer’s.

Darcy’s law expressed in terms of speed, in SI units:

u

k x

P

 

Forchheimer’s equation, same references and units:

2

u

u

k x

P

    

is called the turbulence factor. There are two main options to address non-Darcy flow:

The first is to focus on the impact of non-Darcy flow on the well productivity. This is what

was done historically using rate dependent skin. Normal diffusion is used, but an additional,

rate related skin component is added.

The other way is to model non-Darcy flow by numerically integrating the Forchheimer

equation in the model.