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GIROUD et al. D Leachate Flow <strong>in</strong> Leakage Collection Layers Due <strong>to</strong> Geomembrane Defects<br />

ity, k. The lam<strong>in</strong>ar <strong>flow</strong> assumption is applicable <strong>to</strong> sand and approximately applicable<br />

<strong>to</strong> gravel and geonets. Furthermore, it is assumed that the hydraulic conductivity,<br />

k, of a given <strong>leakage</strong> <strong>collection</strong> layer material has a unique value, that is the hydraulic<br />

conductivity of the saturated material.<br />

S The <strong>leachate</strong> is assumed <strong>to</strong> have the same density and viscosity as water. This assumption<br />

should be satisfied <strong>in</strong> the case of all modern landfills <strong>due</strong> <strong>to</strong> the generally low<br />

concentration of chemicals <strong>in</strong> <strong>leachate</strong>. As a result, the values of the hydraulic conductivity,<br />

k, of the <strong>leakage</strong> <strong>collection</strong> layer material measured us<strong>in</strong>g water are applicable<br />

<strong>to</strong> <strong>leachate</strong> <strong>flow</strong>.<br />

S The <strong>defects</strong> <strong>in</strong> the primary l<strong>in</strong>er are assumed <strong>to</strong> have a small dimension <strong>in</strong> all directions<br />

of the plane of the geomembrane so that the result<strong>in</strong>g leaks can be treated as<br />

po<strong>in</strong>t source leaks. Examples of such <strong>defects</strong> are circular or quasi-circular holes <strong>in</strong><br />

geomembranes with a diameter (or an equivalent diameter) of less than approximately<br />

10 <strong>to</strong> 20 mm (i.e. a surface area less than approximately 1 <strong>to</strong> 3 cm 2 ). Examples of<br />

<strong>defects</strong> that are not consistent with the above assumption are <strong>defects</strong> with a surface<br />

area larger than approximately 3 cm 2 and <strong>defects</strong> with a great length such as cracks<br />

or a relatively long length of open seam <strong>in</strong> a geomembrane.<br />

S The rate of <strong>leachate</strong> migration through a given defect is Q under steady-state <strong>flow</strong><br />

conditions, which are assumed <strong>to</strong> exist <strong>in</strong> all cases.<br />

S It is assumed that <strong>flow</strong>s through various <strong>defects</strong> do not <strong>in</strong>terfere. In other words, the<br />

wetted zones related <strong>to</strong> different <strong>defects</strong> do not overlap. (Cases where wetted zones<br />

may overlap are discussed <strong>in</strong> Section 4.4.5.)<br />

S Capillarity <strong>in</strong> the <strong>leakage</strong> <strong>collection</strong> layer is not considered (which limits the validity<br />

of the study by exclud<strong>in</strong>g <strong>leakage</strong> <strong>collection</strong> <strong>layers</strong> constructed with f<strong>in</strong>e sands) and<br />

the secondary l<strong>in</strong>er is assumed <strong>to</strong> be impermeable (i.e. it is a geomembrane with no<br />

<strong>defects</strong>, possibly on a clay layer, but not a clay layer alone). Therefore, all of the <strong>leachate</strong><br />

that passes through <strong>defects</strong> <strong>in</strong> the primary l<strong>in</strong>er <strong>flow</strong>s <strong>in</strong> the <strong>leakage</strong> <strong>collection</strong><br />

layer.<br />

Other assumptions will be made as required at various steps <strong>in</strong> the analysis.<br />

2.2 AssumptionsSpecific <strong>to</strong> the Case Where the Leakage Collection Layer is not<br />

Full<br />

As mentioned <strong>in</strong> Section 1.2.2, two cases are discussed <strong>in</strong> this paper: the case where<br />

the <strong>leakage</strong> <strong>collection</strong> layer is not full and the case where the <strong>leakage</strong> <strong>collection</strong> layer<br />

is full. The former will be the lead case, and results for the case where the <strong>leakage</strong><br />

<strong>collection</strong> layer is full will then be derived from results for the case where the <strong>leakage</strong><br />

<strong>collection</strong> layer is not full.<br />

In the case where the <strong>leakage</strong> <strong>collection</strong> layer is not full, the <strong>flow</strong> rate through the<br />

considered <strong>defects</strong> <strong>in</strong> the primary l<strong>in</strong>er is assumed <strong>to</strong> be small enough that the maximum<br />

thickness of <strong>leachate</strong> <strong>in</strong> the <strong>leakage</strong> <strong>collection</strong> layer is less than the thickness of the <strong>leakage</strong><br />

<strong>collection</strong> layer. In this case, assumptions regard<strong>in</strong>g the hydraulic gradient and the<br />

shape of the phreatic surface can be made, as described below.<br />

As <strong>in</strong>dicated <strong>in</strong> Section 1.2.1, the <strong>leachate</strong> that, has passed through a defect <strong>in</strong> the primary<br />

l<strong>in</strong>er, first <strong>flow</strong>s more or less vertically through the <strong>leakage</strong> <strong>collection</strong> layer upper<br />

220 GEOSYNTHETICS INTERNATIONAL S 1997, VOL. 4, NOS. 3-4

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