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Сomparative analysis between:


and


It is based on correlation between surface flowrate 

LaTeX Math Inline
bodyq
and bottomhole pressure 
LaTeX Math Inline
bodyp_{wf}
as a function of tubing-head pressure 
LaTeX Math Inline
bodyp_s
and formation

Definition

WFP – Well Performance Analysis  is a specialized analysis of correlation between surface flowrate and wellbore pressure as function of formation pressure and associated production optimization procedures.

Application

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Technology

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WFP is performed on stabilised flow and does not cover transient behavior which is normally covered in Well Testing domain.

The flow is called stabilised if the well productivity index is not changing over time.

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On the other hand, the constant rate flow may not represent a stabilised flow as the bottom-hole pressure and productivity index maybe still in transition after the last rate change.

The WFP methods are not applicable if the well flow is not stabilised even if the flow rate is maintained constant. 

There are two special reservoir flow regimes which are both stabilised and maintain constant flow rate:  steady state regime (SS) and pseudo-steady state regime (PSS).

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The pseudo-steady state (PSS) regime is reached when the flow is stabilised  with no pressure support at the external boundary.

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As for formation and bottom-hole pressure in PSS they will be synchronously varying while in SS they will be staying constant.

The table below is summarizing the major differences between SS and PSS regimes.

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LaTeX Math Inline
bodyJ(t) = \frac{q}{\Delta p}

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constant

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constant

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LaTeX Math Inline
bodyq(t)

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constant

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constant

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Drawdown

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LaTeX Math Inline
body\Delta p(t) = p_e(t) - p_{wf}(t)

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constant

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constant

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LaTeX Math Inline
bodyp_{wf}(t)

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constant

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varying

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pressure

LaTeX Math Inline
bodyp_

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constant

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varying

r
 and current reservoir saturation.


Application

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Technology

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Most reservoir engineers exploit material balance thinking which is based on long-term well-by-well surface flowrate targets  (whether producers or injectors).

In practice, the flowrate targets are closely related to bottomhole pressure and associated limitations and require a specialised analysis to set up the optimal lifting (completion, pump, chocke) parameters. 

This is primary domain of WFP analysis.


WFP is performed on stabilised wellbore and reservoir flow and does not cover transient behaviour which is one of the primary subjects of Well Testing domain.

It's again important to avoid confusion between the termines stationary conditions (which mean that refered properties are not chaning in time) and stabilised flow conditions which may admit pressure and rate vraition.

In practice, the productivity index is usually not known at all times as there is not routine procedure to assess it.

It is usually accepted that a given formation takes the same time to stabilise the flow after any change in well flow conditions and the stabilisation time is assessed based on the well tests analysis.

Although, this is not strictly true and the flow stabilisation time depends on well-formation contact and reservoir property variation around a given well.

This is also compromised in multi-layer formations with cross-layer communication. 


The conventional WFP – Well Performance Analysis is perfomed as the cross-lot with two physical models:

and

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IPR – Inflow Performance Relationship

the 

IPR – Inflow Performance Relation represnts the relation between the bottom-hole pressure 
LaTeX Math Inline
bodyp_{wf}
  and surface flow rate  
LaTeX Math Inline
bodyq
  during the stabilised flow:

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anchor1
alignmentleft

\{ p_{wf}

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  which will be non-linear in generic case. 

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The IPR analysis is closely related to well productivity index  

LaTeX Math Inline
bodyJ_s(q)
 which is defined as below:

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LaTeX Math Block
anchorJ
alignmentleft
J_s(q_{\rm liq}) = \frac{q_{\rm liq}}{p_R-p_{wf}}

for oil producer with surface liquid production

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bodyq_{liq} = q_o + q_w
(water and oil)

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LaTeX Math Block
anchorJ
alignmentleft
J_s(q_g) = \frac{q_g}{p_R-p_{wf}}

\ {\rm vs} \ q \}
cross-plot with two model curves:

Anchor
JP
JP

The intersection of IPR and Lift Curves represent the Stabilised wellbore flow (see Fig. 1)


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Fig. 1. A sample case of stabilised wellbore flow represented by junction point of IPR and Lift Curves.Fig. 2. The dead well scenario.


Given a tubing head pressure 

LaTeX Math Inline
bodyp_s
the WFP Junction Point will be dynamic in time depending on current formation pressure (see Fig. 2) and formation saturation (see Fig. 3). 


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Fig. 3. A sample case of stabilised wellbore flow as function of formation pressure.

Fig. 4. A sample case of stabilised wellbore flow as function of production watercut



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Fig. 5. A bunch of IPRs at different formation pressures and Lift Curves at different THPs.


Workflow

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  1. Check the current production rate against the production target from FDP

  2. If the diffference is big enough to justify the cost of production optimization (see point 8 below) then proceed to the step 3 below

  3. Assess formation pressure based on well tests

  4. Simulate IPR / LC based on the current WOR/GOR

  5. Calculate the stabilized flow bottom-hole pressure

  6. Gather the current bottom-hole pressure
    LaTeX Math Inline
    bodyp_{wf}


  7. Check up the calculation aganst the actual 
    LaTeX Math Inline
    bodyp_{wf}


  8. Recommend the production optimisation activities to adjust bottom-hole pressure 
    LaTeX Math Inline
    bodyp_{wf}
    :

    • adjusting the choke at surface

    • adjusting the pump settings from surface 

    • changing the pump depth

    • changing the tubing size

    • changing the pump

The above workflow is very simplistic and assumes single-layer formation with no cross-flow complications.

In practise, the WFP analysis is often very tentative and production technologists spend some time experimenting with well regimes on well-by-well basis. 


See Also

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Petroleum Industry / Upstream / Production / Subsurface Production / Well & Reservoir Management

Subsurface E&P Disciplines / Production Technology 

WFP – Water Injector ]

Inflow Performance Relation (IPR) ] [ Lift Curves (LC) ]


  

Anchor
WFP
WFP

References

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Joe Dunn Clegg, Petroleum Engineering Handbook, Vol. IV – Production Operations Engineering, SPE, 2007


Michael Golan, Curtis H. Whitson, Well Performance, Tapir Edition, 1996


William Lyons, Working Guide to Petroleum and Natural Gas production Engineering, Elsevier Inc., First Edition, 2010


Shlumberge, Well Performance Manual

for gas producer

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LaTeX Math Block
anchorJ
alignmentleft
J_s(q_g) = \frac{q_g}{p_{wf}-p_R}

for gas injector

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LaTeX Math Block
anchorJ
alignmentleft
J_s(q_w) = \frac{q_w}{p_R-p_{wf}}

for water injector

where

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LaTeX Math Inline
body q_w, \, q_o, \, q_g

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LaTeX Math Inline
bodyp_R

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field-average formation pressure withing the drainage area of a given well

Based on these notions the general WFP – Well Flow Performance can be wirtten in univseral form:

LaTeX Math Block
anchorIPR
alignmentleft
p_{wf} = p_R - \frac{q}{J_s(q)}

providing that  

LaTeX Math Inline
bodyq
 has a specific meaning and sign as per the table below:

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LaTeX Math Inline
body-

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LaTeX Math Inline
body+

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LaTeX Math Inline
bodyq=q_{\rm liq}=q_o+q_w

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LaTeX Math Inline
bodyq=q_g

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LaTeX Math Inline
bodyq=q_w

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LaTeX Math Inline
bodyp_R
– field-average pressure within the drainage area
LaTeX Math Inline
bodyA_e

LaTeX Math Inline
bodyp_e
– pressure value at boudary of the drainage area
LaTeX Math Inline
bodyA_e

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LaTeX Math Inline
bodyq_{\rm liq}=q_o+q_w
– surface liquid rate

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LaTeX Math Inline
bodyq_t = B_w \, q_W + \frac{B_o - R_s B_g}{1 - R_v R_s} \, q_O + \frac{B_g - R_v B_o}{1 - R_v R_s} \, q_G
– total flowrate at sandface

Для однопластовой залежи со слабосжимаемым флюидом продуктивность не зависит от дебита  

LaTeX Math Inline
bodyJ_s = \rm const
 и график ИКС представляет собой прямую линию (Рис. 1).

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Это характерно для водозаборных скважин, водонагнетательных скважин и нефтяных скважин выше давления насыщения.

Для газовых скважин, газоконденсатных скважин, скважин с легкой нефтью, а также нефтяных скважин, где давление опустилось ниже давления насыщения

LaTeX Math Inline
bodyP_{wf} < P_b
, сжимаемость фильрующегося агента являестя высокой, закон фильтрации в прибойной зоне скважины становится нелинейным и кривая ИКС начинает отклоняется вниз от прямой линии (Рис. 2), что означает ухудшение продуктивности скважины с ростом скорости фильтрации в призабойной зоне.

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Fig.2. IPR for compressible fluid production (gas, light oil, saturated oil)

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VLP – Vertical Lift Performance

КВЛ активно используется для анализа оптимального режима работы скважины.

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Sample Case 1 –  Oil Producer Analysis

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Sample Case 2 – Water Injector Analysis

Sample Case 3 – Gas Producer Analysis

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