Lecture 19
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Ground-water Flow to Wells
Fetter 7.1-7.3-1
Wells used to extract ground water (or inject)
Cone of depression - area around a discharging well where the hydraulic head
in the aquifer is lowered by pumping.
Want to compute drawdown and T and S.
Unsteady flow - flow in which head changes with time.
| Assumptions | ||
| (1.) Bottom confining layer | ||
| (2.) All geologic units are horizontal and of infinite extent. | ||
| (3.) Potentiometric surface is horizontal prior to the start of pumping. | ||
| (4.) Potentiometric surface is not changing with time prior to the start of pumping. | ||
| (5.) All changes in potentiometric surface position are due to the effect of the pumping well. | ||
| (6.) Aquifer is homogeneous and isotropic. | ||
| (7.) All flow is radial toward the well. | ||
| (8.) Ground-water flow is horizontal. | ||
| (9.) Darcys Law is valid. | ||
| (10.) Ground-water has constant density and viscosity. | ||
| (11.) Pumping well and observation wells are fully penetrating. | ||
| (12.) Well has an infinitesimal diameter and is 100% efficient. | ||
Unsteady Radial Flow
| Assume that the aquifer has a radial symmetry . | |||
| Radial flow toward well. | |||
| Plan view | Cross Section | ||
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Use polar coordinates to describe flow.

Therefore, can express flow with-
| (1) q value of angle | |
| (2) r Radial distance |
If Aquifer is isotropic in horizontal plane. Then ® Flow is radial.
Equation for confined (radial) -Hantush 1964
| r = radial distance from pumping well. |
If recharge- leakage through a confining layer
| e = rate of vertical leakage (L/T) |
Solutions to the equations are extremely useful
| Includes- | |
| Laplace transforms | |
| Fourier transform | |
| Bessel functions | |
| Error function |
Use these equations to determine drawdown around a pumping well.

Aquifer test in a confined aquifer.

Aquifer test in an unconfined aquifer.