Motivation
The most accurate way to simulate Aquifer Expansion (or shrinkage) is full-field 3D Dynamic Flow Model where Aquifer Expansion is treated as one of the fluid phases and accounts of geological heterogeneities, gas fluid properties, relperm properties and heat exchange with surrounding rocks. Unfortunately, in many practical cases the detailed information on the aquifer is not available which does not allow a proper modelling of aquifer expansion using a geological framework. Besides many practical applications require only knowledge of cumulative water influx from aquifer under pressure depletion. This allows building an Aquifer Drive Models using analytical methods.
The Carter–Tracy (1960) model is a finite aquifer influx analytical model widely used in reservoir engineering to account for water influx in material-balance calculations.
It approximates the van Everdingen–Hurst (1949) solution fore faster computation.
Physical Model
| Radial Composite Reservoir | |
| Transient flow | |
| Computational approximation to van Everdingen-Hurst (VEH) | |
| Fig. 1. Carter-Tracy aquifer drive schematic |
Inputs
t | elapsed time | ||
\mu | aquifer viscosity | h | aquifer thickness |
k | aquifer permeability | r_e | inner radius (reservoir–aquifer interface) |
\phi | aquifer porosity | r_a | outer radius of aquifer |
c_\phi | aquifer pore compressibility | p_i | initial formation pressure |
c_w | aquifer water compressibility | p(t) | field-average formation pressure at time moment t |
Outputs
Q^{\downarrow}_{AQ}(t) | Cumulative subsurface water influx from aquifer at time t, also denoted as W_e(t) |
q_{AQ}^{\downarrow}(t)=\frac{Q^{\downarrow}_{AQ}(t)}{dt} |
Midputs
A_e = \pi \, r_e^2 | |
c_t=c_\phi +c_w | aquifer total compressibility (fluid + rock) |
B = \frac{\theta}{\pi} \cdot A_e \cdot h \cdot \phi \cdot c_t | |
\chi = \frac{ k }{\phi \, \mu \, c_t } | aquifer diffusivity |
t_D = \frac{\pi \, \chi \, t}{A_e} = \frac{ k \, t}{\phi \, \mu \, c_t \, r_e^2} | dimensionless time |
r_D=r_a/r_e | dimensionless radius of aquifer |
F(t_D, r_D) | dimensionless water influx function (solution of Carter–Tracy PDE) |
Mathematical Model
| ||||
|
where
J_1 | first-order Bessel function |
\alpha_n | roots of the zero-order Bessel function J_0(\alpha_n \, r_D)=0 |
Computational Model
| z=\frac{\sqrt{t_D}}{100} |
where
| a0 = 9.61160410×10−5 a1 = 1.10150583×102 a2 = 3.69104053×103 a3 = 1.12033686×104 a4 = −3.14537222×103 a5 = 1.82023227×103 a6 = −1.36968356×103 a7 = −6.36974453×101 a8 = 8.99546667×102 |
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See Also
Petroleum Industry / Upstream / Subsurface E&P Disciplines / Field Study & Modelling / Aquifer Drive / Aquifer Drive Models
[ Material Balance Analysis (MatBal) / Material Balance Pressure @model ]
Reference
2. Tarek Ahmed, Paul McKinney, Advanced Reservoir Engineering (eBook ISBN: 9780080498836)
