Participating Associations:  American Association of Petroleum Geologists American Petroleum Institute Offshore Communications Society of Exploration Geophysicists
  Home       Business Directory       Articles       Jobs       Events       News      
 
SEARCH:    
  Advisory Panel     Associations     Links     Publications     About Us     Advertise     Testimonials     Contact Us  
 

Comment Title*:

Comment*:

Name*:
Email Address*:
Location*:

Add me to mailing list

I Agree to terms and conditions


Exploration & Production: The Oil & Gas Review - 2003, Volume 2


Order high-quality repints of any articles on this website

 

ARTICLES

Bilinear Pressure Signatures of Horizontal Wells
Professor Tom A Jelmert

Originally printed in:
Exploration & Production: The Oil & Gas Review - 2003, Volume 2

  1   2    3    4    5 

Methodology

It has been pointed out that bilinear flow often occurs unexpectedly for horizontal wells. (4) It was demonstrated that this effect could be caused by heterogeneities. Classic bilinear flow responses (straight line of quarter slope on a log-log plot) for horizontal wells could also be explained by rescaling of Cinco-Ley and Samaniego’s limiting equation5 for a finite conductivity fracture. (2) The straight lines, however, represent long-term solutions that may or may not be visible. In this article, the solution to the bilinear flow model is generalised to accommodate small time values. By use of the solution procedure of Cinco-Ley and Samaniego,5 the Laplace space solution for bilinear flow in the vertical plane was found to be:

Equation 1


for the wellbore pressure. The Laplace transformation of the time derivative may be obtained by s-multiplication.

Equation 2


Equations 1 and 2 may be inverted numerically by Stehfest’s algorithm. (6) For small time values, which correspond to large values of the Laplace variable s, the left-hand term within the parenthesis may be neglected in comparison with the right-hand term. Under the assumption that hpD = 2 a zwD, the following equation applies:

Equation 3


Equation 3 may be inverted to yield:

Equation 4


where 
The skin factor has been added to account for the difference between a well in the form of a line and a plane.

The logarithmic derivative becomes:

Equation 5


Equation 5 will present as a straight line with a quarter slope in a log-log co-ordinate system. From Equation 5 it may be concluded that the pressure derivatives from all reservoirs that are characterised by the same dimensionless co-efficient Cv will approach the same quarter slope straight line. The co-efficient will be referred to as the correlation factor of bilinear flow in the vertical plane.

Equation 6


In the same way, the Laplace space solution to bilinear flow in the horizontal plane was obtained as:

Equation 7


The Laplace transform of the pressure derivative may be obtained by s-multiplication.

Equation 8


For small values of s, which correspond to large time values, the left-hand term within the parenthesis may be neglected in comparison with the right-hand term,

Equation 9



which may easily be inverted to yield:

Equation 10



The logarithmic derivative becomes:

Equation 11


From Equation 11, the correlation factor of bilinear flow in the horizontal plane is obtained. The y-direction is parallel to the axis of the well and the x-direction is parallel to it.

Equation 12


It is advantageous to have the highest permeability perpendicular to the well. Hence, the correlation factor is usually < 1 The horizontal permeability ratio is the only parameter in Equation 8. Hence, Ch is the correlation factor during the entire bilinear flow period. Cv does not have this property.

The correlation factor will present as a parameter on a type curve designed for bilinear flow. Hence, the horizontal permeability ratio may be estimated by graphical type curve matching. The anisotropy ratio may be improved by subsequent automatic type curve matching (optimisation).

For large values of the Laplace variable s, which corresponds to small values of time, the second term in the parenthesis Equation 7 may be neglected. Subsequent inversion yields the equation for the conventional linear flow period.

  1   2    3    4    5 
Category:
Drilling & Well Services

 



Tom A Jelmert is Professor of Petroleum Engineering with the Norwegian University of Science and Technology (NTNU), Trondheim, Norway. He has worked with NTNU since 1985. From 1986 to 1997 he also held a position as Adjunct Professor of Mathematics and Physics at the Academy of The Royal Norwegian Air Force. Between 1978 and 1985 he was a research engineer with SINTEF, Trondheim. Professor Jelmert has been a guest scientist with the University of Tulsa, Oklahoma, in the period 1989 to 1990 and with the Colorado School of Mines from 2000 to 2001. He served as a member of the editorial board of the Journal of Petroleum Science and Technology from 1996 to 2002. Professor Jelmert holds a BSc in Electrical Engineering from Purdue University, Indiana and MSc and Dr Ing. degrees in Petroleum Engineering from the Norwegian Institute of Technology (NTH), Trondheim.


Copyright Touch Briefings 2008
 

Articles : a b c d e f g h i j k l m n o p q r s t u v w x y z
Companies : a b c d e f g h i j k l m n o p q r s t u v w x y z
Events : a b c d e f g h i j k l m n o p q r s t u v w x y z
Keywords : a b c d e f g h i j k l m n o p q r s t u v w x y z

Other Touch Group sites:    Touch Briefings Cardiology - Endocrine Disease - Neurology - Oncological Disease - Respiratory Disease Gastroenterology Disease -