Hydraulic conductivity
Hydraulic conductivity, symbolically represented as , is a property of vascular plants, soils and rocks, that describes the ease with which a fluid (usually water) can move through pore spaces or fractures. It depends on the intrinsic permeability of the material, the degree of saturation, and on the density and viscosity of the fluid. Saturated hydraulic conductivity, K_{sat}, describes water movement through saturated media.
By definition, hydraulic conductivity is the ratio of velocity to hydraulic gradient indicating permeability of porous media.
Contents
Methods of determination
There are two broad categories of determining hydraulic conductivity:
 Empirical approach by which the hydraulic conductivity is correlated to soil properties like pore size and particle size (grain size) distributions, and soil texture
 Experimental approach by which the hydraulic conductivity is determined from hydraulic experiments using Darcy's law
The experimental approach is broadly classified into:
 Laboratory tests using soil samples subjected to hydraulic experiments

Field tests (on site, in situ) that are differentiated into:
 small scale field tests, using observations of the water level in cavities in the soil
 large scale field tests, like pump tests in wells or by observing the functioning of existing horizontal drainage systems.
The small scale field tests are further subdivided into:
 infiltration tests in cavities above the water table
 slug tests in cavities below the water table
Estimation by empirical approach
Estimation from grain size
Allen Hazen derived an empirical formula for approximating hydraulic conductivity from grain size analyses:
where
 Hazen's empirical coefficient, which takes a value between 0.0 and 1.5 (depending on literatures), with an average value of 1.0. A.F. Salarashayeri & M. Siosemarde give C as usually taken between 1.0 and 1.5, with D in mm and K in cm/s.
 is the diameter of the 10 percentile grain size of the material
Pedotransfer function
A pedotransfer function (PTF) is a specialized empirical estimation method, used primarily in the soil sciences, however has increasing use in hydrogeology.^{[1]} There are many different PTF methods, however, they all attempt to determine soil properties, such as hydraulic conductivity, given several measured soil properties, such as soil particle size, and bulk density.
Determination by experimental approach
There are relatively simple and inexpensive laboratory tests that may be run to determine the hydraulic conductivity of a soil: constanthead method and fallinghead method.
Laboratory methods
Constanthead method
The constanthead method is typically used on granular soil. This procedure allows water to move through the soil under a steady state head condition while the quantity (volume) of water flowing through the soil specimen is measured over a period of time. By knowing the quantity of water measured, length of specimen, crosssectional area of the specimen, time required for the quantity of water to be discharged, and head , the hydraulic conductivity can be calculated:
where is the flow velocity. Using Darcy's Law:
and expressing the hydraulic gradient as:
where is the difference of hydraulic head over distance , yields:
Solving for gives:
Fallinghead method
In the fallinghead method, the soil sample is first saturated under a specific head condition. The water is then allowed to flow through the soil without adding any water, so the pressure head declines as water passes through the specimen. The advantage to the fallinghead method is that it can be used for both finegrained and coarsegrained soils.^{[2]} Calculating the hydraulic conductivity is more complicated because of the changing pressure head, and requires solving a differential equation; the resulting equation is:
Insitu (field) methods
Augerhole method
There are also insitu methods for measuring the hydraulic conductivity in the field.
When the water table is shallow, the augerhole method, a slug test, can be used for determining the hydraulic conductivity below the water table.
The method was developed by Hooghoudt (1934) ^{[3]} in The Netherlands and introduced in the US by Van Bavel en Kirkham (1948).^{[4]}
The method uses the following steps:
 an augerhole is perforated into the soil to below the water table
 water is bailed out from the augerhole
 the rate of rise of the water level in the hole is recorded
 the value is calculated from the data as:^{[5]}
where: horizontal saturated hydraulic conductivity (m/day), depth of the waterlevel in the hole relative to the water table in the soil (cm), at time , at time , time (in seconds) since the first measurement of as , and is a factor depending on the geometry of the hole:
where: radius of the cylindrical hole (cm), is the average depth of the water level in the hole relative to the water table in the soil (cm), found as , and is the depth of the bottom of the hole relative to the water table in the soil (cm).
The picture shows a large variation of values measured with the augerhole method in an area of 100 ha.^{[6]} The ratio between the highest and lowest values is 25. The cumulative frequency distribution is lognormal and was made with the CumFreq program.
Related magnitudes
Transmissivity
The transmissivity is a measure of how much water can be transmitted horizontally, such as to a pumping well.
 Transmissivity should not be confused with the similar word transmittance used in optics, meaning the fraction of incident light that passes through a sample.
An aquifer may consist of soil layers. The transmissivity for horizontal flow of the soil layer with a saturated thickness and horizontal hydraulic conductivity is:
Transmissivity is directly proportional to horizontal hydraulic conductivity and thickness . Expressing in m/day and in m, the transmissivity is found in units m^{2}/day.
The total transmissivity of the aquifer is:^{[5]}
 where signifies the summation over all layers .
The apparent horizontal hydraulic conductivity of the aquifer is:
where , the total thickness of the aquifer, is , with .
The transmissivity of an aquifer can be determined from pumping tests.^{[7]}
Influence of the water table
When a soil layer is above the water table, it is not saturated and does not contribute to the transmissivity. When the soil layer is entirely below the water table, its saturated thickness corresponds to the thickness of the soil layer itself. When the water table is inside a soil layer, the saturated thickness corresponds to the distance of the water table to the bottom of the layer. As the water table may behave dynamically, this thickness may change from place to place or from time to time, so that the transmissivity may vary accordingly.
In a semiconfined aquifer, the water table is found within a soil layer with a negligibly small transmissivity, so that changes of the total transmissivity () resulting from changes in the level of the water table are negligibly small.
When pumping water from an unconfined aquifer, where the water table is inside a soil layer with a significant transmissivity, the water table may be drawn down whereby the transmissivity reduces and the flow of water to the well diminishes.
Resistance
The resistance to vertical flow () of the soil layer with a saturated thickness and vertical hydraulic conductivity is:
Expressing in m/day and in m, the resistance () is expressed in days.
The total resistance () of the aquifer is:^{[5]}
where signifies the summation over all layers:
The apparent vertical hydraulic conductivity () of the aquifer is:
where is the total thickness of the aquifer: , with
The resistance plays a role in aquifers where a sequence of layers occurs with varying horizontal permeability so that horizontal flow is found mainly in the layers with high horizontal permeability while the layers with low horizontal permeability transmit the water mainly in a vertical sense.
Anisotropy
When the horizontal and vertical hydraulic conductivity ( and ) of the soil layer differ considerably, the layer is said to be anisotropic with respect to hydraulic conductivity.
When the apparent horizontal and vertical hydraulic conductivity ( and ) differ considerably, the aquifer is said to be anisotropic with respect to hydraulic conductivity.
An aquifer is called semiconfined when a saturated layer with a relatively small horizontal hydraulic conductivity (the semiconfining layer or aquitard) overlies a layer with a relatively high horizontal hydraulic conductivity so that the flow of groundwater in the first layer is mainly vertical and in the second layer mainly horizontal.
The resistance of a semiconfining top layer of an aquifer can be determined from pumping tests.^{[7]}
When calculating flow to drains ^{[8]} or to a well field ^{[9]} in an aquifer with the aim to control the water table, the anisotropy is to be taken into account, otherwise the result may be erroneous.
Relative properties
Because of their high porosity and permeability, sand and gravel aquifers have higher hydraulic conductivity than clay or unfractured granite aquifers. Sand or gravel aquifers would thus be easier to extract water from (e.g., using a pumping well) because of their high transmissivity, compared to clay or unfractured bedrock aquifers.
Hydraulic conductivity has units with dimensions of length per time (e.g., m/s, ft/day and (gal/day)/ft² ); transmissivity then has units with dimensions of length squared per time. The following table gives some typical ranges (illustrating the many orders of magnitude which are likely) for K values.
Hydraulic conductivity (K) is one of the most complex and important of the properties of aquifers in hydrogeology as the values found in nature:
 range over many orders of magnitude (the distribution is often considered to be lognormal),
 vary a large amount through space (sometimes considered to be randomly spatially distributed, or stochastic in nature),
 are directional (in general K is a symmetric secondrank tensor; e.g., vertical K values can be several orders of magnitude smaller than horizontal K values),
 are scale dependent (testing a m³ of aquifer will generally produce different results than a similar test on only a cm³ sample of the same aquifer),
 must be determined indirectly through field pumping tests, laboratory column flow tests or inverse computer simulation, (sometimes also from grain size analyses), and
 are very dependent (in a nonlinear way) on the water content, which makes solving the unsaturated flow equation difficult. In fact, the variably saturated K for a single material varies over a wider range than the saturated K values for all types of materials (see chart below for an illustrative range of the latter).
Ranges of values for natural materials
Table of saturated hydraulic conductivity (K) values found in nature
Values are for typical fresh groundwater conditions — using standard values of viscosity and specific gravity for water at 20 °C and 1 atm. See the similar table derived from the same source for intrinsic permeability values.^{[10]}
K (cm/s)  10²  10^{1}  10^{0}=1  10^{−1}  10^{−2}  10^{−3}  10^{−4}  10^{−5}  10^{−6}  10^{−7}  10^{−8}  10^{−9}  10^{−10} 
K (ft/day)  10^{5}  10,000  1,000  100  10  1  0.1  0.01  0.001  0.0001  10^{−5}  10^{−6}  10^{−7} 
Relative Permeability  Pervious  SemiPervious  Impervious  
Aquifer  Good  Poor  None  
Unconsolidated Sand & Gravel  Well Sorted Gravel  Well Sorted Sand or Sand & Gravel  Very Fine Sand, Silt, Loess, Loam  
Unconsolidated Clay & Organic  Peat  Layered Clay  Fat / Unweathered Clay  
Consolidated Rocks  Highly Fractured Rocks  Oil Reservoir Rocks  Fresh Sandstone  Fresh Limestone, Dolomite  Fresh Granite 
Source: modified from Bear, 1972
See also
 Aquifer test
 Pedotransfer function–for estimating hydraulic conductivities given soil properties
References
 ^ Wösten, J.H.M., Pachepsky, Y.A., and Rawls, W.J. (2001). "Pedotransfer functions: bridging the gap between available basic soil data and missing soil hydraulic characteristics". Journal of Hydrology. 251 (34): 123–150. Bibcode:2001JHyd..251..123W. doi:10.1016/S00221694(01)004644.
 ^ Liu, Cheng "Soils and Foundations." Upper Saddle River, New Jersey: Prentice Hall, 2001 ISBN 0130255173
 ^ S.B.Hooghoudt, 1934, in Dutch. Bijdrage tot de kennis van enige natuurkundige grootheden van de grond. Verslagen Landbouwkundig Onderzoek No. 40 B, p. 215345.
 ^ C.H.M. van Bavel and D. Kirkham, 1948. Field measurement of soil permeability using auger holes. Soil. Sci. Soc. Am. Proc 13:9096.
 ^ ^{a} ^{b} ^{c} Determination of the Saturated Hydraulic Conductivity. Chapter 12 in: H.P.Ritzema (ed., 1994) Drainage Principles and Applications, ILRI Publication 16, p.435476. International Institute for Land Reclamation and Improvement, Wageningen (ILRI), The Netherlands. ISBN 9070754339. Free download from: [1] , under nr. 6, or directly as PDF : [2]
 ^ Drainage research in farmers' fields: analysis of data. Contribution to the project “Liquid Gold” of the International Institute for Land Reclamation and Improvement (ILRI), Wageningen, The Netherlands. Free download from : [3] , under nr. 2, or directly as PDF : [4]
 ^ ^{a} ^{b} J.Boonstra and R.A.L.Kselik, SATEM 2002: Software for aquifer test evaluation, 2001. Publ. 57, International Institute for Land reclamation and Improvement (ILRI), Wageningen, The Netherlands. ISBN 9070754541 On line : [5]
 ^ The energy balance of groundwater flow applied to subsurface drainage in anisotropic soils by pipes or ditches with entrance resistance. International Institute for Land Reclamation and Improvement, Wageningen, The Netherlands. On line : [6] . Paper based on: R.J. Oosterbaan, J. Boonstra and K.V.G.K. Rao, 1996, “The energy balance of groundwater flow”. Published in V.P.Singh and B.Kumar (eds.), SubsurfaceWater Hydrology, p. 153160, Vol.2 of Proceedings of the International Conference on Hydrology and Water Resources, New Delhi, India, 1993. Kluwer Academic Publishers, Dordrecht, The Netherlands. ISBN 9780792336518 . On line : [7]. The corresponding free EnDrain program can be downloaded from: [8]
 ^ Subsurface drainage by (tube)wells, 9 pp. Explanation of equations used in the WellDrain model. International Institute for Land Reclamation and Improvement (ILRI), Wageningen, The Netherlands. On line: [9] . The corresponding free WellDrain program can be downloaded from : [10]
 ^ Bear, J. (1972). Dynamics of Fluids in Porous Media. Dover Publications. ISBN 0486656756.
External links
 Hydraulic conductivity calculator