# Slug Tests

by Glenn M. Duffield, President, HydroSOLVE, Inc.

Figure 1. Typical well configuration for a slug test in an unconfined aquifer. |

The slug test method is a popular and inexpensive means of estimating the hydraulic
properties of aquifers (primarily hydraulic conductivity, **K**).

#### Confined Aquifer Methods

Methods for analyzing slug tests in confined aquifers include Cooper et al. (1967), Hvorslev (1951) and Hyder et al. (1994). Strictly speaking, the Bouwer-Rice (1976) solution is intended for unconfined aquifers; however, Bouwer (1989) pointed out that the same solution method also should give reasonable estimates of K in confined aquifers. A study by Brown et al. (1995) tested the applicability of the Bouwer-Rice solution to confined conditions. Based on the cases studied in their work, the Bouwer-Rice solution yielded superior estimates of K compared to the Hvorslev solution for partially penetrating wells in confined aquifers.

#### Unconfined Aquifer Methods

Slug test analysis methods for unconfined aquifers include Bouwer-Rice (1976) and Hyder et al. (1994). For the same reason that Bouwer (1989) found that the Bouwer-Rice method has application to both confined and unconfined aquifers, we may also extend the use of the Hvorslev (1951) method from confined to unconfined aquifers in many cases. According to Brown et al. (1995), the upper boundary condition appears to have very little effect on the estimate of K except when the top of the well screen is close to the boundary (a point made by Bouwer [1989] as well). Therefore, we can expect that application of the Hvorslev solution with an appropriate shape factor for a partially penetrating well will yield reasonable K estimates for an unconfined aquifer when the water table is not close to the top of the well screen.

The following example from Butler (1998) compares the KGS Model (Hyder et al. 1994), Bouwer-Rice (1976) and Hvorslev (1951) methods for a slug test conducted in a partially penetrating well in an unconfined aquifer. The initial displacement in the well was 0.671 m and other parameters for the test are given in Table 1. The depth to the top of the well screen is 16.77 m below the water table and the aquifer thickness is 47.87 m. Analyses performed with AQTESOLV for the three methods are shown in Figures 2 through 4. For consistency and objectivity, the recommended normalized head ranges of Butler (1998) guided the fitting of the Bouwer-Rice and Hvorslev solutions. The KGS Model (Figure 2) rigorously accounts for elastic storage in the aquifer, while the Bouwer-Rice (Figure 3) and Hvorslev (Figure 4) methods both use the quasi-steady-state approximation of slug-induced flow (Butler 1998); however, despite different underlying assumptions, all three methods yield very similar estimates of K for this slug test. Interestingly, the Hvorslev solution, which is commonly associated with confined aquifers, produces an estimate of K that is closer to the value computed with the more rigorous KGS Model than the Bouwer-Rice solution which is typically associated with unconfined aquifers.

Table 1. Well Construction Details for Well 4, Pratt County Monitoring Site 36 | ||||

Well Radius, r _{w} (m) |
Casing Radius, r _{c} (m) |
Screen Length, L (m) |
Aquifer Thickness, b (m) |
Depth to Top of Screen, d (m) |

0.125 | 0.064 | 1.52 | 47.87 | 16.77 |

Figure 2. Analysis of Unconfined Slug Test, Pratt County Well 4, Test 2 Using KGS (Hyder et al. 1994) Model. |

Figure 3. Analysis of Unconfined Slug Test, Pratt County Well 4, Test 2 Using Bouwer and Rice (1976) Solution. |

Figure 4. Analysis of Unconfined Slug Test, Pratt County Well 4, Test 2 Using Hvorslev (1951) Solution. |

#### Normalized Head

Normalized head is defined as follows:

* normalized head* = H(t)/H

_{0}

where H(t) is the displacement measured at time t and H_{0} is the initial
displacement at time t=0.

#### Dimensionless Storage Parameter (a)

Cooper et al. (1967) define a dimensionless storage parameter (α) as follows:

α = r_{w}²S/r_{c}²

where r_{w} is well radius, S is aquifer storage coefficient and r_{c}
is casing radius.

#### Dimensionless Time (t_{D})

Dimensionless time (t_{D}) is defined as follows:

t_{D} = Tt/r_{c}²

where T is transmissivity, t is time and r_{c} is casing radius.

#### Gravel Pack Correction

For a partially submerged well screen, Bouwer (1989) recommends the following calculation to correct the casing radius for slug test analysis:

* equivalent casing radius* = [(1-n)r

_{c}² + nr

_{w}²]

^{½}

where n is effective porosity of the gravel/filter pack, r_{c} is casing radius
and r_{w} is well radius.

#### Effective Screen Length (L)

In most settings, the * effective length of the well screen*
used in equations for slug test analysis is the nominal length of the well screen. In low-permeability aquifers,
Fetter (2001) advises using the length of the
gravel/filter pack in the well annulus for the effective screen length; however,
Butler
(1998) recommends always using the nominal screen length for the analysis of slug test
data. Butler reasons that well development (e.g., pumping, surging, etc.) has little
effect on restoring the aquifer adjacent to the wellbore to its pre-drilling condition
outside of the screened interval of the well. Consequently, sections of the
gravel/filter pack above or below the well screen, where the aquifer adjacent to the
wellbore remains undeveloped, can contribute little flow during a slug test.

#### Double Straight-Line Effect

Bouwer (1989) pointed out a * double straight-line effect* in
certain slug test analyses when the screen of the test well straddles the water table
(i.e., the well screen is partially submerged).

In other cases, data from a slug test may show a * concave upward appearance*
that is similar to the double straight-line effect but unrelated to a partially submerged
well screen. According to
Butler (1998), the concave upward appearance of slug test
data becomes more pronounced as the dimensionless
storage parameter (α) increases.

Figure 5. Slug test response as a function of dimensionless storage parameter (a) for a fully penetrating well in a confined aquifer. Concave upward appearance is more pronounced for larger values of a. |

Figure 6. Slug test response as a function of dimensionless storage
parameter (a) for a fully penetrating well (L/r_{w}=1000)
in an unconfined aquifer. Concave upward appearance is more pronounced for larger
values of a. |

##### » Wells Screened Across Water Table

Slug tests performed in * wells screened across the water table*
often result in data with a double straight line.

Bouwer (1989) interprets the first (earlier) straight segment of the data as drainage into the well from a permeable gravel pack. The second (later) straight portion of the data is considered more indicative of flow into the well from the aquifer.

According to Bouwer (1989), when the well screen is partially submerged and the double straight-line effect is present, the second straight portion of the data should be used to calculate the K of the aquifer with the Bouwer-Rice (1976) slug test solution. Butler (1998) confirms this approach and recommends matching the straight line to normalized head values ranging between 0.2 and 0.3 (see below).

If the well screen remains submerged throughout a slug test, flow into the well should be controlled by the aquifer alone, and the double straight-line effect should not be apparent (Bouwer 1989).

#### Recommended Normalized Head Ranges

To overcome ambiguity in matching straight-line solutions to slug test data exhibiting the double straight-line effect or a concave upward appearance, Butler (1998) recommends matching the Hvorslev (1951) and Bouwer-Rice (1976) straight-line solutions to a specific range of normalized head.

SolutionMethod |
Recommended Normalized Head Rangefor Straight Line Match |

Hvorslev (1951) | 0.15 to 0.25 |

Bouwer-Rice (1976) | 0.20 to 0.30 |

** See also:**
slug tests