Abstract
In order to clarify reservoir characteristics and identify pressure build-up characteristics resulting from the offset effect, well test models of bottomhole pressure in the multi-well system of infinite homogeneous and double porosity reservoirs were derived in consideration of effective radius. For a testing well in the model, skin and wellbore storage effect were considered, while for offset wells, skin and wellbore storage were ignored. The exact solution to Bessel function in the Laplace space was derived with Laplace transform method. Two-type curves were plotted for offset wells being online or offline simultaneously. In addition, characteristics of the type curve were analysed and the method for pressure build-up analysis was established. Under both scenarios mentioned above, long-term asymptotic solutions show that the curves of the pressure derivative rise stepwise, and there appears a multi-radial flow stabilization line. The ratio of height of each stabilization line to that of the first stabilization line is the algebraic sum of the dimensionless production combining the testing well and the effective offset wells. In the meanwhile, the curves of pressure derivatives descend under the scenario of the testing well build-up when the offset wells are producing simultaneously.
Copyright 2017, Shaanxi Petroleum Society.
This paper was prepared for presentation at the 2017 International Field Exploration and Development Conference in Chengdu, China, 21–22 September 2017.
This paper was selected for presentation by the IFEDC&IPPTC Committee following review of information contained in an abstract submitted by the author(s). Contents of the paper, as presented, have not been reviewed by the IFEDC&IPPTC Committee and are subject to correction by the author(s). The material does not necessarily reflect any position of the IFEDC&IPPTC Committee, its members. Papers presented at the Conference are subject to publication review by Professional Committee of Petroleum Engineering of Shaanxi Petroleum Society. Electronic reproduction, distribution, or storage of any part of this paper for commercial purposes without the written consent of Shaanxi Petroleum Society is prohibited. Permission to reproduce in print is restricted to an abstract of not more than 300 words; illustrations may not be copied. The abstract must contain conspicuous acknowledgement of IFEDC&IPPTC. Contact email: paper@ifedc.org or paper@ipptc.org.
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Abbreviations
- \( B \) :
-
Formation-volume factor
- C :
-
WBS coefficient, m3/Pa
- C t :
-
Total compressibility, Pa−1
- h :
-
Net-pay thickness, m
- K :
-
Permeability, m2
- K 0 :
-
Bessel function
- K 1 :
-
Bessel function
- m :
-
\( m = 2\int {\frac{p}{\mu Z}} {\text{d}}p \), MPa2/mPa s
- p i :
-
Initial pressure, Pa
- q j :
-
Rate, m3/s
- \( r_{\text{w}} \) :
-
Wellbore radius, m
- S :
-
Skin factor
- z:
-
Laplace variable
- \( C_{\text{D}} \) :
-
\( C_{\text{D}} = \frac{C}{{2\uppi\varphi hC_{\text{t}} r_{\text{w}}^{2} }} \)
- \( p_{\text{D}} \) :
-
\( p_{{j{\text{D}}}} = \frac{{2\,\uppi\,Kh\left( {p_{\text{i}} - p_{\text{wf}} } \right)}}{{q_{1} \mu B}} \)
- \( q_{{j{\text{D}}}} \) :
-
\( q_{{j{\text{D}}}} = \frac{{q_{j} }}{{q_{1} }} \)
- \( r_{\text{D}} \) :
-
\( r_{\text{D}} = \frac{r}{{r_{\text{w}} {\text{e}}^{ - S} }} \)
- \( t_{\text{D}} \) :
-
Dimensionless time, \( t_{\text{D}} = \frac{Kt}{{\varphi \mu C_{\text{t}} r_{\text{w}}^{2} }} \)
- \( t_{\text{p}} \) :
-
Production time, hour
- t pD :
-
Dimensionless production time
- ΔtD:
-
Dimensionless shut in time
- a:
-
\( \frac{{\lambda C_{\text{D}} }}{{\omega \left( {1 - \omega } \right)}} \)
- \( b \) :
-
\( \frac{{\lambda C_{\text{D}} }}{{\left( {1 - \omega } \right)}} \)
- \( D \) :
-
Diffusivity ratio for composite reservoir, \( D = {{\left( {{k \mathord{\left/ {\vphantom {k {\phi \mu c_{t} }}} \right. \kern-0pt} {\phi \mu c_{t} }}} \right)_{2} } \mathord{\left/ {\vphantom {{\left( {{k \mathord{\left/ {\vphantom {k {\phi \mu c_{t} }}} \right. \kern-0pt} {\phi \mu c_{t} }}} \right)_{2} } {\left( {{k \mathord{\left/ {\vphantom {k {\phi \mu c_{t} }}} \right. \kern-0pt} {\phi \mu c_{t} }}} \right)_{1} }}} \right. \kern-0pt} {\left( {{k \mathord{\left/ {\vphantom {k {\phi \mu c_{t} }}} \right. \kern-0pt} {\phi \mu c_{t} }}} \right)_{1} }} \)
- \( D \) :
-
Non-Darcy flow coefficient
- \( M \) :
-
Mobility ratio for composite reservoir, \( M = {{\left( {{k \mathord{\left/ {\vphantom {k \mu }} \right. \kern-0pt} \mu }} \right)_{2} } \mathord{\left/ {\vphantom {{\left( {{k \mathord{\left/ {\vphantom {k \mu }} \right. \kern-0pt} \mu }} \right)_{2} } {\left( {{k \mathord{\left/ {\vphantom {k \mu }} \right. \kern-0pt} \mu }} \right)_{1} }}} \right. \kern-0pt} {\left( {{k \mathord{\left/ {\vphantom {k \mu }} \right. \kern-0pt} \mu }} \right)_{1} }} \)
- \( N \) :
-
Number of wells
- \( r \) :
-
Distance from the well test wellbore, m
- \( R_{i} \) :
-
Outer radius of inner zone annulus in radial-composite model, m
- \( t \) :
-
Time, h
- \( \Delta t \) :
-
Shut in time, h
- \( \phi \) :
-
Porosity
- \( \lambda \) :
-
Interporosity flow coefficient
- \( \mu \) :
-
Viscosity, cp
- \( \omega \) :
-
Storativity ratio
- \( {\text{D}} \) :
-
Dimensionless variable
- \( {\text{f}} \) :
-
Fracture
- \( {\text{m}} \) :
-
Matrix
- \( {\text{j}} \) :
-
Index
- \( {\text{w}} \) :
-
Wellbore conditions
- \( {\text{wf}} \) :
-
Flowing wellbore conditions
- \( {\text{ws}} \) :
-
Shut in wellbore conditions
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Sun, H., Cui, Y., Wang, X., Zhang, J., Cao, W. (2019). Build-up Analysis of Multi-Well System in Naturally Fractured HTHP Gas Reservoirs. In: Qu, Z., Lin, J. (eds) Proceedings of the International Field Exploration and Development Conference 2017. Springer Series in Geomechanics and Geoengineering. Springer, Singapore. https://doi.org/10.1007/978-981-10-7560-5_166
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