The Alternative Time Function Model
Considering the left hand side of the material balance equation
Where
No Water Drive, a Known Gas Cap
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The Alternative Time Function Model
Considering the left hand side of the material balance equation
Where
No Water Drive, a Known Gas Cap
Introduction
The material balance equation is a complex equation for calculating the original oil
in place, cumulative water influx and the original size of the gas cap as compared to
the oil zone size. This complexity prompted Havlena and Odeh to express the MBE
in a straight line form. This involves rearranging the MBE into a linear equation. The
straight lines method requires the plotting of a variable group against another
variable group selected, depending on the reservoir drive mechanism and if linear
relationship does not exist, then this deviation suggests that reservoir is not
performing as anticipated and other mechanisms are involved, which were not
accounted for; but once linearity has been achieved, based on matching pressure
and production data, then a mathematical model has been achieved. This technique
of trying to match historic pressure and production rate is referred to as history
matching. Thus, the application of the model to the future enables predictions of the
future reservoir performance. To successfully develop this chapter, several textbooks
and materials such Craft & Hawkins (1991), Dake (1994), Donnez (2010), Havlena
& Odeh AS (1964), Numbere (1998), Pletcher (2002) and Steffensen (1992) were
consulted.
The straight line method was first recognized by Van Everdigen et al. (2013) but
with some reasons, it was never exploited. The straight line method considered the
underground recoverable F, gas cap expansion function Eg, dissolved gas-oil expansion function Eo, connate water and rock contraction function Ef,w as the variable for
plotting by considering the cumulative production at each pressure.
Havlena and Odeh presented the material balance equation in a straight line form.
These are presented below:
In evaluating the performance of a reservoir, there is need to adequately identify the
type of reservoir in question based on the signature of pressure history or behaviour
and the production trend. Campbell and Dake plots are the vital diagnostic tools
employed to identify the reservoir type. The plots are established based on the
assumption of a volumetric reservoir, and deviation from this behaviour is used to
indicate the reservoir type.
For volumetric reservoirs whose production is mainly by oil and connate water/
rock expansion, the value of STOIIP, N can be calculated at every pressure where
production data is given. Rearranging the material balance equation as shown below.
expansions is created with a volumetric reservoir data, then the calculated values
of STOIIP, N on the horizontal axis should be constant at all pressure points. In
practice, this is often not the case either because there is water influx or because there
may be faulty pressure or production readings.
production. As production continues and the reservoir pressure decreased, the gas
expansion term increases with an increase in the gas formation volume factor. To
balance this, the withdrawal over oil/water/formation expansion term must also
continue to increase. Thus, in the case of gas cap drive, the Dake plot will show a
continual increasing trend.
Similarly, if water drive is present, the withdrawal over oil/water/formationexpansion term must increase to balance the water influx. With a very strong aquifer,
the water influx may continue to increase with time, while a limited or small aquifer
may have an initial increase in water influx to the extent that it eventually decreases.
The Campbell plot is very similar to Dake’s diagnostic tool, with an exception
that it incorporates a gas cap if required. In the Campbell plot, the withdrawal is
plotted against withdrawal over total expansion, while the water influx term is
neglected. If there is no water influx, the data will plot as a horizontal line. If there
is water influx into the reservoir, the withdrawal over total expansion term will
increase proportionally to the water influx over total expansion. The Campbell plot
can be more sensitive to the strength of the aquifer. In this version of the material
balance, using only ET neglects the water and formation compressibility (compaction) term. The Campbell plot is shown below.
According to Tarek (2010), the linear form of MBE is presented in six scenarios to
determine either m, N, G or We as follow:
• Undersaturated reservoir without water influx
• Undersaturated reservoir with water influx
• Saturated reservoir without water drive
• Saturated reservoir with water drive
• Gas cap drive reservoir
• Combination drive reservoir
Scenario 1: Undersaturated Reservoir Without Water
Influx
Applying the above assumption, the equation reduces to
Scenario 2: Undersaturated Reservoir with Water InfluxApplying the above assumption, the equation reduces to
Scenario 3: Saturated Reservoir Without Water Influx
Applying the above assumption, the equation reduces to
Scenario 4: Saturated Reservoir with Water Influx
Applying the above assumption, the equation reduces to
Scenario 5: Gas Cap Drive Reservoir
• Finding the STOIIP, N when the gas cap size, m is known
• Finding the gas cap size, m the STOIIP, N and the GIIP, G
Finding the STOIIP, N when the gas cap size, m is known
Scenario 6: Combination Drive ReservoirLinear Form of Gas Material Balance Equation
Havlena and Odeh also expressed the material balance equation in terms of gas
production, fluid expansion and water influx as
One of the advantages of Carter-Tracy’s model over Van Everdingen-Hurst model is
that; it does not require superposition and can be easily combined with MBE. Thus,
Carter-Tracy’s model is combined with undersaturated MBE as follows:
Oil Saturation Adjustment Due to Combination Drive
For the case of combination drive, both water and gas invasion zone is incorporated
in the saturation equation given as:
Determination of Present GOC and OWC from
Material Balance Equation
Step 1: Determine the bulk volume of the reservoir rock at each depth interval
Step 2: Make a plot of depth versus the bulk volume
Step 3: Calculate the cumulative water influx from the general material balance
equation (We)
Step 4: Calculate the volume of oil displaced by water (Net water influx into the
reservoir) (OW ¼ We Wp)
Step 5: Calculate the reservoir volume liberated gas (GL)
GL¼ NRsi N Np
Rs
Bg
Step 6: Calculate the expansion of the primary gas cap (Ge)
Ge ¼ mNBoi
Bg
Bgi
1
Step 7: Calculate the gas drive (GD)
GD ¼ GL þ Ge
Step 8: Calculate the produced excess gas (Gpe)
Gpe ¼ Np Rp Rs
Bg
Step 9: Calculate the volume of oil displaced by the gas (Og)
Undersaturated Reservoir with Water Drive
Saturated Water Drive Reservoir
Oil Saturation Adjustment Due to Water Influx
Depletion Drive Reservoir
5.8.1.1 For Undersaturated Reservoir (P > Pb) with No Water Influx
That is, above the bubble point; the assumptions made are:
for Undersaturated Reservoir
From the expression of the isothermal compressibility in terms of effective compressibility, we can express it in terms of
total compressibility, Ct
Saturated Reservoir (P < Pb) Without Water Influx
Calculation of Oil Saturation
As hydrocarbon is produced from the porous rock, water moves to replace the
corresponding space or void left by the produced hydrocarbon because nature avoids
vacuum. In some cases, the effects of the reservoir drive mechanisms need to be
accounted for; which are presented subsequently in this chapter. Mathematically, oil
saturation is given as:
Gas Drive Reservoir
Water drive is the mechanism wherein the displacement of the oil is accomplished by
the net encroachment of water into the oil zone from an underlined water body called
aquifer (Fig. 5.10a).
Production of oil or gas will often change the water saturation which in turn
affects the oil and gas saturation, but the amount of change varies with the reservoir
drive mechanism. In an aquifer driven reservoir on an efficient water flood, as the oil
is produced to the surface facilities via the production tubing, the water saturation
increases accordingly to fill the space previously occupied by the withdrawn oil
(Fig. 5.10b).
This mechanism is represented mathematically as
Water Drive Index ¼ Net water influx
Hydrocarbon Voidage
on Reservoir Engineering)
• Pressure
– Pressure is maintained (remains high) when water influx is active.
Pressure declines slowly at first but then stabilizes due to increasing influx
with increasing pressure differential, but not when water influx is moderate.
• Oil Rate
– Rate remains constant or gradually declines prior to water breakthrough
– Rate decreases as water rate increases
• Producing GOR
– GOR remains constant as long as P > PBP
– Gradually increases if P is below the saturation pressure
• Water Production
– Dry oil until water breakthrough
– Increasing water production to an appreciable amount from the flank wells; a
sharp increase due to water coning in individual wells.
• Ultimate Recovery
– The expected oil range is 35–75%
Rock Compressibility and Connate Water Expansion
Drive
As the reservoir pressure declines, the rock and fluid expand due to the expansion of
the individual rock grains and formation compaction (individual compressibility).
The compressibility of oil, rock and water is generally relatively small which makes
the pressures in the undersaturated oil reservoirs to drop rapidly to the bubble point if
there is no aquifer support. Sometimes, this drive mechanism is not considered or it
is neglected when performing material balance calculation, especially for saturated
reservoirs.
This mechanism is represented mathematically as:
formation Drive Index ¼ rock and connate water expansion
Hydrocarbon Voidage
Gravity Drainage Reservoirs (Prof Onyekonwu MO,
Lecture Note on Reservoir Engineering)
• The mechanism of gravity drainage is operative in an oil reservoir as a result of
difference in densities of the reservoir fluids.
• Gas coming out of solution moves updip to the crestal areas while oil moves
downdip to the wells located low on the structure (Fig. 5.11).
• Reservoir must have:
– High Dip
– High Permeability
– High Kv/Kh ratio
– Homogeneity
– Low Oil Viscosity
• Production Characteristics:
– Formation of a secondary gas cap
– Low GOR from structurally low wells
– Increasing GOR from high structure wells
– Rapid pressure decline to near dead conditions (stripper wells)
– Little or no water production
• While rates are low, RE will be high (70–80% of the initial oil in place)
eventually.
• Gravity drainage is most significant in fractured tight
Combination Drive Reservoirs
Most oil reservoirs produce under the influence of two or more reservoir drive
mechanisms, referred to collectively as a combination drive. A common example
is an oil reservoir with an initial gas cap and an active water drive as shown in the
Fig. 5.12.
5.7.7.1 Production Trends
The production trends of a combination drive reservoir reflect the characteristics of
the dominant drive mechanism. A reservoir with a small initial gas cap and a weak
water drive will behave in a way similar to a solution gas drive reservoir, with rapidly
decreasing reservoir pressure and rising GORs. Likewise, a reservoir with a large gas
cap and a strong water drive may show very little decline in reservoir pressure while
exhibiting steadily increasing GORs and WORs. Evaluation of these production
trends is the primary method a reservoir engineer has for determining the drive
mechanisms that are active in a reservoir.
Recovery
The ultimate recovery obtained from a combination drive reservoir is a function of
the drive mechanisms active in the reservoir. The recovery may be high or low
depending on whether displacement or depletion drive mechanisms dominate. Water
drive and gas cap expansion are both displacement type drive mechanisms and have
relatively high recoveries. Solution gas drive is a depletion type drive and is
relatively inefficient.
Recovery from a combination drive reservoir can often be improved by minimizing the effect of depletion drive mechanisms by substituting or augmenting more
efficient ones through production rate management or fluid injection. To do this, the
drive mechanisms active in a reservoir must be identified early in its life
5.7.7.3 Characteristics of Combination Drive Reservoirs (Prof
Onyekonwu MO, Lecture Note on Reservoir Engineering)
• Gradually increasing water-cut in structurally low wells
• Pressure decline may be rapid if no strong water influx and no gas cap expansion.
• Continuously increasing GOR in structurally high wells if the gas cap is
expanding
• Recovery > depletion Drive but may be less than in water drive or gas-cap drive.
• When an oil reservoir is associated with a gas cap above and an aquifer below, all
drive mechanisms may be operative.
• Development strategy and well rate control are very important in the economic
recovery process.
A. If oil production rate is faster than the encroachment rates of gas cap and
water advance, pressure depletion occurs in the oil zone.
B. If oil production rate is controlled to equal voidage, it is better to have water
displace oil than gas displacing oil.
– Danger: Oil migration into gas cap due to shrinkage of gas cap volume;
some oil will be left trapped as residual.
• RE is usually greater than recovery from depletion drive but less than water drive
or gas-cap drive. The expected recovery is between 25 and 40% OOIP
The production of hydrocarbon from a reservoir into the wellbore involves several
stages of recovery. The available drive mechanisms determine the performance of
the hydrocarbon reservoir. When the hydrocarbon fluids are produced by the natural
energy of the reservoir, it is termed primary recovery; which is further classified
based on the dominant energy responsible for primary production. There are six
primary drive mechanisms, they are:
• Solution Gas (Depletion) Drive
• Water Drive
• Gas Cap Expansion (segregation) Drive
• Rock Compressibility and Connate Water Expansion Drive
• Gravity Drainage
• Combination Drive
5.7.1 Basic Data Required to Determine Reservoir Drive
Mechanism
• Reservoir pressure and rate of decline of reservoir pressure over a period of time.
• The character of the reservoir fluids.
• The production rate.
• Gas-Oil ratio.
• Water-oil ratio.
• The cumulative production of oil, gas and water.
5.7.2 Solution Gas (Depletion) Drive
A solution gas or depletion drive reservoir is a recovery mechanism where the gas
liberating out of the solution (oil) provides the major source of energy. We simply
define it as the oil recovery mechanism that occurs when the original quantity of oil
plus all its original dissolved gas expansion as a result of fluid production from its
reservoir rock (Fig. 5.7).
This drive mechanism is represented mathematically as:
Production Characteristics (Prof Onyekonwu MO, Lecture Note
on Reservoir Engineering)
• Pressure
– declines rapidly and steadily
– decline rate is dependent on production rate
• Oil Rate
– declines rapidly at first as oil mobility decreases
– steady decline thereafter
• Producing GOR
– Increases rapidly as free gas saturation increases.
– Thereafter, decreases rapidly as the remaining oil contains less solution gas.
• Water Production
– Mostly negligible as depletion type reservoirs are volumetric (closed) systems.
• Ultimate Oil Recovery
– It may vary from less than 5% to about 30%. Thus, according to Cole (1969)
these characteristics can be use to identify a depletion drive reservoir.
5.7.3 Gas Cap Expansion (Segregation) Drive
Segregation drive (gas-cap drive) is the mechanism wherein the displacement of oil
from the formation is accomplished by the expansion of the original free gas cap as
shown in Fig. 5.8.
The following are some of the points to note in a gas cap expansion drive
mechanism:
• A gas cap, existing above an oil zone in the structurally higher parts of a reservoir,
provides a major source of energy. The pressure at the original GOC (Fig. 5.8) is
the bubble point pressure since the underlain oil is saturated.
• As pressure declines in the oil column, two things happen:
– Some dissolved gas comes out of oil
– Gas cap expands to replace the voidage
Formation of free gas in the oil column should be minimized as much as possible.
This is achieved if:
– Gas is re-injected in the gas cap, and
– Gas is allowed to migrate upstructure (Gravitational Segregation) (Fig. 5.9).
Figure 5.6 shows an initial condition of a reservoir with original gas cap and the
setting when the reservoir pressure as dropped due to fluid expansion. The material
balance equation uses the principle of conservation of mass. It states that the total
amount of hydrocarbon withdrawn is equal to the sum of the expansion of the oil
plus the original dissolved gas plus the primary gas plus the expansion of the connate
water & decrease in pore volume plus the amount of water the encroached into the
reservoir.
From the diagram, we have that
The derivation of the general material balance is presented below
Quantity of Oil Initially in the Reservoir
NBoi
5.6.2.2 Quantity of Oil Remaining in the Reservoir
The Free/Liberated Gas in the Reservoir
Expansion of Oil Zone
In the oil zone, will have the original volume of oil plus the original dissolved gas in
the oil
Expansion of Connate Water and Decrease in Pore Volume
The rock compressibility is expressed as
Total Underground Withdrawal
The total underground withdrawal (TUW) due to the pressure drop is the sum of the
oil + gas + water production. Mathematically, it is
Quantity of Injection Gas and Water