Advanced Artificial Lift for Production Solutions and Optimization Engineers Presented by Jeff Kain
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Introduction to Nodal Analysis
Objectives •
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Understand the components of Inflow performance Understand the components of vertical lift performance Understand combining inflow and vertical lift performance Describe the Pressure versus depth relationship for different lift methods
IDEAL FLOW ASSUMPTIONS Ideal well Purely radial flow Infinite reservoir Uniform thickness Stabilized flow Single phase Above bubble point Homogeneous & isotropic reservoir Perforations penetrate throughout reservoir Reservoir shape Proximity of wellbore Wellbore clean / uncased No skin Darcy’s law
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NON IDEAL FLOW Departures from Darcy’s law Effects at boundaries Position of well Non homogeneous reservoir Perforation positions High velocities Fluid type / high GOR Transient behavior Relative permeability effects - oil/water/gas near the wellbore • Depletion if reservoir • Flow restrictions (skin)
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INFLOW PERFORMANCE SKIN
• Restricted flow into the wellbore
• The total skin factor may be calculated from well test data
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• Ideal flow conditions rarely exist
INFLOW PERFORMANCE PRINCIPLE ORIGINS OF SKIN Schlumberger Private
The relationship between well inflow rate and pressure drawdown can be expressed in the form of a Productivity Index, denoted ‘PI’ or ‘J’, where:
WELL & RESERVOIR INFLOW PERFORMANCE ( Successful design depends upon prediction of flow rate)
FACTORS AFFECTING PI
•Bubble point pressure •Dew point pressure
2. Relative permeability behaviour •Ratio of effective permeability to a particular fluid (oil, gas or water) to the absolute permeability of the rock
3. Oil viscosity •Viscosity decreases with pressure decrease to Pb •Viscosity increases as gas comes out of solution
4. Oil formation volume factor (bo) •As pressure is decreased the liquid will expand •As gas comes out of solution oil will shrink
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1. Phase behaviour
WELL & RESERVOIR INFLOW PERFORMANCE ( Successful design depends upon prediction of flow rate)
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AS RATE INCREASES IS NO LONGER STRAIGHT LINE • Increased gas sat. Near wellbore - rel. Perm. Effects • Laminar > turbulent flow • Exceeds critical flow of sandface
WELL & RESERVOIR INFLOW PERFORMANCE ( Successful design depends upon prediction of flow rate)
• Vogel • Back pressure/Fetkovich • Lit (Jones, Blount and Glaze) • Normalized pseudo pressure
WELL & RESERVOIR INFLOW PERFORMANCE ( Successful design depends upon prediction of flow rate)
VOGEL
Q/Qmax = 1 - 0.2(Pwf/Pws) - 0.8(Pwf/Pws)2 where:
Q = the liquid production rate, stb/d Qmax = the maximum liquid rate for 100% drawdown Pwf = bottom hole flowing pressure, psi Pws = the reservoir pressure, psi
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Dimensionless reference curve based on the following equation:
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WELL & RESERVOIR INFLOW PERFORMANCE ( Successful design depends upon prediction of flow rate)
SUMMARY OF FACTORS AFFECTING PREDICTION OF WELL PRODUCTION
• Nature of drive mechanisms • Physical nature of reservoir (non homogeneous) • Availability of stabilized flow • Changes over time & drawdown • Increased gas solution near wellbore • Stabilised flow near wellbore • Flow regime near wellbore • Critical flow at wellbore
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• Presence of three phase flow
MULTIPHASE FLOW OUTFLOW PERFORMANCE MOVEMENT OF A MIXTURE OF FREE GASES AND LIQUIDS
VLP is a function of physical properties not inflow • Tubing ID • Wall roughness • Inclination • Liquid / gas density • Liquid / gas viscosity • Liquid / gas velocity • Well depth / line lengths • Surface pressure • Water cut • GOR • Liquid surface tension • Flowrate
PRESSURE LOSS IN WELLBORE Schlumberger Private
‘Complicated expression’
Z
δP/δZ Schlumberger Private
• System described by a energy balance expression • Mass energy per unit mass in = energy out • (+ - exchange with surroundings) • For wellbore- pressure Calc. for length of pipe • Integrated each section • Pressure can be divided into three terms
PRESSURE LOSS IN WELLBORE GRAVITY TERM
FRICTION TERM
2
ACCELERATION TERM
δP/δZtotal = g/gcρcosθ + fρv /2gcd + ρv/gc[δP/δZ]
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TOTAL PRESSURE DIFFERENCE
GRAVITY TERM
g/gcρcosθ Correcting weight of fluid Dominant term Single phase simple Multiphase complex
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Pressure loss due to gravity Schlumberger Private
• Based on fluid densities at element for conditions Pelement, Telement • Phase volumes = % of pipe occupied by fluid * density of fluid • Assumes liquid and gas phases at same velocity • This is the no slip case that will produce minimum delta P due to gravity
SLIP Schlumberger Private
• The gas phase moves at a faster velocity than the liquid phase due to buoyancy forces • Consequence is a change in the areas of each phase in an element • The slip corrected liquid area is termed LIQUID HOLDUP • Correction from phase volumes to holdup volumes through multi-phase correlations • Complex determination characterised in flow regime maps
Liquid Holdup • Consider an element for Pelement , Telement
% Liquid
LIQUID Liquid Holdup
GAS
Mixture density = L density * % L + G density * %G
% Gas
GAS 1 - Liquid Holdup
Slip corrected Mixture density = L density * HL + G density * (1(1-HL)
fρv /2gcd Increases with rate Proportional to velocity Proportional to relative roughness Laminar vs turbulent flow Effective viscosity Effective mixture density Sensitive to gas volumes
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ACCELERATION TERM
ρv/gc[δP/δZ] Expansion of fluid as pressure decreases Smallest term Often ignored Need to account in high rate
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Proportion of terms in oil well close to sandface (no significant GLR)
GRAVITY FRICTION
Proportion of terms in oil well significant GLR close to surface
GRAVITY FRICTION ACCELERATION
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ACCELERATION
PRESSURE LOSS IN WELLBORE Schlumberger Private
• Fluid density in every term • Errors would be cumulative • PVT important
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