general governing equation for steady-state, heterogeneous, anisotropic conditions 2d laplace eqn....
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Wz
hK
zy
hK
yx
hK
xzyx
)()()(
General governing equationfor steady-state, heterogeneous, anisotropic conditions
02
2
2
2
z
h
x
h2D Laplace Eqn.
--Homogeneous and isotropic aquifer without a sink/source term.--2D flow in a profile; (Unconfined aquifer with a water table boundary condition; recharge occurs as a result of the boundary condition.)
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Mathematical Model of the Toth Problem
02
2
2
2
z
h
x
h0
x
h0
x
h
0z
h
h = c x + zo
Unconfined aquifer
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b = 1 m
x
z
z
x b
02
2
2
2
z
h
x
h
Aquiferb
Tothproblem
x
z
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02
2
2
2
y
h
x
h
2D horizontal flow in an aquifer with constant thickness, b.
Aquiferb
x
y
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Figure from Hornberger et al. 1998
b unconfined aquiferb is not constant
confined aquifer
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2D horizontal flow in an aquifer with constant thickness, b.
Aquiferb
x
y
with recharge
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Wz
hK
zy
hK
yx
hK
xzyx
)()()(
with a source/sink term
T
R
y
h
x
h
2
2
2
2Poisson Equation
2D horizontal flow; homogeneous and isotropic aquiferwith constant aquifer thickness, b, so that T=Kb.
RbWz
hK
zy
hbK
yx
hbK
xzyx
)()()(
2D horizontal flow
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Map of Long Island, N.Y.
South Fork
Charles Edward Jacob (1914-1970)Consultant to the Town of Southampton, NY
December 1968
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bocean ocean
groundwater divide
C.E. Jacob’s Conceptual Model of theSouth Fork of Long Island
R
x = 0 x = Lx = - L
We can simulate this system assuming horizontal flow in a “confined” aquifer if we assume that T= Kb.
h datum
water table
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1D approximation used by C.E. Jacob
T
R
dx
hd
2
2
h(L) = 0
0dx
dh at x =0
ocean ocean
R
x = 0 x = Lx = - L
Governing Eqn.Boundary Conditions
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h(x) = R (L2 – x2) / 2T
Analytical solution for 1D “confined” version of the problem
C.E. Jacob’s Model
T
R
dx
hd
2
2
h(L) = 0
0dx
dh at x =0
Governing Eqn.
Boundary conditions
R = (2 T) h(x) / ( L2 – x2)
Forward solution
Inverse solution for R
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Rearrange eqn to solve for T,given value for R and h(0) = 20 ft.
Inverse solution for T
L
R = (2 T) h(x) / ( L2 – x2)
Inverse solution for R
Solve for R with h(x) = h(0) = 20 ft.
Observation wellon the groundwaterdivide
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x
y
ocean
ocean
T= 10,000 ft2/dayL = 12,000 ft
2L
L
T
R
y
h
x
h
2
2
2
2
Island Recharge Problem
oceanwell
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• Head measured in an observation well is known as a head target.
Targets used in Model Calibration
• The simulated head at the node representing the observation well is compared with the measured head.
• During model calibration, parameter values (e.g., R and T) are adjusted until the simulated head matches the observed value.
• Model calibration solves the inverse problem.
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x
y
ocean
oceanSolve the forward problem:
GivenR= 0.00305 ft/dT= 10,000 ft2/day
Solve for h at each nodal point
2L
L = 12,000 ft
T
R
y
h
x
h
2
2
2
2
Island Recharge Problem
ocean
well
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T
R
y
h
x
h
2
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2
Gauss-Seidel Iteration Formula for 2D Poisson Equation with x = y = a
Write the finite difference approximation:
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Island Recharge Problem4 X 7 Grid
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Water Balance
IN = Out
IN = R x AREA
Out = outflow to the ocean
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Top 4 rows
Red dots represent specified head cells, which are treated as inactive nodes.
Black dots are active nodes. (Note that the nodes along the groundwater divides are active nodes.)
Head at a node is theaverage head in the areasurrounding the node.
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Top 4 rows
IN =R x Area = R (L-x/2) (2L - y/2) 2L
L
Also: IN = R (2.5)(5.5)(a2)
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Top 4 rows
x/2 x x
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x/2Top 4 rows
OUT = Qy + Qx
Qy = K (x b) (h/y)Note: x = y Qy = T h
Qx = K (y b)(h/x)
or Qx = T h
Qx
Qy
y
Qy = (Th) /2
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Welly/2
Bottom 4 rows
Qx = (T h)/2
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Island Recharge Problem4 X 7 Grid
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Water Budget Error