Transient Water Balance Eqn. Inflow = Outflow + S Recharge Discharge
OUT – IN = x y z = - V/ t = change in storage Ss = V / (x y z h) V = Ss h (x y z) t
OUT – IN = General governing equation for transient, heterogeneous, and anisotropic conditions
div (K grad h) = Ss (h t) – W Law of Mass Balance + Darcy’s Law = Governing Equation for Groundwater Flow --------------------------------------------------------------- div q = - Ss (h t) +W (Law of Mass Balance) q = - K grad h (Darcy’s Law) div (K grad h) = Ss (h t) – W
2D profile 2D confined 2D unconfined Storage coefficient is either storativity (S) or specific yield (Sy). S = Ss b (& Tx = Kx b; Ty= Ky b) Ss is specific storage.
End Transient problems require multiple arrays of head values n+3 Time planes t n+2 t n+1 t Initial conditions
2D confined 1D, transient, homogeneous, isotropic, confined, no sink/source term
Reservoir Problem 1D, transient Confined Aquifer t > 0 1D, transient
(represents static steady state) BC: h (0, t) = 16 m; t > 0 h (L, t) = 11 m; t > 0 datum x L = 100 m t = 0 IC: h (x, 0) = 16 m; 0 ≤ x ≤ L (represents static steady state) Modeling “rule”: Initial conditions should represent a steady state configuration of heads.
At t = tss the system reaches a new steady state: datum x L = 100 m At t = tss the system reaches a new steady state: h(x) = ((h2 –h1)/ L) x + h1 [analytical solution: equation 4.12 (W&A)] BC: h(L) = h2 h(0) = h1 GE:
Governing Eqn. for transient Reservoir Problem 1D, transient, homogeneous, isotropic, confined, no sink/source term i-1,j i+1,j i,j i+1/2 i-1/2
Explicit Approximation
Explicit Solution Eqn. 4.11 (W&A) Everything on the RHS of the equation is known. Solve explicitly for ; no iteration is needed.
Explicit approximations are unstable unless small time steps are used. We can derive the stability criterion by writing the explicit approx. in a form that looks like the SOR iteration formula and setting the terms in the position occupied by equal to 1. For the 1D governing equation used in the reservoir problem, the stability criterion is: or
For the reservoir problem: T = 0.02 m2/min S = 0.002 x = 10 m
Explicit Solution Spreadsheet
t = 5 min
Transient Water Balance Eqn. Inflow = Outflow +Storage Storage = V2 – V1 Recharge t2 Discharge V2 > V1
Transient Water Balance Eqn. Inflow = Outflow +Storage Storage = V2 – V1 Recharge t1 Discharge t2 V2 < V1 Inflow -Storage = Outflow Inflow + abs(Storage) = Outflow
Water Balance- version 1 Storage = V(t2)- V(t1) IN > OUT then water going into storage and Storage is + OUT > IN then water is coming out of storage and Storage is – IN – OUT= Storage MODFLOW Convention: Water coming out of storage goes into the aquifer (IN column). Water going into storage comes out of the aquifer (OUT column). Total IN Total OUT Total IN = Total Out Flow in ABS(Flow out) ABS(Storage) Storage
Water Balance- version 2 Storage = V(t1)- V(t2) IN > OUT then water going into storage and Storage is - OUT > IN then water is coming out of storage and Storage is + IN - OUT = Storage Convention: Water coming out of storage goes into the aquifer (IN column). Water going into storage comes out of the aquifer (OUT column). Total IN(+) Total OUT(-) Flow in Storage Flow out Total IN = ABS(Total Out)
Reservoir Problem Water Balance IN OUT t > 0 Storage IN + change in storage = OUT (where here the change in storage term is intrinsically positive) + - Flow in Flow out Convention: Water coming out of storage goes into the aquifer (+ column). Storage Total IN = ABS(Total Out)
Units + - Flow in Flow out Storage L3/T (m3/min)
OUT – IN = x y z = - V/ t = change in storage Ss = V / (x y z h) V = Ss h (x y z) t
Storage Term for the Water Balance 3D problem: V = Ss h (x y z) t t V = S h (x y) where S = Ss b t 2D problem: In 1D Reservoir Problem, y is taken to be equal to 1.
Water Balance % Error = ABS(Total IN- Total Out) / Min(Total IN:Total Out)
Stablity criterion for explicit solution: For the reservoir problem: T = 0.02 m2/min S = 0.002 x = 10 m Judging by the water balance error, t = 5 min may be too large.