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Finite Difference Solutions to the ADE. Simplest form of the ADE Even Simpler form Plug Flow Plug Source Flow Equation.

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Presentation on theme: "Finite Difference Solutions to the ADE. Simplest form of the ADE Even Simpler form Plug Flow Plug Source Flow Equation."— Presentation transcript:

1 Finite Difference Solutions to the ADE

2 Simplest form of the ADE Even Simpler form Plug Flow Plug Source Flow Equation

3 Effect of Numerical Errors (overshoot) (MT3DMS manual)

4 (See Zheng & Bennett, p. 174-181) v j-1 jj+1 xx x Explicit approximation with upstream weighting

5 Explicit; Upstream weighting (See Zheng & Bennett, p. 174-181) v j-1 jj+1 xx x

6 Example from Zheng &Bennett v = 100 cm/h  l = 100 cm C1= 100 mg/l C2= 10 mg/l With no dispersion, breakthrough occurs at t = v/  l = 1 hour

7 v = 100 cm/hr  l = 100 cm C1= 100 mg/l C2= 10 mg/l  t = 0.1 hr Explicit approximation with upstream weighting

8 Implicit; central differences Implicit; upstream weighting Implicit Approximations

9

10 = Finite Element Method

11 Governing Equation for Ogata and Banks solution

12 j-1 jj+1 xx x j-1/2j+1/2

13 Governing Equation for Ogata and Banks solution Finite difference formula: explicit with upstream weighting, assuming v >0 Solve for c j n+1

14 Stability Constraints for the 1D Explicit Solution (Z&B, equations 7.15, 7.16, 7.36, 7.40) Courant Number Cr < 1 Stability Criterion Peclet Number Controls numerical dispersion & oscillation, see Fig.7.5

15 CoCo Boundary Conditions a “free mass outflow” boundary (Z&B, p. 285) Specified concentration boundary C b = C o C b = C j j j+1 j-1j j+1 j-1

16 Spreadsheet solution (on course homepage)

17 We want to write a general form of the finite difference equation allowing for either upstream weighting (v either + or –) or central differences.

18 j-1 jj+1 xx x j-1/2j+1/2

19 Upstream weighting: In general: See equations 7.11 and 7.17 in Zheng & Bennett


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