SPE Production & Operations
Volume 21, Number 1, February 2006, pp. 89-97

SPE-89754-PA

Simplified Wellbore-Flow Modeling in Gas/Condensate Systems

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DOI  More information 10.2118/89754-PA http://dx.doi.org/10.2118/89754-PA

Citation

  • Kabir, C.S. and Hasan, A.R. 2006. Simplified Wellbore-Flow Modeling in Gas/Condensate Systems. SPE Prod & Oper21 (1): 89-97. SPE-89754-PA.

Summary

Predicting long-term reservoir performance with realistic wellbore models is fraught with uncertainty owing to the complexity of two-phase flow. That is because even a calibrated two-phase-flow model departs from its expected performance trend when changes in flow conditions occur. These inevitable changes include gas/liquid ratio, wellhead pressure, and flowline pressure with time, among others. Influx of water further exacerbates the prediction problem.

This study explores the possibility of using simplified approaches to compute bottomhole pressure (BHP) from wellhead pressure (WHP), measured rates, gravity of producing fluids, and tubular dimensions. BHP computations on three independent data sets comprising 167 gas/condensate-well tests suggest that the no-slip homogeneous model applies quite well. Statistical results show the homogeneous model compares quite favorably with mechanistic two-phase-flow models. However, the main advantage of the simplified model is that its recalibration with field data is not required because the gas/oil ratio increases with time, thereby making the model increasingly reliable.

Most field data sets suggest random error in BHP calculations; uncertainty in rate measurements appears to be the most probable cause. High-gas-liquid-ratio (GLR) systems can tolerate large errors in rate measurements, but low-GLR wells demand greater accuracy because of increasing importance of the hydrostatic head.

Introduction

Two-phase-flow modeling for gas/condensate wells has not received as much attention as that for oil wells. Recent SPE books (Brill and Mukherjee 1999; Hasan and Kabir 2002) on this topic make very little mention of this flow condition, presumably because modeling is supposed to conform to that offered for oil wells. This study probes this premise, among other issues.

The popular Gray correlation (User’s Manual for API 14B 1978) appears to do a good job in most gas/condensate wells. However, applicability of this correlation outside the bounds of its specified parameters remains unclear. Take the upper limits of condensate/gas ratio (CGR) of 50 STB/MMscf, or flow-string diameters of 3.5 in., for instance. Questions arise whether one should use a different model when one of these criteria, as set by Gray, is not met.

Boundaries of applicability often get violated beyond a correlation’s original intent; Gray’s correlation is no exception in this regard. Practicality demands that a user specifies one computational approach for flow in pipes when long-term integrated reservoir/wellbore/flowline performance is sought over a field’s producing life. Declining CGR and increasing water production with time have the potential to complicate any modeling effort. What also remains unclear is how to treat the multicomponent fluid mixture entering the wellbore/flowline system after undergoing compositional calculations in the reservoir.

Besides the two-component gas/liquid Gray correlation (User’s Manual for API 14B 1978) other approaches have emerged for modeling gas/condensate flow. The semimechanistic model of Govier and Fogarasi (1975) represents the multicomponent approach with flash calculations. In contrast, the wet-gas concept offered by Peffer et al. (1988) suggests extreme pseudoization with single-component gas. Nonetheless, the simplified approach of Peffer et al. with good accuracy is appealing. A minor drawback of both methods is exclusion of the accelerational term, which may be significant in wells producing fluids at high GLR.

This paper advocates the use of a two-component homogeneous model to circumvent issues with any rigorous two-phase-flow modeling, such as delineating flow-pattern boundaries, estimating slip between phases, and doing flash calculations. We show that Gray’s correlation is essentially a homogeneous model, and the model of Ansari et al. (1994) also simplifies to a homogeneous model when mist flow is assumed in gas/condensate wells. The steady-state version of the transient simulator OLGA (Bendiksen et al. 1991) also lends support to the notion of homogeneous modeling.

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History

  • Original manuscript received: 4 June 2004
  • Revised manuscript received: 13 June 2005
  • Manuscript approved: 15 June 2005
  • Version of record: 20 February 2006