Lecture 14
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Equations of Ground-water Flow
Fetter 5.6
Let us put Darcys law in terms of Force and Potential
| Remember |
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| Since, |
Express Darcys Law in terms of potential
One dimensional form of Darcys Law
If flow though an open pipe Channel
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Q = VA | |
| Apply to Darcys Law | |||
| Specific Discharge (Darcy Flux) | |||
| This is an Apparent velocity. | |||
| What is not accounted for in a geologic unit? | |||
Area is actually the porosity
| Where n |
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| v |
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This is the seepage velocity or Average linear flow velocity.
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| For instance |
| 100 | 90 | 80 | ||
| K = 0.2ft/d | ||||
| n |
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1000 feet between 100 and 80 feet contours |
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Laplace Equation
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| Assume | |||||
| (1) Isotropic | |||||
| (2) Homogeneous | |||||
| (3) Fluid moving in one direction | |||||
| Remember | |||||
| Law of Mass Conservation | |||||
| -No net change in mass in a small volume of aquifer. | |||||
Physics
Law of conservation of energy -
| First Law of Thermodynamics | ||
| Energy can be neither lost nor gained, it can only change forms. | ||
| Second Law | ||
| "there is no such thing as a free lunch" | ||
All used to derive main equations ground-water flow
Control Volume
| q - flow per unit cross
sectional area |
|
| Pwqx - flow perpendicular to x axis | |
| Therefore, mass flux into control volume = qxr wdydz along x axis | |
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Total Mass Accumulation
Terms Along 3 axes |
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Volume water in control = ndxdydz
change in mass of water |
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Changes in Aquifer and water compress change in head.
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Know from Darcys Law
Substitute for q in

Get

General equation for flow in three dimensions for isotropic homogeneous, confined aquifer.
| Simplify ® two dimensional, no vertical flow | ||
| know |
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| T = Kb | ||
| then |
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Steady-state
| no head change with time | ||
| i.e. water table position does not change with respect to time. | ||
Laplace equation