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ProductionFacilities and processing of production Intermediate 29 min read

Water injection systems

A water injection system is the whole chain from the source of water to the reservoir: the water intake, water treatment, pump stations, water lines, distribution to the wells, and the injection wells. In Russian-language practice it is called a pressure maintenance system (in Russian, PPD), because the injected water keeps up the reservoir pressure. For years the system must deliver the volume of water that the field needs, with such quality and at such pressure that the reservoir takes it without getting plugged, and without cracking where cracking does harm.

Why it matters

Waterflooding (pushing the oil to the wells with injected water) gives most of the oil of many fields. The pressure maintenance system is one of the most expensive and energy-hungry parts of a field. A mistake in the choice of the source or in the treatment of the water leads to scale (hard mineral deposits) and plugged wells. A mistake in pressure leads to fractures, and the water goes along them to the producing wells, past the oil. This lesson explains where the water comes from and how we check that waters are compatible, what quality requirements the water must meet and how we treat it, and how the pumps and the distribution to the wells are arranged. It also explains how injectivity (how much water a well takes for a given pressure), wellhead pressure and fracture propagation pressure (the pressure above which the rock cracks) are related, and how we monitor injection.

Quick refresher

  • A pressure maintenance system consists of a source, treatment, pump stations, water lines, distribution blocks and injection wells. We design it for the whole life of the field: the share of produced water in the injection grows with time, and the share of source water falls.
  • Each source brings its own troubles: produced water brings oil, suspended solids, hydrogen sulfide and bacteria; underground water brings gases and iron; sea water brings oxygen, living organisms and sulfates; fresh surface water brings seasonal turbidity (cloudiness) and the swelling of clays. Incompatible waters mixed at the surface form a precipitate right in the pipes, filters and wells.
  • The reservoir sets the water quality: particles a third of the pore throat size or larger build a cake (a layer of solids) on the wall of the well, and those from a tenth to a third plug the pores from inside. The lower the permeability, the smaller the allowed particles.
  • We remove oxygen first mechanically, by vacuum or by stripping with gas (blowing gas through the water), which lowers its partial pressure. Then we bind what is left with a scavenger. Without deaeration, we need more than a hundred times as much scavenger.
  • The bottomhole pressure of an injection well is the wellhead pressure plus the weight of the water column minus the friction in the tubing. The injection limit is set by the fracture propagation pressure at the bottom of the hole. We can convert it to a wellhead pressure only for a given rate, because at a high rate the friction amounts to megapascals.
  • The pump station keeps the pressure needed by the “tightest” well (the one that takes water with the most difficulty), the others are throttled, and part of the power is lost in chokes. A Hall plot (a plot of cumulative pressure × time against cumulative injected volume) built from daily data shows plugging (the slope grows), cleaning and the opening of fractures (the slope falls): the slope equals 1/I1/I.
Key relationships
I=qpw−pˉI = \dfrac{q}{p_w - \bar p}

injectivity index of an injection well

pw=pwh+ρgH−Δpfrp_w = p_{\text{wh}} + \rho g H - \Delta p_{\text{fr}}

bottomhole pressure in injection: wellhead pressure plus the water column minus the friction in the tubing

qmax⁡=I (pfrac−Δpmargin−pˉ)q_{\max} = I\,(p_{\text{frac}} - \Delta p_{\text{margin}} - \bar p)

the largest rate at which the bottomhole pressure stays below the fracture propagation pressure with a margin

dth≈28k/ϕd_{\text{th}} \approx 2\sqrt{8k/\phi}

pore throat diameter by the model of a bundle of straight capillaries (a lower estimate)

ΔΣ(pw−pˉ)ΔtΔW=1I\dfrac{\Delta\Sigma(p_w - \bar p)\Delta t}{\Delta W} = \dfrac{1}{I}

slope of the Hall plot in steady injection

Common pitfalls
  • Mixing waters of different sources without a compatibility analysis: the precipitate will form in your own system.
  • Converting the fracture pressure limit to the wellhead with the hydrostatic pressure alone, or carrying a wellhead pressure limit found at a high rate over to a low rate.
  • Counting on an oxygen scavenger to replace the deaerator.
  • Judging plugging by the rise of the injection pressure without taking the rate into account. The right way is to look at the injectivity and at the slope of the Hall plot.
  • Keeping the pressure of the whole station for one “tight” well, instead of stimulating that well (treating the zone around it) or giving it a separate pump.

After this lesson you can

  • compare the sources of water for injection (produced, underground, sea and surface water) and name the treatment that each one needs
  • judge the compatibility of waters that are mixed in one system, and estimate the mass of salt that can drop out in it in a year
  • link the allowed particle size in the water to the pore throats (the narrow openings between pores) of the reservoir, and list the other quality requirements
  • calculate what partial pressure of oxygen a deaerator (a unit that removes oxygen) must leave and how much scavenger (a chemical that binds oxygen) is needed for the remainder
  • calculate the wellhead pressure of an injection well, counting hydrostatic pressure and friction, find the largest rate without opening a fracture, and estimate the power losses in distributing water among wells
  • read the injection history from a Hall plot: plugging, treatment and the opening of a fracture

What an injection system consists of

The field development project decides how much water to inject, and where. It sets the voidage replacement (how much of the volume of oil and water taken out is put back by injection), the pattern of injection wells, and the pressure in the reservoir (Why water is injected: pressure maintenance and oil displacement). The injection system has to deliver this: it takes the water, treats it, raises its pressure and distributes it to the wells, day after day, for decades. The volumes are large. One injection well takes from tens to thousands of cubic metres a day, and a field takes tens of thousands (loads on the facilities).

Pressure maintenance system: water sources, treatment, water injection pump station, high-pressure water line, water distribution block and injection wellswater supplywellPWRU:produced waterCPF:produced waterwatertreatment:cleaning,filters, gases,chemicalsWIPS:pumpsWDB:meteringinjectionwellslow pressurehigh pressurewater quality checkWIPS — water injection pump station,WDB — water distribution block

A diagram from left to right. On the left are three sources: a water supply well with a submersible pump, produced water from the preliminary water removal unit, and water from the central processing facility. They come together in a water treatment block: removal of oil and suspended solids, filters, removal of gases, chemicals. Then a low-pressure water line leads to the water injection pump station with multistage centrifugal pumps, and from there a thick high-pressure water line leads to the water distribution block with flowmeters and regulators, from which three lines go to the injection wells. Circles mark the points where the water quality is checked: after treatment, at the outlet of the pump station and at the wellheads.

SchematicA pressure maintenance system on land (schematic): sources of water, treatment, the water injection pump station (WIPS), high-pressure water lines, the water distribution block (WDB) and the injection wells. The circles mark the points where the water quality is checked. In the boxes on the left, PWRU is the preliminary water removal unit and CPF is the central processing facility. WIPS, WDB, PWRU and CPF are short labels used only in the figure.
Links of the pressure maintenance system
  1. 1
    Source and water intake

    Water supply wells with submersible pumps, a sea water intake with screens, and produced water from the preliminary water removal units and the central processing facility (Produced water: composition, treatment and disposal).

  2. 2
    Treatment

    Removal of oil and suspended solids, filtration, removal of oxygen and hydrogen sulfide, and dosing of chemicals. Each source has its own scheme.

  3. 3
    Pump stations

    Water injection pump stations, often in packaged form (assembled from factory-made blocks), with multistage centrifugal pumps. Booster pumps give the main pumps enough pressure at their inlet.

  4. 4
    Water lines

    Low-pressure lines go from the treatment to the pump stations, and high-pressure lines from the stations to the wells. Coatings protect them from corrosion, or they are made of fibreglass.

  5. 5
    Distribution

    Water distribution blocks have a flowmeter and a flow regulator for each well. Injection is metered well by well here.

  6. 6
    Injection wells

    A wellhead with valves and pressure gauges, and tubing (the pipe that carries the water down the well) with a packer (a seal that closes the space around the tubing). The packer protects the casing (the steel pipe that lines the well) from the injection pressure. When water is injected into several formations, equipment for separate injection is used (Multiple-zone completions: commingled and segregated production).

The pump stations are based on sectional multistage centrifugal pumps (in Russian practice they have the type name CNS). Such a pump has many impellers (spinning wheels with blades) one after another on one shaft, and each stage adds to the pressure. The designation gives the delivery in cubic metres per hour and the head in metres (the height to which the pump could lift the water). For example, the pump CNS 180-1900 delivers 180 m³/h at a head of 1900 m. The head is converted to pressure through the density of the liquid pumped, Δp=ρgH\Delta p = \rho g H: 1900 m of fresh water is about 18.6 MPa, and 1900 m of brine with a density of 1040 kg/m³ is about 19.4 MPa. A pump develops the same head, and the pressure depends on what it pumps. For individual wells with low injectivity (wells that take little water for a given pressure), we install separate pumps: plunger pumps (piston pumps, good for high pressure at a low rate), or horizontal multistage pumps at the wellhead.

Injection is one of the largest consumers of energy in a field. The hydraulic power of the pumps equals the rate times the pressure rise (hydraulic power), and it grows together with the injected volumes. So we keep the pressure in the system no higher than needed, and we adjust the power of the pumps with variable speed drives (devices that change the pump speed), not by throttling (closing a valve to hold the flow back). By the affinity laws the delivery of a pump is proportional to the rotation speed, and its head is proportional to the square of it.

Where the water comes from

Sources of water for injection
Source
Produced water
Advantages
available in any field with a water cut (water in the produced liquid); injection into its own reservoir
Difficulties
oil, suspended solids, hydrogen sulfide, bacteria; the volume is set by production
Treatment
removal of oil and suspended solids, a closed system, biocides (chemicals that kill bacteria)
Source
Underground water of aquifers (water-bearing layers)
Advantages
constant composition, few suspended solids, usually no oxygen
Difficulties
iron, carbon dioxide or hydrogen sulfide; water supply wells are needed
Treatment
removal of gases and iron, filtration
Source
Sea water
Advantages
unlimited volume at offshore fields
Difficulties
saturated with oxygen, full of living organisms, rich in sulfate
Treatment
screens and filters, chlorination, deaeration (removal of dissolved oxygen), and if needed removal of sulfates
Source
Fresh surface water (rivers, lakes)
Advantages
available near the shore
Difficulties
turbidity and composition change with the seasons; fresh water harms shaly (clay-rich) reservoirs
Treatment
settling with coagulants (chemicals that make fine particles clump together), filtration, deaeration
Source
Crossflow from an aquifer in the same well
Advantages
no surface facilities
Difficulties
the rate is hard to measure and control; a strong aquifer is needed
Treatment
only a check of the compatibility of the formations

The last option (a dump flood) is possible when an aquifer with a higher pressure lies above or below the productive formation: the water flows across in the same well by itself or with the help of a submersible pump.

How much water is needed from the source depends on the year of development. With full voidage replacement it is the reservoir volume of the produced oil, qoBo/Bwq_oB_o/B_w. In the example of the lesson on produced water it is about 7.8 thousand m³/d on the plateau and about 0.8 thousand in year 20, when the injection consists almost entirely of produced water (the water balance of a field). So we size the water intake and the treatment of source water for the first years. Later we take them out of service in parts or reassign them, while we build up the treatment of produced water.

The law of Kazakhstan also affects the choice. Under the Water Code, taking underground water or water from surface water bodies is, as a general rule, special water use, which needs a permit. Drinking water must not be used in industry if water of another quality will do and the process does not require drinking water. Under the Environmental Code, injecting produced formation water, sea water, desalinated water, or industrial water with a salinity of 2000 mg/L or more for pressure maintenance is not counted as a discharge (as of the texts of the codes of October 2026).

Water compatibility and scale

The injected water must be compatible with three things: with the reservoir rock (it must not cause swelling or movement of clays), with the formation water (it must not form precipitates where they meet), and with the other waters with which it is mixed in the same system. The first two checks are covered in the lesson on formation damage in injection. The same lesson has the saturation index and the mass of precipitate for the example of barium sulfate. Here we take the third: mixing at the surface, where the precipitate (a solid that drops out of the water) forms not in the reservoir but in the system's own pipes, filters and wells.

While there is little produced water, we mix it with the water of the source, and the share of each changes from year to year. If the produced water contains barium or strontium and the source water contains sulfate, the mixture becomes supersaturated with barium or strontium sulfate: it holds more of the dissolved salt than the water can keep, and the salt starts to settle out. A similar trouble is calcium carbonate: on heating and loss of carbon dioxide, a mixture rich in calcium and bicarbonate deposits carbonate on the walls of heat exchangers and pipes.

Worked exampleCan produced water be mixed with water from an aquifer?
Given (assumed data)
Produced water
barium 15 mg/L, practically no sulfate
Aquifer water (the source)
sulfate 900 mg/L, no barium
Shares in the injection
from the water balance of the field in the lesson on produced water: in year 8, 14,040 m³/d are injected, of which 6740 is source water; in year 20, 12,947 m³/d, of which 799 is source water
Constants
as in the lesson on formation damage: the solubility product of barite Ksp=1.08⋅10−10K_{sp} = 1.08\cdot 10^{-10} (mol/L)² at 25 °C, the product of the activity coefficients 0.03; molar masses: barium 137.33, sulfate 96.06, barite 233.38 g/mol
Solution
  1. Year 8. The share of source water is 6740/14,040=0.4806740/14{,}040 = 0.480. In the mixture there is barium (1−0.480)⋅15/137.33=0.0568(1 - 0.480)\cdot 15/137.33 = 0.0568 mmol/L and sulfate 0.480⋅900/96.06=4.4970.480\cdot 900/96.06 = 4.497 mmol/L.
  2. The saturation index is SI=log⁡100.03⋅0.0568⋅10−3⋅4.497⋅10−31.08⋅10−10\mathrm{SI} = \log_{10}\dfrac{0.03\cdot 0.0568\cdot 10^{-3}\cdot 4.497\cdot 10^{-3}}{1.08\cdot 10^{-10}} =1.85= 1.85. The mixture is strongly supersaturated.
  3. By the formula for the mass of precipitate, x=0.0560x = 0.0560 mmol/L drops out, which is 98.6% of the barium of the mixture; there is tens of times more sulfate. This is 0.0560⋅233.38=13.070.0560\cdot 233.38 = 13.07 g of barite per cubic metre, or 13.07⋅14,040/1000=183.513.07\cdot 14{,}040/1000 = 183.5 kg a day, or 67.0 t a year.
  4. Year 20. The share of source water is 799/12,947=0.0617799/12{,}947 = 0.0617; barium 0.1025 and sulfate 0.578 mmol/L; SI=1.22\mathrm{SI} = 1.22, which is lower than in year 8.
  5. But x=0.0950x = 0.0950 mmol/L drops out (92.7% of the barium), 22.18 g/m³, which is 22.18⋅12,947/1000=287.222.18\cdot 12{,}947/1000 = 287.2 kg a day, or 104.8 t a year. For comparison, all the barium of the produced water expressed as barite is 12,148⋅15⋅233.38/137.33/100012{,}148\cdot 15\cdot 233.38/137.33/1000 =309.7= 309.7 kg a day.
Answer: No, they cannot be mixed. In year 8 about 183.5 kg of barite a day (67.0 t a year) can drop out in the system, and in year 20 about 287.2 kg a day (104.8 t a year), although the saturation index fell from 1.85 to 1.22.

What it means. While there is more sulfate in the mixture than barium, almost all the barium that the produced water brings drops out, and the mass of precipitate grows together with the produced water, although the saturation index falls. The index tells about the “driving force”, not about the amount. Tens of tonnes of barite a year means plugged filters, pumps, water lines and perforation tunnels of the injection wells (the channels shot through the casing into the reservoir), and barite hardly dissolves in acid. There are three ways out. We can inject the waters separately, into different groups of wells (but after breakthrough they will meet at the producing wells; Sources of formation damage). We can choose a source without sulfate. Or we can remove the sulfate with membranes (nanofiltration: membranes with very fine pores). An inhibitor delays the precipitation but does not change the equilibrium. With such supersaturation and tonnes of possible precipitate, it only moves the precipitation further along the path of the water, to the injection well and into the reservoir near it. The composition of the produced water was taken as constant, although after breakthrough of the injected water it has less barium, so for the late years the calculation overestimates the precipitate. The constant is taken for 25 °C and the product of the activity coefficients is assumed. With a large excess of sulfate (year 8) the barium sets the mass of precipitate, and refining the constants hardly changes it. With a smaller excess (year 20) the mass is more sensitive to them, so we refine it with a calculation at the working temperature and salinity. The data in this example are assumed for illustration.

Barite that can drop out when produced water is mixed with aquifer water46810121416182022050100150200250300350Project yearBarite, kg/dSI 1.85SI 1.22all the barium of produced watercan drop out

A chart in kilograms of barite per day, from 0 to 350, by project year from 5 to 21. The solid curve starts from zero in year 5, when there is no produced water, grows quickly to about 180 in year 8, and then slowly to about 290 by year 20. The dashed line of the barium of the produced water runs a little above it and separates from the solid curve in the late years, when there is little sulfate in the mixture: in year 20 about 310 against 287.

CalculatedBarite that can drop out in the injection system when produced water (barium 15 mg/L) is mixed with aquifer water (sulfate 900 mg/L), by year. The dashed line is all the barium of the produced water expressed as barite. The shares of the waters follow the water balance of the field at full voidage replacement.
  • Water analysis: the full ion composition of each water, including barium, strontium, iron, bicarbonate, sulfate and pH, in several samples. The composition of produced water changes with the breakthrough of the injected water.
  • Calculation of mixtures: the saturation index and the mass of precipitate for all mixing ratios, at the temperature and pressure of each part of the system, from the water intake to the bottom of the hole.
  • Laboratory check: mixing the waters in different proportions at working temperature and watching for cloudiness and precipitate, and flowing the water through core of the reservoir.
  • Decision: separate systems, another source, removal of sulfates or softening (removing calcium and magnesium), and inhibitors where the supersaturation is small.

Water quality requirements

An injection well takes hundreds of thousands of cubic metres of water in a year, and everything that is suspended in the water stays near the wellbore. Even a few milligrams per litre means hundreds of kilograms of particles a year (plugging in injection). Not only particles of sand and clay are dangerous, but also oil droplets, which glue particles together and reduce the permeability to water, corrosion products, iron sulfide and the slime of bacteria. Which particles are dangerous for a particular reservoir is set by the size of its pore throats.

An empirical rule (a rule found from experience; selection of bridging agents) says that particles a third of the throat diameter or larger are held at the wall of the well and build an external cake. Particles from a tenth to a third penetrate the reservoir and plug the pores from inside, and still smaller ones pass through. We measure the throat size on core by mercury injection (forcing mercury into a sample under rising pressure). For an estimate, a simple model is enough: a bundle of capillaries (the bundle of capillaries model):

Pore throat diameter by the model of a bundle of straight capillaries
dth≈28kϕd_{\text{th}} \approx 2\sqrt{\frac{8k}{\phi}}
where:
  • dthd_{\text{th}}characteristic diameter of the pore throat, m
  • kkpermeability of the reservoir (1 mD = 0.987⋅10−150.987\cdot 10^{-15} m²), m²
  • ϕ\phiporosity, fraction

Units: SI

Holds when
  • The rock is represented by a bundle of identical straight tubes. With tortuosity τ\tau (the winding of the flow paths) the radius is τ\tau times larger, so the formula gives a lower estimate, and the allowed particle sizes derived from it have a margin.
  • This is an order-of-magnitude estimate. Real throats have a wide distribution of sizes, and the design is based on the large ones, which carry the main flow.

The throats grow as the root of the permeability: a reservoir ten times more permeable has throats about three times wider. So a tight reservoir needs water cleaned of finer particles.

Worked exampleWhich particles are dangerous for two reservoirs
Given (assumed data)
Reservoir A
permeability 50 mD, porosity 0.18
Reservoir B
permeability 500 mD, porosity 0.22
Solution
  1. Reservoir A: k=50⋅0.987⋅10−15=4.935⋅10−14k = 50\cdot 0.987\cdot 10^{-15} = 4.935\cdot 10^{-14} m², dth=28⋅4.935⋅10−14/0.18d_{\text{th}} = 2\sqrt{8\cdot 4.935\cdot 10^{-14}/0.18} =2.96= 2.96 µm.
  2. Particles of a third of the throat, 2.96/3=0.992.96/3 = 0.99 µm, build a cake on the wall. Particles from a tenth, 0.300.30 µm, up to 0.99 µm, penetrate and plug the pores.
  3. Reservoir B: k=4.935⋅10−13k = 4.935\cdot 10^{-13} m², dth=8.47d_{\text{th}} = 8.47 µm. The cake is built by particles of 2.82 µm and larger, and particles from 0.85 to 2.82 µm penetrate inside.
Answer: The throats of reservoir A are about 2.96 µm, and its pores are plugged by particles from 0.30 to 0.99 µm. The throats of reservoir B are about 8.47 µm, and the particles dangerous for its pores are three times larger, from 0.85 to 2.82 µm.

What it means. Water that is fit for reservoir B can plug reservoir A: a filter that holds back particles from 5 µm will let into it exactly the particles that plug the pores from inside. This is the logic of the industry standards: the lower the permeability, the lower the allowed content of suspended solids and the finer the particles. The estimate is rough and made with a margin, because with tortuosity the throats are wider. We refine it with the throat size distribution from mercury injection tests and by flowing water through core. The data in this example are assumed for illustration.

What is limited in injection water and why
Indicator
Suspended particles and their size
Why it is dangerous
a cake on the wall, plugging of pores
How it is met
settling, filtration, coagulants
Indicator
Oil
Why it is dangerous
glues particles together and reduces the permeability to water
How it is met
treatment of produced water
Indicator
Dissolved oxygen
Why it is dangerous
corrosion and its products, which are new particles
How it is met
a closed system, deaeration, a scavenger
Indicator
Hydrogen sulfide and iron
Why it is dangerous
corrosion, a precipitate of iron sulfide
How it is met
degassing, removal of iron, separate systems
Indicator
Bacteria (sulfate-reducing bacteria, SRB, and others)
Why it is dangerous
slime, hydrogen sulfide, infection of the reservoir
How it is met
chlorination, biocides, cleanliness
Indicator
pH, ion composition
Why it is dangerous
scale, swelling of clays
How it is met
compatible sources, inhibitors

The exact standards for a field are set by its project documents on the basis of tests of the waters and of core.

Sea water is saturated with oxygen, so it is treated more strictly. In offshore projects we bring dissolved oxygen down to tens of parts per billion (ppb) or less, for example no more than 20 ppb at the pump outlet, because steel in salt water with oxygen quickly gets covered with pits. We check the quality at several points: after the filters, after the deaerator, at the pump outlet and at the wellheads of the most distant wells, where corrosion products and bacteria have got into the water on its way along the water lines.

Treatment of water for injection

Treatment of sea water (an example of a full scheme)
  1. 1
    Water intake

    Screens hold back debris and living organisms. We choose the place and depth of the intake so that the water is as clean and as constant in composition as possible. Lift pumps deliver it to treatment.

  2. 2
    Chlorination

    Sodium hypochlorite, often made by electrolysis of the sea water itself, kills algae and bacteria and keeps them from fouling filters and pipes.

  3. 3
    Coarse and fine filtration

    Granular filters (sand, anthracite, which is a hard coal, and garnet, a heavy mineral sand) with coagulants, then cartridge filters. We wash the filters with a reverse flow.

  4. 4
    Deaeration

    Oxygen is removed in a column, under vacuum or by stripping (a stream of gas, nitrogen or associated gas, carries the oxygen out of the water), and an oxygen scavenger takes care of what is left.

  5. 5
    Removal of sulfates

    If the formation water is rich in barium or strontium, nanofiltration membranes hold back sulfate and let sodium chloride pass.

  6. 6
    Chemicals and pumps

    Biocides in shock doses from time to time, scale and corrosion inhibitors, and booster and injection pumps.

We treat produced water by the scheme of the lesson on produced water: settling tanks, hydrocyclones, flotation, filters. We keep it in a closed system without air. Underground water usually needs only to be freed of gases and iron and filtered. If we remove the iron by oxidation, we must remove the oxygen again afterwards. We check each scheme for mixing with all the other waters of the system.

Deaeration (removing dissolved oxygen) rests on Henry's law: the equilibrium concentration of a dissolved gas is proportional to its partial pressure over the water. Water saturated with air holds about 7–10 mg/L of oxygen (less in sea water than in fresh water, and the less, the warmer the water), and the partial pressure of oxygen in air is about 21 kPa. To leave only tens of parts per billion in the water, the partial pressure of oxygen over the water must be hundreds of times lower. We do this by lowering the total pressure (vacuum) or by replacing the gas over the water with an oxygen-free one (stripping).

Equilibrium oxygen content of water (Henry's law)
C=Csat pO2pO2airC = C_{\text{sat}}\,\frac{p_{\mathrm{O_2}}}{p_{\mathrm{O_2}}^{\text{air}}}
where:
  • CCequilibrium concentration of dissolved oxygen, mg/L
  • CsatC_{\text{sat}}concentration in water saturated with air at atmospheric pressure, at the same temperature and salinity, mg/L
  • pO2p_{\mathrm{O_2}}partial pressure of oxygen in the gas over the water (the share of oxygen times the absolute pressure), kPa
  • pO2airp_{\mathrm{O_2}}^{\text{air}}partial pressure of oxygen in air: 0.2095⋅101.325=21.230.2095\cdot 101.325 = 21.23 kPa, kPa

Units: concentrations in identical units, pressures in identical units

Holds when
  • Equilibrium: the water is in contact with the gas long enough. In a column it is approached gradually, stage by stage, so in practice more oxygen is left.
  • The temperature and salinity are the same as for CsatC_{\text{sat}}. With heating, the solubility of oxygen falls.

A deaerator cannot leave less in the water than corresponds to the partial pressure of oxygen in the gas over it. This sets the requirements for the vacuum and for the purity of the stripping gas. The remainder is bound chemically.

Worked exampleA deaerator and an oxygen scavenger for sea water
Given (assumed data)
Water
sea water, 20,000 m³/d at 15 °C; saturated with air, about 8 mg/L of oxygen
Requirement
not more than 20 ppb (0.020 mg/L) of oxygen in the injection water
Deaerator
a vacuum column at 4 kPa (abs.) or a gas stripping column at 150 kPa (abs.); 50 ppb is left after the column
Scavenger
sodium bisulfite: 2 NaHSO3+O2→Na2SO4+H2SO42\,\mathrm{NaHSO_3} + \mathrm{O_2} \to \mathrm{Na_2SO_4} + \mathrm{H_2SO_4}; molar masses NaHSO3\mathrm{NaHSO_3} 104.06, O2\mathrm{O_2} 32.00, SO42−\mathrm{SO_4^{2-}} 96.06 g/mol
Solution
  1. The partial pressure of oxygen in equilibrium with 0.020 mg/L is 21.23⋅0.020/8=0.053121.23\cdot 0.020/8 = 0.0531 kPa, which is 400 times less than in air.
  2. In a vacuum column at 4 kPa, the share of oxygen in the gas over the water must be not more than 0.0531/4=1.330.0531/4 = 1.33%. With stripping at a pressure of 150 kPa, the stripping gas must contain not more than 0.0531/1500.0531/150, that is 354 ppm of oxygen (by moles).
  3. Scavenger: for 1 mg of oxygen, 2⋅104.06/32.00=6.502\cdot 104.06/32.00 = 6.50 mg of bisulfite. After the column: 0.05⋅6.50=0.3250.05\cdot 6.50 = 0.325 mg/L, that is 6.5 kg a day (with no margin for incomplete reaction).
  4. Without a deaerator: 8⋅6.50=52.08\cdot 6.50 = 52.0 mg/L, which is 1040 kg a day, or 380 t a year.
  5. Each milligram of oxygen turns into 2⋅96.06/32.00=6.002\cdot 96.06/32.00 = 6.00 mg of sulfate: after the column this is 0.30 mg/L, without it 48.0 mg/L.
Answer: The deaerator must keep the partial pressure of oxygen at not more than 0.0531 kPa: in a vacuum column at 4 kPa, not more than 1.33% of oxygen in the gas. Then about 6.5 kg of scavenger a day are needed, and without a deaerator about 1040 kg, which is 160 times more.

What it means. Mechanical deaeration removes almost all the oxygen, and chemistry cleans up the remainder. Full chemical removal would take hundreds of tonnes of chemical a year, and the chemical itself would add almost 50 mg/L of sulfate to the water, one more reason for barite if the formation water contains barium. We inject the scavenger after the column and far from the chlorination point, because chlorine and bisulfite react with each other and are wasted. The calculation is an equilibrium one: a column works worse than equilibrium, so we take the vacuum and the stripping gas with a margin. The data in this example are assumed for illustration.

Bacteria need special attention. Sulfate-reducing bacteria brought in with the water, especially sea water, which is rich in sulfate, multiply in the reservoir near the injection wells and produce hydrogen sulfide. Years later it appears in the production of producing wells that earlier gave “sweet” oil (oil without hydrogen sulfide). So we treat the injected water with biocides, and we monitor the bacteria and the hydrogen sulfide in the production from the first years of waterflooding.

Pumps, water lines and distribution to the wells

From the pump station the water goes along high-pressure water lines to the water distribution blocks, and from there to the wells. The pressure at the outlet of the station is one for all, but the wells need different pressures: each has its own injectivity and its own design rate. The station keeps the pressure needed by the “tightest” well, and for the others it is lowered by regulators and chokes (valves or narrow openings that take off the extra pressure). The energy that the pump spent on this excess pressure turns into heat.

Power lost in throttling
Nthr=∑iqi (phdr−pwh,i)86.4N_{\text{thr}} = \sum_i \frac{q_i\,(p_{\text{hdr}} - p_{\text{wh},i})}{86.4}
where:
  • NthrN_{\text{thr}}hydraulic power that the pump spends on pressure that the regulators then take off, kW
  • qiq_iinjection rate into well ii, m³/d
  • phdrp_{\text{hdr}}pressure in the header of the water distribution block, MPa
  • pwh,ip_{\text{wh},i}wellhead pressure that well ii needs for its rate, MPa

Units: metric oilfield units: m³/d, MPa, kW

Holds when
  • 86.486.4 is the same constant as in the formula for the hydraulic power of a pump: the seconds in a day divided by a thousand.
  • The losses in the water lines from the station to the block are the same for all wells and are not included here.
  • The electric power is 1/η1/\eta times the hydraulic power, where η\eta is the efficiency of the pump unit.

The losses are greater the larger the rate of the “easy” wells and the more their pressure differs from that of the “tight” one. We reduce them by splitting the wells into pressure levels, by installing separate pumps for the “tight” wells, or by stimulating those wells (treating the near-wellbore zone) so that the common pressure is enough for them.

Wells of one water distribution block
Well
IW-1
Rate, m³/d
600
II, m³/(d·MPa)
60
pwp_w, MPa
32.00
pwhp_{\text{wh}}, MPa
9.68
Well
IW-2
Rate, m³/d
450
II, m³/(d·MPa)
150
pwp_w, MPa
25.00
pwhp_{\text{wh}}, MPa
1.76
Well
IW-3
Rate, m³/d
250
II, m³/(d·MPa)
22
pwp_w, MPa
33.36
pwhp_{\text{wh}}, MPa
9.29
Well
IW-4
Rate, m³/d
700
II, m³/(d·MPa)
140
pwp_w, MPa
27.00
pwhp_{\text{wh}}, MPa
5.44

II is the injectivity, pwp_w the bottomhole pressure and pwhp_{\text{wh}} the wellhead pressure. The reservoir pressure is 22 MPa. The depth, tubing and water are as for the well of the next section: the water column gives 24.49 MPa, and the friction in the tubing is calculated from the rate. The data are assumed for illustration.

Worked exampleHow much power is lost in the chokes of a water distribution block
Given (assumed data)
Wells
four; the rates and the wellhead pressures needed are in the table above
Pump station
loss in the water line to the block 0.6 MPa, pressure at the pump inlet 0.3 MPa, efficiency of the pump unit 0.75
Solution
  1. An example of the calculation of the wellhead pressure for IW-1: the bottomhole pressure is 22+600/60=32.0022 + 600/60 = 32.00 MPa. The wellhead pressure is 32.00−24.49+2.17=9.6832.00 - 24.49 + 2.17 = 9.68 MPa, where 2.17 MPa is the friction in the tubing at 600 m³/d (the next section).
  2. The “tightest” well is IW-1: it needs 9.68 MPa. The pressure at the outlet of the station is 9.68+0.6=10.289.68 + 0.6 = 10.28 MPa, and the pumps raise it by 10.28−0.3=9.9810.28 - 0.3 = 9.98 MPa. The hydraulic power is 2000⋅9.98/86.4=231.02000\cdot 9.98/86.4 = 231.0 kW.
  3. Losses in the regulators: IW-2, 450⋅(9.68−1.76)450\cdot(9.68 - 1.76); IW-3, 250⋅(9.68−9.29)250\cdot(9.68 - 9.29); IW-4, 700⋅(9.68−5.44)700\cdot(9.68 - 5.44). The sum is 6629.5 MPa·m³/d, and 6629.5/86.4=76.76629.5/86.4 = 76.7 kW, which is 33% of the pump power.
  4. If IW-2 and IW-4 are moved to a separate header with the pressure of IW-4, 5.44 MPa, the saving is 1150⋅(9.68−5.44)/86.4=56.41150\cdot(9.68 - 5.44)/86.4 = 56.4 kW of hydraulic power, or 56.4/0.75=75.256.4/0.75 = 75.2 kW of electric power, that is 659 MWh a year.
Answer: About 76.7 kW is lost in the chokes, which is 33% of the hydraulic power of the pumps. Two pressure levels save about 75.2 kW of electric power, or 659 MWh a year.

What it means. A third of the power goes into first raising the pressure and then taking it off. Note IW-3 too: with its low injectivity it needs almost the same wellhead pressure as IW-1, and its bottomhole pressure is 33.36 MPa, close to the fracture propagation pressure. Stimulating the near-wellbore zone of IW-3 and giving IW-2 and IW-4 a separate “easy” header is often cheaper than keeping the pressure of the whole system for the worst well. The calculation is for one operating mode. The rates of the wells change, so we check the decision over the whole range. The data in this example are assumed for illustration.

Injectivity and injection pressure

How much water a well takes at a given pressure is shown by the injectivity index: the rate divided by the amount by which the bottomhole pressure exceeds the reservoir pressure. It is the mirror image of the productivity index of a producing well (productivity index). In steady state (when the pressure no longer changes with time) it is set by the transmissibility of the reservoir (permeability times thickness over viscosity), the skin (a number that shows how much the zone around the well helps or hinders flow) and the dimensions of the area. In time it changes. As the water zone around the well grows, it rises or falls depending on the ratio of the mobilities of water and oil (mobility ratio), and when the near-wellbore zone is plugged, it falls.

Injectivity index
I=qpw−pˉI = \frac{q}{p_w - \bar p}
where:
  • IIinjectivity index, m³/(d·MPa)
  • qqinjection rate at standard conditions, m³/d
  • pwp_wbottomhole pressure during injection (for producing wells the bottomhole pressure is written pwfp_{wf}), MPa
  • pˉ\bar preservoir pressure in the injection area, MPa

Units: metric oilfield units

Holds when
  • The injection is close to steady state. Right after a change of the rate, the pressure has not settled yet.
  • The reservoir pressure in the injection area is known, from a falloff test (pressure falloff after shut-in) or from neighbouring wells.
  • The fracture has not opened. After it opens, the rate grows with almost no rise in pressure, and the injectivity stops being a constant.

For a homogeneous reservoir in steady state, the injectivity is given by the same formula as the productivity, but with the viscosity and the formation volume factor of water (how much its volume changes between the reservoir and the surface; the form is below). By comparing II over time, we can see plugging and the results of well treatments.

In other unit systems (1)
Homogeneous reservoir, steady state (metric oilfield units)
I=0.536 k hμwBw(ln⁡rerw+S)I = \frac{0.536\,k\,h}{\mu_w B_w\left(\ln\dfrac{r_e}{r_w} + S\right)}

kk in mD, hh in m, μw\mu_w in mPa·s, BwB_w in m³/m³, rer_e and rwr_w in m, II in m³/(d·MPa). Here pˉ\bar p is the pressure at the boundary rer_e, as in the Dupuit equation and in the derivation of the Hall plot. If pˉ\bar p is the average pressure of the area, the brackets contain ln⁡(re/rw)−1/2+S\ln(r_e/r_w) - 1/2 + S (average pressure).

0.536=2π⋅0.08530.536 = 2\pi\cdot 0.0853, as in the Dupuit equation (Steady-state radial flow).

The pressure is measured at the wellhead, but the reservoir “sees” the bottomhole pressure. In injection the two are linked by the weight of the water column, which helps the pump, and by the friction in the tubing, which hinders it (friction factor):

Bottomhole pressure of an injection well
pw=pwh+ρgH−Δpfr,Δpfr=λ Hd ρv22p_w = p_{\text{wh}} + \rho g H - \Delta p_{\text{fr}},\qquad \Delta p_{\text{fr}} = \lambda\,\frac{H}{d}\,\frac{\rho v^2}{2}
where:
  • pwhp_{\text{wh}}wellhead pressure, Pa
  • ρ\rhodensity of the injected water, kg/m³
  • HHvertical depth of the middle of the injection interval (for friction, the length of the tubing along the hole; in a vertical well they coincide), m
  • λ\lambdaDarcy friction factor (from the Haaland formula), —
  • d, vd,\ vinner diameter of the tubing and the mean velocity of the water in it, v=4q/(πd2)v = 4q/(\pi d^2), m, m/s

Units: SI; to get MPa, divide by 10610^6

Holds when
  • A single-phase flow of water. The viscosity and density are at the mean temperature in the tubing.
  • Friction grows roughly as the square of the rate, so at a low rate it can be neglected, and at a high rate it cannot.
  • Injection down the annulus (the space between the tubing and the casing) or into a deviated well needs its own lengths and diameters.

At a constant wellhead pressure the bottomhole pressure rises when the rate falls: the friction disappears and the water column stays. That is why a pressure limit found for the bottom of the hole is converted to the wellhead for a specific rate.

The upper limit of the bottomhole pressure is set by the rock: above the fracture opening (propagation) pressure, the water goes into the reservoir through a fracture. We find this pressure with a step-rate test (step-rate test): we inject water at a series of rising rates, and a bend in the line of pressure against rate shows that a fracture has opened. We keep the bottomhole pressure below it with a margin. The limit is not constant. Cold water cools the rock near the well and lowers the fracture pressure (stresses at the wall of the well), while the rise of the reservoir pressure during injection raises it. Sometimes in tight reservoirs the injection is deliberately above the fracture opening pressure. Then the spacing of the wells is matched with the direction of the fractures, so that the water does not go along them straight to the producing wells (well patterns).

Worked exampleWhat rate and what wellhead pressure are allowed
Given (assumed data)
Well
vertical, the middle of the interval at 2400 m; tubing with an inner diameter of 62 mm, roughness 0.05 mm
Water
density 1040 kg/m³, viscosity in the tubing 0.9 mPa·s
Reservoir
reservoir pressure 22 MPa, injectivity 60 m³/(d·MPa), injection plan 600 m³/d
Fracture propagation pressure
36 MPa at the bottom of the hole from a step-rate test; the margin adopted is 1 MPa
Solution
  1. The water column: 1040⋅9.81⋅2400=24,485,7601040\cdot 9.81\cdot 2400 = 24{,}485{,}760 Pa, that is 24.49 MPa. The bottomhole pressure at 600 m³/d is 22+600/60=32.0022 + 600/60 = 32.00 MPa.
  2. Friction: v=600/86,400/(π⋅0.0622/4)=2.30v = 600/86{,}400/(\pi\cdot 0.062^2/4) = 2.30 m/s, the Reynolds number (it shows how turbulent the flow is) is about 165 thousand, λ=0.0204\lambda = 0.0204, and Δpfr=0.0204⋅24000.062⋅1040⋅2.3022\Delta p_{\text{fr}} = 0.0204\cdot\dfrac{2400}{0.062}\cdot\dfrac{1040\cdot 2.30^2}{2} =2.17= 2.17 MPa.
  3. The wellhead pressure is 32.00−24.49+2.17=9.6832.00 - 24.49 + 2.17 = 9.68 MPa.
  4. The limit: the bottomhole pressure is not higher than 36−1=3536 - 1 = 35 MPa, so qmax⁡=60⋅(35−22)=780q_{\max} = 60\cdot(35 - 22) = 780 m³/d. At this rate v=2.99v = 2.99 m/s, λ=0.0200\lambda = 0.0200, the friction is 3.60 MPa, and the wellhead pressure is 35−24.49+3.60=14.1135 - 24.49 + 3.60 = 14.11 MPa.
  5. If the limit is converted to the wellhead with hydrostatic pressure alone, 35−24.49=10.5135 - 24.49 = 10.51 MPa, the well will be allowed only about 635 m³/d, which is 19% less than it can really take.
  6. The opposite mistake: 14.11 MPa is held at the wellhead, but the injectivity has halved because of plugging. The rate will fall to about 459 m³/d and the friction to 1.30 MPa, and without a fracture the bottomhole pressure would be 14.11+24.49−1.30=37.3014.11 + 24.49 - 1.30 = 37.30 MPa, which is above the fracture propagation pressure: the fracture will open.
Answer: The plan of 600 m³/d needs 9.68 MPa at the wellhead. Without opening a fracture, the well will take up to 780 m³/d at 14.11 MPa at the wellhead. A wellhead pressure limit is valid only for its own rate.

What it means. The friction in the tubing at 600–780 m³/d is two to four megapascals, comparable to the margin to the fracture pressure. So converting between the wellhead and the bottom of the hole without friction is wrong in both directions: with hydrostatic pressure alone the limit is too low at a high rate, and a wellhead limit found at a high rate is dangerous at a low rate. It is more reliable to limit the bottomhole pressure, calculated from the wellhead pressure and the rate, or to set the wellhead pressure limit as a curve against the rate (the figure below). The cooling of the rock lowers the fracture opening pressure with time, so we review the limit with new step-rate tests. The data in this example are assumed for illustration.

Wellhead pressure of an injection well: needed for injection, and the limit020040060080010000510152025Injection rate, m³/dWellhead pressure, MPa780 m³/dpressure neededlimit: bottomhole 35 MPalimit: hydrostatic pressure only635

A chart of wellhead pressure from 0 to 25 MPa against the rate from 0 to 1000 cubic metres per day. The solid curve of the pressure needed starts from zero at 141 cubic metres per day and rises, accelerating, to 9.7 MPa at 600 and 14.1 MPa at 780 cubic metres per day. The dashed curve of the limit pressure starts from 10.5 MPa and rises slowly because of friction to 16.4 MPa at 1000 cubic metres. The curves cross at 780 cubic metres per day. A horizontal line at 10.5 MPa crosses the solid curve at about 635 cubic metres per day.

CalculatedWellhead pressure of the well of the example against the rate: the pressure needed for injection (solid line) and the limit at which the bottomhole pressure equals 35 MPa (dashed line). The horizontal line is the same limit converted with hydrostatic pressure alone. The lines meet at the largest allowed rate. Up to 141 m³/d the water column is heavier than needed, and the well takes water with no pressure at the wellhead.

Monitoring injection: the Hall plot and other signs

  • Rate and pressure of each well: daily, from the flowmeters of the water distribution blocks and the pressure gauges at the wellheads. From them come the injectivity and the Hall plot.
  • Water quality: suspended solids, oil, oxygen, iron and bacteria, after each treatment stage and at the wellheads of distant wells.
  • Corrosion: coupons and probes in the water lines, wall thickness, iron in the water.
  • Well tests: a pressure falloff after shut-in (falloff test) gives the reservoir pressure, the permeability and the skin. Injection profiles along the hole (production logging) show which layers take water. Step-rate tests give the fracture propagation pressure.
  • The reservoir: voidage replacement by area (Why water is injected: pressure maintenance and oil displacement), pressure maps, and tracer tests that show which producing wells an injection well is connected with.

The cheapest and most sensitive tool is the Hall plot. Its horizontal axis is the cumulative injection WW (the total injected so far), and its vertical axis is the cumulative sum of the excesses of the bottomhole pressure over the reservoir pressure multiplied by time, Σ(pw−pˉ)Δt\Sigma(p_w - \bar p)\Delta t. The link of the slope with permeability and skin is derived in the lesson on formation damage. For monitoring it is enough that in steady injection, in each period, (pw−pˉ)Δt=qΔt/I(p_w - \bar p)\Delta t = q\Delta t/I, that is, the sum grows in proportion to the injection with a slope 1/I1/I.

Slope of the Hall plot and injectivity
mH=Δ ⁣[∑(pw−pˉ) Δt]ΔW=1Im_H = \frac{\Delta\!\left[\sum (p_w - \bar p)\,\Delta t\right]}{\Delta W} = \frac{1}{I}
where:
  • mHm_Hslope of the Hall plot on a segment, MPa·d/m³
  • ΔW\Delta Winjection over the segment, m³
  • Δt\Delta tlength of the averaging period (a day, a month), d
  • IIaverage injectivity index over the segment, m³/(d·MPa)

Units: metric oilfield units

Holds when
  • The injection in each period is close to steady state, and the reservoir pressure in the injection area hardly changes. Its rise also increases the slope.
  • We calculate the bottomhole pressure from the wellhead pressure, counting the hydrostatic pressure and the friction at the actual rate.
  • The slope over a segment is an average. If the injectivity changed within the segment, the slope is the average value of 1/I1/I, weighted by the injection.

A straight line means that the state of the well does not change. A growing slope means that the injectivity falls (plugging, a rise of the reservoir pressure). A falling slope means that the injectivity grows, after a treatment or when a fracture opens. In the second case the pressure hardly rises when the rate grows and stands at the fracture opening pressure.

Injection history of an injection well (monthly averages)
Month
1
Rate, m³/d
600
Bottomhole pressure, MPa
32.0
W, m³
18,000
Σ, MPa·d
300
Month
2
Rate, m³/d
600
Bottomhole pressure, MPa
32.0
W, m³
36,000
Σ, MPa·d
600
Month
3
Rate, m³/d
600
Bottomhole pressure, MPa
32.0
W, m³
54,000
Σ, MPa·d
900
Month
4
Rate, m³/d
600
Bottomhole pressure, MPa
32.0
W, m³
72,000
Σ, MPa·d
1200
Month
5
Rate, m³/d
570
Bottomhole pressure, MPa
32.0
W, m³
89,100
Σ, MPa·d
1500
Month
6
Rate, m³/d
535
Bottomhole pressure, MPa
32.0
W, m³
105,150
Σ, MPa·d
1800
Month
7
Rate, m³/d
500
Bottomhole pressure, MPa
32.0
W, m³
120,150
Σ, MPa·d
2100
Month
8
Rate, m³/d
470
Bottomhole pressure, MPa
32.0
W, m³
134,250
Σ, MPa·d
2400
Month
9
Rate, m³/d
640
Bottomhole pressure, MPa
31.0
W, m³
153,450
Σ, MPa·d
2670
Month
10
Rate, m³/d
640
Bottomhole pressure, MPa
31.0
W, m³
172,650
Σ, MPa·d
2940
Month
11
Rate, m³/d
640
Bottomhole pressure, MPa
31.0
W, m³
191,850
Σ, MPa·d
3210
Month
12
Rate, m³/d
640
Bottomhole pressure, MPa
31.0
W, m³
211,050
Σ, MPa·d
3480
Month
13
Rate, m³/d
1050
Bottomhole pressure, MPa
36.1
W, m³
242,550
Σ, MPa·d
3903
Month
14
Rate, m³/d
1150
Bottomhole pressure, MPa
36.2
W, m³
277,050
Σ, MPa·d
4329
Month
15
Rate, m³/d
1250
Bottomhole pressure, MPa
36.2
W, m³
314,550
Σ, MPa·d
4755

A month is taken as 30 days, and the reservoir pressure is 22 MPa. Σ is the cumulative sum of (pw−pˉ)Δt(p_w - \bar p)\Delta t. The bottomhole pressure is calculated from the wellhead, as in the previous example. The data are assumed for illustration.

Worked exampleWhat happened to the well: reading the Hall plot
Given (assumed data)
History
the table above: months 1–4, normal injection; 5–8, the rate falls at the same pressure; at the start of month 9, an acid treatment; from month 13 the rate was raised to 1050–1250 m³/d
Fracture propagation pressure
36.0 MPa at the bottom of the hole from a step-rate test
Solution
  1. Months 1–4: ΔΣ=1200\Delta\Sigma = 1200 MPa·d, ΔW=72,000\Delta W = 72{,}000 m³. The slope is 1200/72,000=0.016671200/72{,}000 = 0.01667, and the injectivity is 72,000/1200=60.072{,}000/1200 = 60.0 m³/(d·MPa).
  2. Months 5–8: ΔΣ=1200\Delta\Sigma = 1200, ΔW=62,250\Delta W = 62{,}250. The slope is 0.01928, 16% larger, and the injectivity is 51.9: the near-wellbore zone is getting plugged.
  3. Months 9–12: ΔΣ=1080\Delta\Sigma = 1080, ΔW=76,800\Delta W = 76{,}800. The slope is 0.01406 and the injectivity is 71.1, higher than the initial one: the treatment removed not only the new plugging but also part of the old.
  4. Months 13–15: ΔΣ=1275\Delta\Sigma = 1275, ΔW=103,500\Delta W = 103{,}500. The slope is 0.01232 and the apparent injectivity is 81.2. The rate rose from 1050 to 1250 m³/d, while the bottomhole pressure stays at 36.1–36.2 MPa, at the fracture propagation pressure. Without a fracture, a rate of 1050 m³/d at an injectivity of 71.1 would need 22+1050/71.1=36.822 + 1050/71.1 = 36.8 MPa.
Answer: Plugging in months 5–8 (the injectivity from 60.0 to 51.9), a successful treatment (71.1), and from month 13 injection through a fracture: an apparent injectivity of 81.2 at a pressure that has run up against the fracture opening pressure.

What it means. The fall of the slope in the last segment looks like a success, but it is a fracture. At an injectivity of 71.1, the well without a fracture would take not more than 71.1⋅(35−22)=92471.1\cdot(35 - 22) = 924 m³/d with a margin of 1 MPa. The geology decides what to do next. If the fracture will go towards a producing well, we lower the rate. If the project provides for injection above the fracture opening pressure, we monitor the water cut of the nearest producing wells. We look for the cause of the plugging in months 5–8 in the water (suspended solids, oil, corrosion products) and confirm it with a falloff test. The data in this example are assumed for illustration.

Hall plot of the injection history050100150200250300350010002000300040005000Cumulative injection W, thousand m³Σ(pw − p̄)Δt, MPa·d1–45–8: plugging9–12: after treatment13–15: fractureslope of months 1–4

A chart: the cumulative injection from 0 to 350 thousand cubic metres on the horizontal axis, and the cumulative sum from 0 to 5000 megapascal-days on the vertical axis. Fifteen points lie on a broken line of four segments. The first reaches 72 thousand cubic metres and 1200. The second, steeper, reaches 134 thousand and 2400. The third, gentler, reaches 211 thousand and 3480. The fourth, gentler still, reaches 315 thousand and 4755. A dashed straight line continues the slope of the first segment: the points of the second segment rise above it, and the last points go below it. The segments are labelled: plugging, after the treatment, fracture.

CalculatedThe Hall plot of the injection history in the table: the points are the ends of the months, and the dashed line continues the slope of months 1–4. The slope grows with plugging (months 5–8, the points go above the dashed line), falls after the treatment (9–12) and falls still more with injection through a fracture (13–15).

Terms and symbols

Pressure maintenance system
Injection of water to keep up the reservoir pressure, and the whole system of facilities that does it.
Water injection pump station
A pump station (often packaged, that is, assembled from ready-made blocks) that delivers water under pressure to a group of injection wells.
Sectional multistage centrifugal pump
A pump with many impellers on one shaft. In Russian practice its type name, such as CNS 180-1900, gives the delivery in m³/h (180) and the head in metres (1900).
Water distribution block
A block with a flowmeter and a flow regulator for each well. It distributes the water among the wells.
Water compatibility
The ability of a water to mix with another water and to contact the rock without precipitates, swelling or movement of clays.
Deaeration
Removal of oxygen from water by lowering its partial pressure, by vacuum or by gas stripping.
Oxygen scavenger
A chemical that binds the oxygen left after deaeration, for example sodium bisulfite.
Injectivity index II
The injection rate per unit of excess of the bottomhole pressure over the reservoir pressure, m³/(d·MPa).
Fracture propagation pressure
The bottomhole pressure above which the reservoir takes water through a growing fracture. It is found with a step-rate test.
Hall plot
The cumulative sum of (pw−pˉ)Δt(p_w - \bar p)\Delta t against the cumulative injection. The slope equals 1/I1/I.

Common mistakes and misconceptions

Wrong

“Both waters are fit for injection separately, so they can be mixed.”

In fact

Water with barium and water with sulfate are each clean on their own, but together they give barite in the pipes and wells, tens of tonnes a year in the example of the lesson. We check compatibility for all mixing ratios.

Wrong

“The wellhead pressure limit is the fracture pressure minus the weight of the water column.”

In fact

This is true only without friction. At a high rate the friction in the tubing is megapascals, and such a limit underestimates the allowed rate. A limit found at a high rate is dangerous at a low rate. What we limit is the bottomhole pressure.

Wrong

“An oxygen scavenger is more reliable than a deaerator, so let us just add more of it.”

In fact

Full chemical treatment of sea water would take hundreds of tonnes of chemical a year, and the chemical also adds sulfate. The scavenger cleans up the remainder after mechanical deaeration.

Wrong

“The injection pressure has grown, so the well is getting plugged.”

In fact

The pressure may have been raised for the sake of the rate, or the reservoir pressure may have risen. Plugging is shown by a fall of the injectivity, that is, a growth of the slope of the Hall plot.

Wrong

“The slope of the Hall plot has fallen, so the treatment worked.”

In fact

The slope also falls when a fracture opens. If the bottomhole pressure stays at the fracture opening pressure when the rate grows, the water is going through a fracture.

Connections to other topics

Check yourself

  1. 1

    Sea water is going to be injected into a reservoir with barium in the formation water. Which of the following reduces the risk of sulfate scale first of all?

    1. A.Removal of sulfates from the sea water by membranes
    2. B.Heating the water
    3. C.Chlorination
    4. D.Deaeration of the water
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    Correct answer: A. Removal of sulfates from the sea water by membranes

    Barite forms from the barium of the formation water and the sulfate of the injected water. Deaeration and chlorination fight corrosion and bacteria, and heating has little effect on the solubility of barite. Removing the sulfate means removing one of the two ions. Other ways are another source of water, or inhibitors at moderate supersaturation.

  2. 2

    An injection well 2000 m deep takes 500 m³/d at a wellhead pressure of 6.0 MPa. The water density is 1050 kg/m³, the friction in the tubing is 1.5 MPa and the reservoir pressure is 20 MPa. Find the bottomhole pressure and the injectivity index.

    Show the answer

    The water column is 1050⋅9.81⋅2000=20.61050\cdot 9.81\cdot 2000 = 20.6 MPa. The bottomhole pressure is 6.0+20.6−1.5=25.16.0 + 20.6 - 1.5 = 25.1 MPa, the excess over the reservoir pressure is 5.1 MPa, and the injectivity is 500/5.1≈98500/5.1 \approx 98 m³/(d·MPa). If friction is forgotten, the injectivity would come out as 500/6.6≈76500/6.6 \approx 76, almost a quarter less.

  3. 3

    The slope of the Hall plot over the last three months has grown by 30%, and the reservoir pressure in the injection area, according to a test, has not changed. What does this mean and what should be done?

    1. A.The injectivity has fallen by about a quarter: the near-wellbore zone is getting plugged, so check the water and treat the well
    2. B.A fracture has opened: lower the pressure
    3. C.Nothing: the slope of the Hall plot is not linked with injectivity
    4. D.The injectivity has grown by 30%: the injection can be increased
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    Correct answer: A. The injectivity has fallen by about a quarter: the near-wellbore zone is getting plugged, so check the water and treat the well

    The slope equals 1/I1/I. A growth of 30% means that the injectivity has fallen to 1/1.3≈0.771/1.3 \approx 0.77 of the former value, almost a quarter. With an unchanged reservoir pressure the cause is plugging of the near-wellbore zone. The water quality is checked (suspended solids, oil, iron, bacteria), the diagnosis is confirmed with a falloff test, and a treatment is planned.

  4. 4

    Why is it not enough to remove oxygen from water by simply pumping the air over it down to 10 kPa (abs.), if the water must end up with 20 ppb of oxygen and water saturated with air holds 9 mg/L?

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    By Henry's law the partial pressure of oxygen that is needed is 21.2⋅0.020/9≈0.04721.2\cdot 0.020/9 \approx 0.047 kPa. If there is air over the water at 10 kPa, the oxygen in it is 0.21⋅10=2.10.21\cdot 10 = 2.1 kPa, 45 times more. Over the water there must be almost pure water vapour or an oxygen-free gas: either a deeper vacuum (the water then boils, and the vapour pushes out the air) or stripping with nitrogen, and a scavenger for the remainder.

  5. 5

    A pump station serves four wells. One of them, with low injectivity, needs 5 MPa more than the others. Which solutions will reduce the energy losses?

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    The pumps keep the pressure needed by the “tightest” well, the others are throttled, and the power q Δp/86.4q\,\Delta p/86.4 kW goes into the chokes. What helps: stimulating the “tight” well (acid, hydraulic fracturing) so that the common pressure is enough for it; a separate pump at its wellhead; splitting the wells into pressure levels; and variable speed control of the pumps instead of throttling.

  6. 6

    What does the Water Code of Kazakhstan say about the injection into the subsoil of formation water produced with oil?

    1. A.It needs only a notification
    2. B.It is allowed only at sea
    3. C.It is prohibited
    4. D.The condition of having environmental permits and a permit for special water use, set for the discharge and injection of such waters, does not apply to injection for pressure maintenance
    Show the answer

    Correct answer: D. The condition of having environmental permits and a permit for special water use, set for the discharge and injection of such waters, does not apply to injection for pressure maintenance

    Under paragraph 4 of Article 123 of the Water Code, the discharge of underground water taken incidentally in subsoil use, and its injection into the subsoil, are allowed only with environmental permits and permits for special water use, except for the injection for pressure maintenance of formation water produced with hydrocarbons. Injection into disposal horizons (layers used only to get rid of water) does not fall under the exception. The other requirements for the field remain in force: the project and the environmental permit for the facility.

Updated: 19 October 2026