Production System Modelling

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Chapter Overview

Vertical Lift Performance

Section 11.3 of 69 min3 code examples

Definition: The Vertical Lift Performance (VLP) describes the relationship between the bottom-hole flowing pressure (p_{wf}) and the production rate (q). It represents the pressure required to lift fluids from the bottom-hole to the surface against gravity, friction, and acceleration.

Oil Well VLP (Single Phase)

For a single-phase liquid, the pressure gradient (dp/dz) is the sum of hydrostatic (elevation), acceleration and frictional components.

Differential Equation:

dpdz=ρgsin(θ)+2fρv2D\frac{dp}{dz} = \rho g \sin(\theta) + \frac{2f \rho v^2}{D}

Where: - \rho = fluid density (lb/ft^3) - g = gravitational constant - f = Fanning friction factor - v = fluid velocity (ft/s) - D = tubing internal diameter (ft)

Numerical Example (ODEs with SepalSolver): We solve for p_{wf} by integrating from surface pressure (p_{surf}) to the total depth (H).

Example 1C#

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Code is ready to run
OutputFrom the book
Bottom-hole Flowing Pressure (Pwf) = 3849.29 psi
OilVLP.png

A comprehensive Vertical Lift Performance (VLP) model would account hydrostatic (elevation), frictional, and kinetic (acceleration) pressure gradient components.

For Multiphase flow, it would be necessary to consider the mixture density, two-phase friction factor, and no-slip density. The governing equation for multiphase flow is:

dPdz=ρmgsin(θ)144+2ftpρnsvm2gD+ρmvmgdvmdz\cfrac{dP}{dz} = \cfrac{\rho_m g \sin(\theta)}{144} + \cfrac{2 f_{tp} \rho_{ns} v_m^2}{g D} + \cfrac{\rho_m v_m}{g} \cfrac{dv_m}{dz}

\rho_m = mixture density, f_{tp} = two-phase friction factor, \rho_{ns} = no-slip density, v_m = mixture velocity, D = tubing internal diameter, g = gravitational constant.

Multiphase hydraulics are evaluated using the Beggs & Brill correlation, requiring fluid PVT properties including gas solubility (R_s), oil formation volume factor (B_o), and phase viscosities. Gas compressibility (Z) is evaluated using the Kareem et al. (2016) explicit correlation.

Example 2C#

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Code is ready to run
OutputFrom the book
Multiphase_VLP.png

Gas Well VLP

Gas VLP is more complex because gas density is highly dependent on pressure. As gas rises, it expands, increasing velocity and frictional losses.

Differential Equation:

dpdz=pMzRTgsin(θ)+2fρv2D\frac{dp}{dz} = \frac{p M}{z R T} g \sin(\theta) + \frac{2f \rho v^2}{D}

Numerical Example (ODEs with SepalSolver): In this example, the gradient function must recalculate gas density (\rho_g = \frac{p M}{Z R T}) at every step of the integration.

Example 3C#

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Code is ready to run
OutputFrom the book
Bottom-hole Flowing Pressure (Pwf) = 642.03 psi
GasVLP.png