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Consider a water injector with main pay in Reservoir Layer #1 and spontaneous fracture extending down to Reservoir Layer #2 (see Fig. 1).

Assume that fracture is not fixed and requires surplus pressure 

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body\Delta p_f
 to get opened against the rock burden. 

When injection bottomhole pressure 

LaTeX Math Inline
body--uriencoded-- p_%7Bwf%7D
 is below fracture opening value 
LaTeX Math Inline
body--uriencoded-- p_%7Bwf%7D < \Delta p_f
 then water is going to the main pay only (Reservoir Layer #1) and flow radially around the well.

When injection bottomhole pressure 

LaTeX Math Inline
body--uriencoded-- p_%7Bwf%7D
 is above fracture opening value 
LaTeX Math Inline
body--uriencoded-- p_%7Bwf%7D > \Delta p_f
 then water is going to the fracture and then gets distributed between Reservoir Layer #1 and Reservoir Layer 2


Fig. 1. Dual-layer well schematic




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q = q_1 + q_2




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p_{wf} = p_e + q/J



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J = J_1 + J_2



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p_e = \Delta p_f + \frac{J_1 \cdot p_1 + J_2 \cdot (p_2- \delta p_2)}{J_1 + J_2}



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anchorpe
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p_e = \frac{J_1 \cdot p_1 + J_2 \cdot p_c}{J_1 + J_2}



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anchorpc
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p_c = \left(1 + \frac{J_1}{J_2} \right) \Delta p_f + p_2 - \delta p_2


where

Well

LaTeX Math Inline
bodyq

total subsurface flowrate of the well

LaTeX Math Inline
bodyJ

total well productivity Index

LaTeX Math Inline
bodyp_e

apparent formation pressure of dual-layer formation

LaTeX Math Inline
bodyh

true vertical height between the layers tops

LaTeX Math Inline
body\rho

wellbore fuid density

LaTeX Math Inline
bodyg

gravity constant

LaTeX Math Inline
body\Delta p_f

fracture opening pressure
Layer #1

LaTeX Math Inline
body--uriencoded--p_%7Bwf%7D

bottom-hole pr4essure at Layer #1 top

LaTeX Math Inline
bodyq_1

total subsurface flowrate of the Layer #1

LaTeX Math Inline
bodyp_1

formation pressure of the Layer #1

LaTeX Math Inline
bodyJ_1

productivity Index of the Layer #1
Layer #2

LaTeX Math Inline
body--uriencoded--p_%7Bwf2%7D = p_%7Bwf%7D + \rho \, g\, h

bottom-hole pr4essure at Layer #2 top

LaTeX Math Inline
bodyq_2

total subsurface flowrate of the Layer #2

LaTeX Math Inline
bodyp_2

formation pressure of the Layer #2

LaTeX Math Inline
bodyJ_2

productivity Index of the Layer #2


Expand
titleDerivation


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p_{wf, 1} = p_{wf} = \Delta p_f + p_1  + q_1/J_1


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p_{wf,2} = p_{wf} + \delta p_2 = \Delta p_f + p_2 + q_2/J_2


This leads to

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q_1 = J_1 \cdot (p_{wf} - p_1 - \Delta p_f)


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q_2 = J_2 \cdot (p_{wf,2} - p_2 - \Delta p_f) = J_2 \cdot (p_{wf} - (p_2 + \Delta p_f-\delta p_2) )

and

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q = q_1 + q_2 = q_1 = J_1 \cdot (p_{wf} - (p_1 + \Delta p_f))+ J_2 \cdot (p_{wf} - (p_2-\delta p_2  + \Delta p_f) )


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q =  (J_1+J_2)\cdot  p_{wf} - J_1 \cdot (p_1 + \Delta p_f) + J_2 \cdot ((p_2-\delta p_2 + \Delta p_f) )

or

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q =  J \cdot (p_{wf}-p_e), \ {\rm where} \ J = J_1 + J_2 \ {\rm and} \ p_e = J^{-1} \cdot (J_1 \cdot (p_1 + \Delta p_f) + J_2 \cdot (p_2-\delta p_2 + \Delta p_f))

or

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p_e = \Delta p_f +  J^{-1} \cdot (J_1 \cdot p_1  + J_2 \cdot (p_2-\delta p_2))




See Also


Petroleum Industry / Upstream /  Production / Subsurface Production / Subsurface E&P Disciplines / Field Study & Modelling / Production Analysis / Productivity Diagnostics

Production Technology / Well Flow Performance ]

Formation pressure (Pe) ] Multi-layer IPR ]