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Well Tests to Characterize Idealized Lateral Heterogeneities by Vasi Passinos K 1,S 1 K 2,S 2
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Faults Steeply Dipping Beds
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Igneous Rocks Facies Change Reef Marine Clay Batholith Country rock Dike Channel sand Floodplain deposits
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Confined Aquifer Unconfined Aquifer
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Conceptual Models LocalNeighboring T1 S1T1 S1 T 2 S 2 LL 2-Domain Model3-Domain Model Matrix Strip T m S m LLw T s S s =S m
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Analysis Governing Equation Initial Condition when Boundary Conditions
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Analysis – 2-Domain Conditions at the contact L 1 2
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Analysis – 3-Domain Conditions at the contact m m s Lw
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Method – Analytical Transient analytical solution using Method of Images (Fenske, 1984)
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Methods – Numerical Transient numerical model using MODFLOW 2-Domain – T r and S r were varied 3-Domain - T r and w of the strip were varied. Grid optimized for small mass balance errors The properties of the model were selected so that the drawdown and time from the numerical model were dimensionless
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Dimensionless Time Drawdowns were evaluated at three dimensionless times to illustrate effects during development of drawdown fields. Dimensionless time used for type curves Dimensionless time used in drawdown fields
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2-Domain Model T Contrast T r =10 T r = 1 T r =0.1 t dLA t dLB t dLC
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2-Domain Model S Contrast S r = 10 S r = 1 S r = 0.1 t dLA t dLB t dLC
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3-Domain Model T Contrast T r = 10 T r = 1 T r = 0.1 t dLB t dLC t dLD
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2-Domain T Contrast – 0.125L
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2-Domain T Contrast – 0.5L
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2-Domain S Contrast – 0.125L
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2-Domain S Contrast – 0.5L
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Graphical Evaluation – 2-Domain Estimate Aquifer Properties t o = 0.029 S = 0.017 s = 2.3 T = 1 t o = 0.42 S = 0.35 s = 4.1 T = 0.55
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Graphical Evaluation – 2-Domain Estimate Aquifer Properties t o = 2.7 S = 0.136 s = 4.1 T = 0.55
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T E =1 S E =0.0179 T L =0.55 S L =0.25 T E =1 S E =0.0179 T L =0.55 S L =0.136 T L =0.55 S L =0.06 T L =0.55 S L =0.27 T L =0.55 S L =0.021 T L =0.55 S L =0.068 T L =0.55 S L =0.029 T L =0.55 S L =0.021 L LL
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Critical Region An early semi-log straight line can be determined by The second derivative was compared to plots with a variety of curves. An early SLSL could be identified by a second derivative of 0.2 or less from 0.3<t dL <2.5.
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Critical Region Observation points confined to a region that is within 0.3 to 0.5 of the distance between the pumping well and the linear discontinuity
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Distance to the Contact t c = 7.3 Streltsova, 1988
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3-Domain T Contrast - 0.125L
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3-Domain T Contrast - 0.5L
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Strip Transmissivness & Conductance Hydraulic properties of the strip depend on strip conductivity and width Strip K greater than matrix Strip K less than matrix
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Strip Transmissivness & Conductance
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Graphical Evaluation – 3-Domain Estimate Aquifer Properties t o = 0.09 S = 0.054 s = 2.3 T = 1 t o = 0.028 S = 0.017 s = 2.3 T = 1
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Determine Properties of Strip SLSL analysis on the first line will give T and S of the area near the well. Take the derivative of time and determine the maximum or minimum slope. Using equations from curve fitting determine T ssd or C d of the layer. Solve for T ss or C
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Non-Uniqueness s s Log (t) Dual Porosity Overlying Leaky Layer without storage Unconfined Aquifer w/delay yield from storage Overlying Leaky Layer with storage Streltsova, 1984 Streltsova, 1988 Streltsova, 1984 Neuman, 1975
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Field Example 500 feet Down Up Ridge stream N fault
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Field Case - Site Map N 500 feet BW-109 BW2 L B-4 Felsic Mafic
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Drawdown from Pumping Well
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Drawdown from Piezometers
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Using Semi-Log Straight- Line Analysis : Minimum slope using the derivative curve is 0.5 T ssd =34=K s w/K a L T ss = 24 ft 2 /min w = 10 to 20 ft Determining Hydraulic Properties L = 280 ft Distance to fault b = 21.5 ft screened thickness T m = 0.05 ft 2 /min S m = 2x10 -4 ??? T s = 26 to 52 ft 2 /min T s /T m = 500 to 1000
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Conclusions 2-Domain Model Using the Jacob method to analyze well tests: Piezometers r < 0.25L gives T, S of local region. Piezometers r > 0.25L gives average T of both regions. Piezometers r > 0.25L unable to predict S
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Conclusions – 2-Domain Piezometers in neighboring region also give average T of both regions. L can be determined from intersecting SLSLs using a piezometer within the critical region
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Conclusions 3-Domain Model Drawdown for low conductivity vertical layer controlled by conductance. C=K s /w Drawdown for high conductivity vertical layer controlled by strip transmissivness. T ss =K s *w Feasible to determine properties of a vertical layer from drawdown curves.
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Conclusions Analyzing piezometers individually is a poor approach to characterizing heterogeneities. Drawdown curves non-unique. Require geological assessment.
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Acknowledgments Funding –Geological Society of America –Brown Foundation –National Science Foundation Others…
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