## ASTM-D4105 › Historical Revision Information

Standard Test Method for (Analytical Procedure) for Determining Transmissivity and Storage Coefficient of Nonleaky Confined Aquifers by the Modified Theis Nonequilibrium Method

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### Scope

1.1 This test method covers an analytical procedure for determining transmissivity and storage coefficient of a nonleaky confined aquifer under conditions of radial flow to a fully penetrating well of constant flux. This test method is a shortcut procedure used to apply the Theis nonequilibrium method. The Theis method is described in Test Method D4106.

1.2 This test method is used in conjunction with the field procedure given in Test Method D4050.

1.3 Limitations—The limitations of this test method are primarily related to the correspondence between the field situation and the simplifying assumptions of this test method (see 5.1). Furthermore, application is valid only for values of u less than 0.01 (u is defined in Eq 2, in 8.6).

1.4 This standard does not purport to address all of the safety concerns, if any, associated with its use. It is the responsibility of the user of this standard to establish appropriate safety and health practices and determine the applicability of regulatory limitations prior to use.

### Significance and Use

Assumptions:

Well discharges at a constant rate, Q.

Well is of infinitesimal diameter and fully penetrates the aquifer, that is, the well is open to the full thickness of the aquifer.

The nonleaky aquifer is homogeneous, isotropic, and areally extensive. A nonleaky aquifer receives insignificant contribution of water from confining beds.

Discharge from the well is derived exclusively from storage in the aquifer.

The geometry of the assumed aquifer and well conditions are shown in Fig. 1.

Implications of Assumptions:

Implicit in the assumptions are the conditions of radial flow. Vertical flow components are induced by a control well that partially penetrates the aquifer, that is, not open to the aquifer through its full thickness. If the control well does not fully penetrate the aquifer, the nearest piezometer or partially penetrating observation well should be located at a distance, r, beyond which vertical flow components are negligible, where according to Reed (5)

This section applies to distance-drawdown calculations of transmissivity and storage coefficient and time-drawdown calculations of storage coefficient. If possible, compute transmissivity from time-drawdown data from wells located within a distance, r, of the pumped well using data measured after the effects of partial penetration have become constant. The time at which this occurs is given by Hantush (6) by:

Fully penetrating observation wells may be placed at less than distance r from the control well. Observation wells may be on the same or on various radial lines from the control well.

The Theis method assumes the control well is of infinitesimal diameter. Also, it assumes that the water level in the control well is the same as in the aquifer contiguous to the well. In practice these assumptions may cause a difference between the theoretical drawdown and field measurements of drawdown in the early part of the test and in and near the control well. Control well storage is negligible after a time, t, given by the following equation after weeks (7).

where: | ||
---|---|---|

_{c} | = | the radius of the control well in the interval that includes the water level changes. |

Application of Theis Nonequilibrium Method to Unconfined Aquifers:

Although the assumptions are applicable to confined conditions, the Theis solution may be applied to unconfined aquifers if drawdown is small compared with the saturated thickness of the aquifer or if the drawdown is corrected for reduction in thickness of the aquifer and the effects of delayed gravity yield are small.

Reduction in Aquifer Thickness—In an unconfined aquifer, dewatering occurs when the water levels decline in the vicinity of a pumping well. Corrections in drawdown need to be made when the drawdown is a significant fraction of the aquifer thickness as shown by Jacob (8). The drawdown, s, needs to be replaced by s′, the drawdown that would occur in an equivalent confined aquifer, where:

Gravity Yield Effects—In unconfined aquifers, delayed gravity yield effects may invalidate measurements of drawdown during the early part of the test for application to the Theis method. Effects of delayed gravity yield are negligible in partially penetrating observation wells at a distance, r, from the control well, where:

after the time, t, as given in the following equation from Neuman (9):

where: | ||
---|---|---|

_{y} | = | the specific yield. |

For fully penetrating observation wells, the effects of delayed yield are negligible at the distance, r, in Eq 11 after one tenth of the time given in the Eq 12.

FIG. 1 Cross Section Through a Discharging Well in a Nonleaky Confined Aquifer

### Keywords

aquifer tests; aquifers; confined aquifers; control wells; groundwater; hydraulic properties; observation wells; storage coefficient; transmissivity; unconfined aquifers; Aquifers; Coefficient of storage; Confined aquifers; Control wells; Field testing--ground water/aquifers; Ground water; Hydraulic conductivity/transmissivity; Observation wells; Storativity; Theis methods of analysis; Transmissivity and reflectivity; Unconfined/unconsolidated aquifers; ICS Number Code 93.160 (Hydraulic construction)

### To find similar documents by ASTM Volume:

04.08 (Soil and Rock (I): D420 - D5876)

### To find similar documents by classification:

93.160 (Hydraulic construction Hydraulic energy equipment, see 27.140)

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### Document Number

ASTM-D4105-96(2008)

### Revision Level

1996 R08 EDITION

### Status

Superseded

### Modification Type

Reapproval

### Publication Date

Oct. 1, 2008

### Document Type

Test Method

### Page Count

5 pages

### Committee Number

D18.21