Well 1:Unconfined Aquifer

nach unten Introduction


This example shows a homogeneous and isotropic aquifer with a steady state flow and a groundwater withdrawal at a well. We are looking for the lowering of the groundwater surface caused by the withdrawal. For this problem analytical solutions can be found in literature.

Model and parameters
Theoretical background
Discretisation
Comparison of the results
Literature



nach oben nach unten Model and parameters

The following figure represents the principle of a lowered aquifer caused by a withdrawal at a well.

Modellprinzip


Figure: Principle of the model

The example should have the following characteristics:

permeability kf = 5*10-4 m/s> KWER
thickness M = 45 m GELA = 45
UNTE = 0
reach R = 500 m expansion of the model
well radius r0 = 0,3 m -
initial potential head H0 = 40,00 m
HB = 32,55 m
POTE = 40
(edge)
POTE = 32,55
(nodes inside r0)



nach oben nach unten Theoretical background

A partial Laplace differential equation is derived from the potential function and the flow function to get the analytic solution of a 2D flow. The derivable function of a complex variable for this problem is:
Formel01
With the potential- and flow function
Formel02 Formel03
circle potential lines and linear streamlines result. The boundary conditions are given with h(R) = H0 and h(r0) = HB. The productiveness of the well is calculated with the formulation

formel04
and with one of the boundary conditions to
Formel05
If the withdrawal is preset and the adjusting altitude in the well should be calculated this is done by converting the function for HB given above
Formel06
The potential head is determined with
formel04
and the boundary condition h(r0) = HB. For this the equation given above is converted to h so that
Formel07
results. In this equation the boundary condition h(r0) = HB is entered and the constant c can be determined.
Formel08
Entering the constant c into h(r) results in this:
Formel09
This equation can be summarized by transformation:
Formel10
With the boundary condition of the model area mentioned above and the equation for the reach of the well by Sichardt the altitude in the well can be calculated.
Formel11
From this
Modellprinzip
(see description concerning the model parameters mentioned above)
The productiveness of the well is determined to:
Modellprinzip



nach oben nach unten Discretisation

The file Brunnen_f_s_e.zip includes the file "Brunnen_frei_stat.net". With this mesh file the validation was done. A horizontal model with the time unit "year" was created. The initial parameters are described in the table in the chapter "Model and parameters". The generated mesh is shown in the following figure.

netz



Figure: FE-mesh in SPRING

 

The next figure shows the calculated potential heads (red lines) and the nodes to which the attribute POTE was assigned(blue points).

potentiale


Figure: With SPRING calculated potential heads



nach oben nach unten Comparison of the calculation results

The following figure shows the results of SPRING arranged face to face to the analytical solution. The analytical solution is computed with the file Brunnen_frei_stat_e.xls. This file is also saved in the file brunnen_f_s_e.zip. You can see clearly that the solution of SPRING does not vary much. The maximum difference between the two calculated potential heads is 0,05m. The productiveness which is calculated in SPRING varies about -0,00241 m3/s. This is an amount which can be neglected. If the grid is refined around the well the difference will be smaller.

vergleich


Comparison of the analytical solution with the results in SPRING



nach oben Literature

[David] Ioan David; Grundwasserhydraulik Strömungs- und Transportvorgänge, Vieweg, 1997
[Kinzelbach] W. Kinzelbach; Numerische Methoden zur Modellierung des Transports von Schadstoffen im Grundwasser, Oldenbourg, 1987
[SPRING] SPRING; Simulation of Processes in Groundwater, Programm- beschreibung,Version 3.2

Seitenanfang
Theoretical background