Lesson 4 Air, Gas, Mist Drilling

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    PETE 689Underbalanced Drilling (UBD)

    Harold Vance Department of Petroleum Engineering

    Read: UDM - Chapter 2.1 - 2.4

    Lesson 4Air, Gas and Mist Drilling.

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    Air, Gas, and Mist DrillingGases used in UBD.

    Dry air drilling. Nitrogen drilling.

    Natural gas drilling.

    Mist drilling.

    Optimized hole cleaning.

    Harold Vance Department of Petroleum Engineering

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    Gases for UB Drilling

    Air.

    Cryogenic Nitrogen.Membrane Nitrogen.

    Engine Exhaust.Natural gas.

    Harold Vance Department of Petroleum Engineering

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    Gases for UB Drilling

    79% N2, 21% O

    2.

    Corrosion.

    Fire.

    US$3,000 Day.

    Mod and Demob.

    Harold Vance Department of Petroleum Engineering

    Compressed Air

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    Cryogenic Nitrogen40 year old technology.

    Made as a by product of liquid

    oxygen manufacture.

    Air replacement.

    No corrosion.

    No downhole fires.

    99.9% pure N27K-40K US$/day.

    Harold Vance Department of Petroleum Engineering

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    Delivery

    Bottled gas.

    Truck.

    Storage tank ona ship.

    Harold Vance Department of Petroleum Engineering

    Cryogenic Nitrogen

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    Stainless Steel

    Liquid Nitrogen

    (-320O

    F)

    Carbon Steel

    Gaseous Nitrogento well

    80OF, 0-10,000 psi

    Pump

    Vaporizer

    Cryogen Nitrogen-PumpingEquipment

    Harold Vance Department of Petroleum Engineering

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    ProcedureDetermine Gas Volume Required.

    Convert from Liquid Volume.

    1 gallon liquid nitrogen produces93.12 ft3 of N2

    at SCP.

    1 m3 of N2

    liquid produces 698 m3

    of gas at SCP.

    Harold Vance Department of Petroleum Engineering

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    Nitrogen

    Conversion Factors

    1 gal of liquid nitrogen is

    93.12 ft3 at STC.

    1 gal of liquid nitrogen is0.1333 ft3.

    1 liter of liquid nitrogen is698 litres of gas at STC.

    Harold Vance Department of Petroleum Engineering

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    Cryogenic Nitrogen CostWorld-wide

    1-3 US $/gal. 0.10 US $/scf.

    Canada

    0.02 US $/scf.South America

    1.00 US $/m3.Harold Vance Department of Petroleum Engineering

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    UB Drilling Gas AlternativesNitrogen Membranes

    95% N2, 3-5% O2.

    Corrosion considerations.

    Combustion considerations.

    Approximately 15,000 US $/day.Mob/demob costs.

    Harold Vance Department of Petroleum Engineering

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    Membrane NitrogenOn site manufacture.

    Dependent on concentration.

    Directly proportional topressure and rate.

    Inversely proportional to gaspartial pressure.

    Driven by dissolution anddiffusion.

    Harold Vance Department of Petroleum Engineering

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    Individual Hollow

    Polmeric Gas Separation Fiber

    Harold Vance Department of Petroleum Engineering

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    Individual Hollow

    Polmeric Gas Separation Fiber

    Harold Vance Department of Petroleum Engineering

    Oxygen and Water Vapor are Fast Gaseswhich quickly permeate the membrane,allowing Nitrogen to flow through thefiber bores as the product stream.

    Nitrogen

    Oxygen

    Water VaporNitrogen

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    HOLLOW FIBERMEMBRANE

    FEED AIR

    OXYGEN- ENRICHED AIR

    NITROGEN

    ENRICHEDGAS

    N2 Generating

    Unit A Bundle Of Fibers

    Harold Vance Department of Petroleum Engineering

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    Equipment RequiredCompressor.

    Filters-fibers will plug ifthe air is not filtered.

    NPU or NGU.

    Controller.Booster(s).

    Harold Vance Department of Petroleum Engineering

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    Drilling

    Rig

    Optional BoosterCompressor

    Filter andAir Separation

    Membrane System

    Feed Air

    Compressor

    Membrane

    Nitrogen Production Unit

    Harold Vance Department of Petroleum Engineering

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    1997 Nitrogen Unit.

    N2 units with

    coolers.8x30x8 high

    23,000 psi

    1200 scfm N2 at5% 02

    Harold Vance Department of Petroleum Engineering

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    Skid-Mounted Nitrogen

    Producing Unit (NPU)1998

    Harold Vance Department of Petroleum Engineering

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    Weatherford 2000

    Nitrogen Generation Unit.

    1. N2 500-600 scfm.

    2. 2000 psi comp.

    3. 27 gph diesel.

    4. 8x20x16 high.

    Nominal O2 5%

    1.

    2.3.

    4.

    Harold Vance Department of Petroleum Engineering

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    Nitrogen Membrane System

    1999

    1

    2 35

    Harold Vance Department of Petroleum Engineering

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    ProcedureDetermine volume requirement.

    Determine maximum oxygenconcentration.

    Determine effective volume fromunits.

    Determine pressure requirement.

    Harold Vance Department of Petroleum Engineering

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    Oxygen Concentration

    % Oxygen is only partially a

    valid concept for fire. Ignition temperatures and

    water content play a big part.

    % Oxygen is important forcorrosion.

    Harold Vance Department of Petroleum Engineering

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    Recent Combustion Work

    Testing:

    Alberta Research Council.

    Counter claims of increasedcorrosion and combustion with

    membrane generated N2

    Harold Vance Department of Petroleum Engineering

    Mi i

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    MinimumOxygen for Combustion

    (with Methane)

    Harold Vance Department of Petroleum Engineering

    %OxygenR

    equiredforCom

    bustion

    Pressure (psia)

    12.00

    11.50

    11.00

    10.50

    10.00

    9.50

    9.00

    8.50

    8.00

    0 500 1000 1500 2000 2500 3000

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    Nitrogen Source SelectionCryogenic vs. Membrane

    Location.

    Job duration.

    Volume requirement.

    Pressure requirement.Purity requirement.

    Harold Vance Department of Petroleum Engineering

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    Operating Cost

    Canada

    USA Crossover between cryogenic costs

    and membrane costs is generallyabout three days of operation.

    Transportation and mobilization arebig items.

    Harold Vance Department of Petroleum Engineering

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    Cryogenic

    Nitrogen Operating Cost

    Canada

    10,000 US $/day minimum. 40,000 US $/day maximum.

    (500-1800 scfm for 20 hrs/day).

    Harold Vance Department of Petroleum Engineering

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    Harold Vance Department of Petroleum Engineering

    Flow Path

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    Exhaust Gas

    Generating Unit 1980

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    ExhaustGas System

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    Natural Gas for UB Drilling

    Available.

    No downhole fires.

    No corrosion.

    Low cost, long termcontracts.

    Harold Vance Department of Petroleum Engineering

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    Pressure

    Determine requirement

    as for air, but allow forlesser specific gravity.

    Delivery pressure set atsource.

    Harold Vance Department of Petroleum Engineering

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    Fuel Gas & Group Gas Pipeline

    Harold Vance Department of Petroleum Engineering

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    Natural Gas Pipeline Hook Up(Lyons, 1984)

    ~500Psig

    Pipeline

    Flow

    Choke/Controller

    Flow to rig.

    Auxiliary line

    to rig.

    Main Pipeline.

    Harold Vance Department of Petroleum Engineering

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    Natural Gas Concerns

    May be pressure limited.

    Heavier hydrocarbonsrepress foam so be surethat they are stripped out.

    Harold Vance Department of Petroleum Engineering

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    Amoco Crossfield

    Gas Recovery Project

    Harold Vance Department of Petroleum Engineering

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    177.8 mm Casing @ 2403 m

    155.6 mm Openhole

    778 m

    2350m

    Target TMD = 3181 m

    88.9 mm Drill Pipe

    KOP = 2250 m

    120.6mm PDM

    Elkton: GasBHP = 7.0 MPaBHT = 80oC

    Drilling FluidWater = 1000 kg/m3

    Viscosity = 1cP

    Amoco Crossfield 9-12 Well

    Harold Vance Department of Petroleum Engineering

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    Crossfield

    Gas Recovery ProjectWhy it was done:

    Increasing public concernsover flaring.

    Increasing EUB requirements

    for public consultation andnotification.

    Harold Vance Department of Petroleum Engineering

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    Perfect fit with Amocos goal of

    reducing greenhouse gasemissions.

    Try out new idea and technology.Great plumbing setup.

    Crossfield

    Gas Recovery Project

    Harold Vance Department of Petroleum Engineering

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    Gas Recovery Project

    Gas Flare System

    Horizontal Separator

    Choke Manifold

    RBOPTM

    Produced GasCompressors

    Feed Gas Line

    Gas Gathering Line

    Drilling Rig

    Feed Gas Compressors

    Gas Processing Unit

    Flare KnockoutVessel

    Harold Vance Department of Petroleum Engineering

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    Compression

    & Scrubber/Filter Units

    Recovery Gas CompressorsScrubber/Filter Unit

    Feed Gas Compressors

    Harold Vance Department of Petroleum Engineering

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    Flow Control Manifold

    Harold Vance Department of Petroleum Engineering

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    Gas Scrubber & Filter Unit

    Harold Vance Department of Petroleum Engineering

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    Gas Recovery Summary

    Harold Vance Department of Petroleum Engineering

    0

    2

    4

    6

    8

    10

    12

    14

    16

    MMCFD

    Gas Conserved Gas Flared

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    Gas Recovery SummaryConserved 92%.

    Inc. Cost 170k US $.

    No need to optimizeGLRs.

    75 MMCFD well.

    Harold Vance Department of Petroleum Engineering

    0

    2

    4

    6

    8

    10

    12

    14

    16

    Gas Conserved Gas Flared

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    Crossfield

    Gas Recovery ProjectResults

    Estimated costs were 250kUS $,actual cost was 170kUS $.

    Conserved 92% of flow from thewell.

    Eliminated need to optimize thegas/liquid ratios.

    75 MMCFD storage well.

    Harold Vance Department of Petroleum Engineering

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    Hole CleaningOptimizing hydraulics with gasses is

    primarily concerned with holecleaning - getting the cuttings that

    are generated by the bit out of thehole.

    With gas, rheological properties have

    very little to do with hole cleaning.Hole cleaning with gasses is almost

    entirely dependent on the annularvelocity.

    Harold Vance Department of Petroleum Engineering

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    Drag and Gravitational ForcesFlowing air exerts a drag force on

    cuttings.

    Gravitational force on the cuttings

    Therefore there is a thresholdvelocity in which the cuttings will

    be lifted from the wellbore.

    Threshold velocity increases withsize of cuttings.

    Harold Vance Department of Petroleum Engineering

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    Hole CleaningCompressibility of air (or gas)

    complicates matters.

    Frictional pressure increasesdownhole pressure - decreasesvelocity downhole.

    Suspended cuttings increase thedensity of the air, increasingdownhole pressure.

    Harold Vance Department of Petroleum Engineering

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    Hole Cleaning

    Harold Vance Department of Petroleum Engineering

    Temperature has an effect on

    volumetric flow rate.

    We must pump at a velocity

    high enough to remove the

    cuttings, but not too highwhere we waste energy.

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    Hole Cleaning Criteria

    Terminal Velocity Criteria.

    Minimum Energy Criteria.

    Minimum BHP Criteria.

    Harold Vance Department of Petroleum Engineering

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    Terminal Velocity CriteriaGray determined that the

    minimum velocity of the gas

    must be at least as high as theterminal velocity of the cuttingin order to lift the cutting from

    the wellbore.

    Vc = Vf- Vt

    Harold Vance Department of Petroleum Engineering

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    g gravitational acceleration, 32.17 ft/sec2

    dc characteristic particle diameter, ft.

    Cd drag coefficient.

    c density of cuttings, lbm / ft3

    f density of fluid, lbm/ ft3

    Terminal Velocity

    Harold Vance Department of Petroleum Engineering

    =Vt 4gdccf

    3Cd f

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    Terminal Velocity

    Harold Vance Department of Petroleum Engineering

    Vt = 3.369dcTc

    P

    For flat cuttings

    Vt = 4.164dcTc

    P

    For sub-round cuttings, T and P are atbottom hole conditions in 0R and psia.

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    Terminal Velocity

    Terminal velocity in air drilling

    is determined mainly by: cutting diameter, shape, and

    density.

    bottom hole temperature andpressure.

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    Factors Effecting Vt

    Shape (roundness).

    Increased Size.Increased Temperature.

    Increased Density.

    Increased Pressure.

    Increases.

    Increases. Increases.

    Increases.

    Decreases.

    Harold Vance Department of Petroleum Engineering

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    Terminal VelocityAs pressure increases Vt decreases.

    As pressure increases Air velocity

    decreases.

    If the mass flow rate of gas remainsconstant the local air velocity

    decreases with increasing pressure.The air flow rate required to lift the

    cuttings increases with increasing BHP.Harold Vance Department of Petroleum Engineering

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    =m +dP fm mV

    2m

    dL 2g (Dh Dp)Eq. 2.5

    fm Friction factor of the mixture

    of air and cuttings.

    m Mixture density, lbm/cu.ft.

    Vm Mixture velocity, ft/s.g Acceleration due to gravity.

    Dh Hole diameter, ft.

    Dp Pipe diameter, ft.

    Friction Pressure

    Harold Vance Department of Petroleum Engineering

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    Friction Pressure

    Harold Vance Department of Petroleum Engineering

    fm= a + c

    a =

    0.14

    ( Dh Dp)0.333

    Weymouth quation.

    Gou argued that Nikuradse is more correct.

    1a

    = 1.14 0.86ln 2

    Dh - Dp

    = absolute roughness of the pipe.

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    Friction Pressure

    Mixture density of air and cuttings inthe annulus is determined by the massof the cuttings and the density of theair.

    Air density is a function of the pressure.

    Mass of the cuttings in the wellbore is afunction of:

    ROP Hole cleaning efficiency.

    Harold Vance Department of Petroleum Engineering

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    Friction Pressure

    Pressure drops down the drillstringand through the bit play a part inBHP due to temperature effects.

    Temperature is also effected by:

    Formation temperature.

    Influx of formation fluid (expansionof gas into the wellbore).

    Mechanical friction.

    Pressure.Harold Vance Department of Petroleum Engineering

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    Required injection rates?Relating downhole air velocities to

    surface injection rates is quite

    complex.We need cuttings shape and size

    to determine terminal velocity.

    Methods required knowledge ofthe cutting shape and size.

    Harold Vance Department of Petroleum Engineering

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    Minimum Energy CriteriaProbably the most widely used criteria

    was developed by Angel in 1957.

    Angel assumed that, for efficientcuttings transport downhole, thekinetic energy of the air striking each

    cutting should be the same as that ofair giving efficient cuttings transportat standard pressure andtemperature.

    Harold Vance Department of Petroleum Engineering

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    Minimum Energy Criteria

    Harold Vance Department of Petroleum Engineering

    1

    2minV

    2min= stpV

    2stp

    1

    2

    Pmin Density of air (or gas) at the minimumrequired downhole injection rate, lbm/cuft.

    Vmin Air (or gas) velocity downhole, ft/min.

    Pstp Density of air (or gas) at standard temp andpressure, lbm/cuft.

    Vstp Air (or gas) velocity at standard Temp andpressure, ft/min.

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    Minimum Energy Criteria

    Harold Vance Department of Petroleum Engineering

    Vmin= Vstp

    Pstp

    Pmin

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    Minimum Energy Criteria

    Experience from shallow blast holes,drilled in limestone quarryingoperations, indicated that cuttings were

    transported efficiently if the air velocityequaled or exceeded 3,000 feet perminute.

    This is equivalent to Grays terminalvelocity for flat cuttings with a diameterof 0.46 in. and for sub-rounded particlesof 0.26 in.

    Harold Vance Department of Petroleum Engineering

    Minimum Energy Criteria

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    Minimum Energy Criteria

    Harold Vance Department of Petroleum Engineering

    dP

    dL= m+

    mmV2

    m

    2g (Dh Dp)

    m = a 1+Wc

    Wa

    Wc Mass of cuttings generated in a given time;the mass flow rate of cuttings, lbm/min.

    Wa Mass of air flowing past any point in the well ingiven time; the mass flow rate of air, lbm/min.

    Angel computed the downhole air pressure

    with eq. 2.5

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    Minimum Energy Criteria

    Harold Vance Department of Petroleum Engineering

    Pb = P2

    s-abTs

    2 T abT2

    G a Ts G - a+

    2aG

    Ps Surface air pressure, lbf/sq.ft, absolute.

    Ts Surface temperature,0F.

    G Annular temperature gradient,0

    F/100.T Downhole temperature = Ts+Gh

    h Hole depth.

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    Minimum Energy Criteria

    Harold Vance Department of Petroleum Engineering

    SQ + 28.8.

    ROP.

    Dh2

    53.3Qa =

    S Gas specific gravity (air=1)

    Q Gas flow rate, scf/mROP Penetration rate, ft/hr

    1.625 x 10-6Q2

    (Dh Dp) 1.333 (Dh2 Dp2)2b=

    Dh Hole diameter, ft.

    D2 Drillpipe diameter, ft.

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    Minimum Energy CriteriaThis was combined with the cuttingstransport criterion defined in Eq 2.10to deduce the minimum air flow rate

    as a function of hole depth, annulargeometry, and penetration rate.

    Eq. 2.10

    Harold Vance Department of Petroleum Engineering

    Vmin = Vstp stpmin

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    Minimum Energy Criteria

    To simplify, the average downholetemperature can be used to

    calculate BHP.

    Harold Vance Department of Petroleum Engineering

    6.61S(Ts + Gh) Q2

    (D2

    h D2

    p)2

    V2

    stp

    = (P2s + bT2

    av) e2ah/Tav bT2av

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    This was solved numerically for the gasinjection rate required to give anannular velocity equivalent in cuttingslifting power to air with a velocity of3000 ft/min.

    A series of charts was generated fordifferent combinations of hole size,drillpipe diameter and penetration rates

    Minimum Energy Criteria

    Harold Vance Department of Petroleum Engineering

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    Qmin can be approximated by:

    Qmin = Qo + NH

    Qo Injection rate (scfm) at zerodepth that corresponds to anannular velocity of 3000 ft/min

    N Factor dependent on thepenetration rate (Appendix C)

    H Hole depth, (thousands of feet).

    Harold Vance Department of Petroleum Engineering

    Minimum Energy Criteria

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    Data for calculating approximate circulation rates required toproduce a minimum annular air velocity which is equivalent in

    lifting power to standard air velocity of 3.000 ft/min.

    (Angel, 1957).

    Appendix C

    Harold Vance Department of Petroleum Engineering

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    Harold Vance Department of Petroleum Engineering

    BottomholePress

    ure(psia)

    250

    200

    150

    100

    50

    0

    0 2000 4000 6000 8000 10000 12000

    Depth (feet)

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    Harold Vance Department of Petroleum Engineering

    BottomholePress

    ure(psia)

    0 2000 4000 6000 8000 10000 12000

    Depth (feet)

    80

    70

    50

    40

    30

    20

    10

    0

    60

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    7-7/8 hole 3-1/2 drillpipe

    6 drill collars 3800 hole depth

    Harold Vance Department of Petroleum Engineering

    Annular Bottomhole Pressuresin An Air Drilled Hole-comparison OfPredictions And Measurements Made While Circulating Off-bottom

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    Harold Vance Department of Petroleum Engineering

    BottomholePressure(psia)

    45

    40

    25

    20

    30

    35

    500 600 700 800 900 1000 1100 1200 1300

    Flow Rate (scfm)

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    Harold Vance Department of Petroleum Engineering

    BottomholePress

    ure(psia)

    500 600 700 800 900 1000 1100 1200 1300

    Flow Rate (scfm)

    34

    32

    30

    28

    26

    24

    22

    20

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    Harold Vance Department of Petroleum Engineering

    Comparison of air rates recommended by several different cuttingstransport analyses (after Guo et al, 199412).

    RequiredRateo

    fAir(scfm)

    3.5

    3

    2.5

    2

    1.5

    1

    0.5

    00 2000 4000 6000 8000 10000 12000 14000 16000 18000

    Depth ( feet)

    Minimum BHP Criteria

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    Minimum BHP Criteria

    Angel analysisdoes not predict aminimum BHP, butgives a pressure

    that decreasesmonotonicallywith decreasingair flow rate.

    The influence of air flow rate onannular pressure drop (after Supon

    and Adewumi 19915)

    Annulus Air Velocity

    AnnulusPressureDrop

    AnnulusPressureDrop