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The word  "Inflow" is misnomer as Inflow Performance Relation Relationship (IPR) analysis is applicable for both producers and injectors.

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The Inflow Performance Relation Relationship (IPR) analysis is closely related to well Productivity Index (PI)  

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bodyJ_s
 which is defined as below:

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For undersaturated reservoir the numerically-simulated Inflow Performance Relation Relationship (IPR)s have been approximated by analytical models and some of them are brought below. 

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These correaltions should be calibrated to the available well test data to set a up a customised IPR model for a given formation.


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Fig1
Fig1

Water and Dead Oil IPR

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For a single layer formation with low-compressibility fluid (water or dead oil) the PI does not depend on drawdown (or flowrate) 

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bodyJ_s = \rm const
 and IPR plot is reperented by a straight line (Fig. 1)

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where 

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bodyq_{max} = J_s \, p_R
  is the maximum reservoir deliverability when the bottom-hole is at atmospheric pressure and also called Absolute Open Flow (AOF).


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Fig2
Fig2

Dry Gas IPR

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For gas producers, the fluid compressibility is high and formation flow is essentially non-linear, inflicting the downward trend on the whole IPR plot (Fig. 2).

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But obviously more tests will make assessment more accruate.


Saturated Oil IPR

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For saturated oil reservoir the free gas flow inflict the downward trend of IPR plot  similar to dry gas (Fig. 3).

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Vogel IPR @ model
Vogel IPR @ model
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Undersaturated Oil IPR

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For undersaturated oil reservoir 

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bodyp_r > p_b
 the behavior of IPR model will vary on whether the bottom-hole pressure is above or below bubble point.

When it is higher than bubble point 

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bodyp_{wf} > p_b
 then formation flow will be single-phase oil and production will follow the constant Inflow Performance Relation Relationship (IPR)

When bottom-hole pressure goes below bubble point 

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bodyp_{wf} < p_b
  the near-reservoir zone free gas slippage also inflicts the downward trend at the right side of IPR plot (Fig. 3).

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q_{max} = q_b \, \Big[1 + \frac{1}{1.8} \frac{p_b}{(p_r - p_b)}  \Big]




Saturated Multiphase IPR

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For saturated 3-phase water-oil-gas reservoir the IPR analysis is represented by oil and water components separately (see Fig. 4.1 and Fig. 4.2).

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\frac{q_w}{q_{w, \, max}} = 1 - 0.72 \, \frac{p_{wf}}{p_r} - 0.28 \Bigg(\frac{p_{wf}}{p_r} \Bigg)^2 

Undersaturated Multiphase IPR

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For undersaturated 3-phase water-oil-gas reservoir the IPR analysis is represented by oil and water components separately (see Fig. 4.1 and Fig. 4.2).

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The analytical correlation for saturated 3-phase oil flow is given by Wiggins model:

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\frac{q_o}{q_{o, \, max}} = 1 - 0.52 \, \frac{p_{wf}}{p_r} - 0.48 \Bigg(\frac{p_{wf}}{p_r} \Bigg)^2  


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\frac{q_w}{q_{w, \, max}} = 1 - 0.72 \, \frac{p_{wf}}{p_r} - 0.28 \Bigg(\frac{p_{wf}}{p_r} \Bigg)^2 


See Also

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

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Vogel IPR @model ] [ Richardson and Shaw IPR @ model ] Wiggins IPR @ model ]


Reference

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Gilbert
Gilbert
Gilbert, W.E.: "Flowing and Gas-Lift Well Performance," Drill. and Prod. Prac., API (1954) 126.

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