Transcript Lesson 6

Introduction to MT3DMS
All equations & illustrations taken
from the MT3DMS manual
Refer to the document on
the course homepage entitled
“MT3DMS Solution Methods and Parameter Options”
(Look under the MT3DMS tab on the homepage)
General form of the ADE:
Expands to 9 terms
Expands to 3 terms
(See eqn. 3.48 in Z&B)
9 Dispersion
Coefficients
This schematic assumes that
MODFLOW
MT3DMS
MT3DMS time steps are selected by the code considering
stability constraints, if any, and Courant numbers.
Dispersion, sink/source, chemical reactions
Advection
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MT3DMS Solution Options
1
2
3
4
x
j-1
j-1/2
j
j+1
j+1/2
Upstream weighting
Central differences
MT3DMS Solution Options
Explicit Approximation
Courant Number
Stability constraints
for explicit solutions
Courant Number
v t
Cr 
x
6 Courant Numbers
One for each face of
the cell block
Cr < 1
MT3DMS Solution Options
Use GCG Solver
Use GCG Solver
Use GCG Solver
Implicit Approximation
for advection term
MT3DMS Solution Options
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TVD ULTIMATE METHOD
a higher order FD method
Conventional FD methods
use 3 nodes in the FD
approximation. The TVD
method uses 4 nodes with
upstream weighting. This
essentially eliminates
numerical dispersion.
Steps in the TVD Method
Check for
oscillation
errors
Correction
for oscillation
errors
oscillation
TVD ULTIMATE METHOD
In one dimension
Compare with an equation for a
lower order explicit approximation
c j n 1  
vt
(c j n  c j 1n )  c j n
x
MT3DMS Solution Options
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Eulerian vs Lagrangian Methods
• Eulerian: fixed coordinate system with mass flux
through an REV
• Lagrangian: moving particles; each particle carries mass.
The Random Walk method is a Lagrangian method.
• Mixed Eulerian-Lagrangian methods use particles to solve
the advection portion of the ADE and an Eulerian method
to solve the rest of the equation.
Method of Characteristics
(MOC)
2
where  is a weighting factor to weight
concentration between time level n and
an intermediate time level n*, normally
 = 0.5
3
1
n 1
n 1
Step 1 is a Lagrangian method;
 Cm  Cm
4 Cm
Step 3 is a Eulerian method.
Also update concentration of each particle. For example,
n 1
n
n 1
C

C


C
for particles in cell m:
p
p
m
n*
• MOC uses multiple particles per cell.
• MMOC uses one particle per cell.
• HMOC uses multiple particles in high concentration regions
and one particle per cell elsewhere.
Dynamic Particle Allocation
Breakthrough curve for example problem
in the MT3DMS manual
Compare with Fig. 7.26 in Z&B
1.20
Central FD
TVD
1.00
HMOC
TVD
Upstream weighting
Central FD
Concentration
0.80
Upstream FD
0.60
0.40
0.20
0.00
0.00
0.20
0.40
0.60
Time (years)
0.80
1.00
1.20
MT3DMS Solution Options
PS#2
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3
4
2