Properties of Aquifers Part I - Porosity & Permeability - Myweb @ CW ...

Properties of Aquifers Part I - Porosity & Permeability - Myweb @ CW ... Properties of Aquifers Part I - Porosity & Permeability - Myweb @ CW ...

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GLY 15/518 - Groundwater Geology Chapter 2: Sections 3.2 - 3.5 Material for week of 9/17/12 Properties of Aquifer Materials There are two basic characteristics of an aquifer in terms of its potential as a water resource. I) First is various measures as to how much water is held in an aquifer including: porosity (η), specific yield (Sy), and storage (Sr) II) The other is measures of how easily the water flows through the aquifer: permeability, hydraulic conductivity (k), transmissivity (T) I) Quantity of Available Water in an Aquifer porosity types: Most sediment and rock contains some amount of void space intergrain spaces: ! a primary porosity in sediments and sedimentary rock ! ! (though cementation decreases this) vessicles: ! a primary porosity in volcanic rocks dissolution voids: ! a secondary porosity in limestone fractures: ! a secondary porosity in all kinds of rock porosity: Porous aquifer materials contain void spaces throughout the mass of sediment and rock. The space available for water storage can be defined as porosity in sediments: The amount of void space in sediments and sedimentary rocks depends on the properties of the materials, including packing, grain size, grain shape, sorting, the degree of cementation, etc. packing: Uniform-size spheres stacked one on top of another (like balls in a box) have a cubic packing structure. Cubic packing results in about 48% porosity (52% of space taken up by the solid balls). If uniform spheres are stacked so the spheres of every other row fit into the hollows between balls of the adjacent row, this rhombohedral packing reduces porosity to its minimum (for uniform spheres) of about 26%. Of course natural sediments are neither perfectly spherical, perfectly uniform in size, nor packed in perfectly cubic or rhombohedral order but will fall somewhere between those two end members. sorting: Well-sorted (fairly uniformly sized) sediments (or spheres) maintain a relatively high degree of porosity. But if sediments occur in a mixture of sizes, the smaller particles will fill in the spaces between the larger particles, reducing the porosity.

GLY 15/518 - Groundwater Geology<br />

Chapter 2: Sections 3.2 - 3.5<br />

Material for week <strong>of</strong> 9/17/12<br />

<strong>Properties</strong> <strong>of</strong> Aquifer Materials<br />

There are two basic characteristics <strong>of</strong> an aquifer in terms <strong>of</strong> its potential as a water<br />

resource.<br />

I) First is various measures as to how much water is held in an aquifer including:<br />

porosity (η), specific yield (Sy), and storage (Sr)<br />

II) The other is measures <strong>of</strong> how easily the water flows through the aquifer:<br />

permeability, hydraulic conductivity (k), transmissivity (T)<br />

I) Quantity <strong>of</strong> Available Water in an Aquifer<br />

porosity types: Most sediment and rock contains some amount <strong>of</strong> void space<br />

intergrain spaces: ! a primary porosity in sediments and sedimentary rock<br />

! ! (though cementation decreases this)<br />

vessicles: !<br />

a primary porosity in volcanic rocks<br />

dissolution voids: ! a secondary porosity in limestone<br />

fractures: !<br />

a secondary porosity in all kinds <strong>of</strong> rock<br />

porosity: Porous aquifer materials contain void spaces throughout the mass <strong>of</strong><br />

sediment and rock. The space available for water storage can be defined as<br />

porosity in sediments: The amount <strong>of</strong> void space in sediments and sedimentary rocks<br />

depends on the properties <strong>of</strong> the materials, including packing, grain size, grain<br />

shape, sorting, the degree <strong>of</strong> cementation, etc.<br />

packing: Uniform-size spheres stacked one on top <strong>of</strong> another (like balls in a box) have<br />

a cubic packing structure. Cubic packing results in about 48% porosity (52% <strong>of</strong><br />

space taken up by the solid balls). If uniform spheres are stacked so the spheres <strong>of</strong><br />

every other row fit into the hollows between balls <strong>of</strong> the adjacent row, this<br />

rhombohedral packing reduces porosity to its minimum (for uniform spheres) <strong>of</strong><br />

about 26%. Of course natural sediments are neither perfectly spherical, perfectly<br />

uniform in size, nor packed in perfectly cubic or rhombohedral order but will fall<br />

somewhere between those two end members.<br />

sorting: Well-sorted (fairly uniformly sized) sediments (or spheres) maintain a relatively<br />

high degree <strong>of</strong> porosity. But if sediments occur in a mixture <strong>of</strong> sizes, the smaller<br />

particles will fill in the spaces between the larger particles, reducing the porosity.


sediment size:<br />

geological classification:! gravel: particles > 2mm (boulders, cobbles, pebbles, granules)<br />

! sand: particles between 2 mm and 1/16 mm<br />

! silt: particles between 1/16 mm and 1/256 mm<br />

! clay: particles smaller than 1/256 mm<br />

Gravel and sand are all visible particles. Clay and all but the very coursest silt are<br />

microscopic. Silt and clay are called mud.<br />

sediment size gradation: The size distribution <strong>of</strong> a sediment is determined by passing<br />

a sample through a stack <strong>of</strong> nested baskets with each lower basket having a finer wire<br />

mesh. The size fractions caught in each basket are then weighed. The sediment size<br />

distribution is then plotted on a semi-log grain-size distribution plot. A wide distribution<br />

<strong>of</strong> particle sizes is a poorly sorted sediment. A tight distribution <strong>of</strong> grain sizes is a wellsorted<br />

sediment.<br />

uniformity coefficient, C u is a measure <strong>of</strong> the gradation <strong>of</strong> a sediment. It is<br />

calculated as the following ratio:<br />

C u = d 60 / d 10<br />

d 60 = soil particle diameter at which 60% <strong>of</strong> the mass <strong>of</strong> a soil sample is finer<br />

d 10 = the diameter at which 10% is finer<br />

d 60 and d 10 can be read <strong>of</strong>f a grain-size distribution plot<br />

C u > 6 is well graded (poorly-sorted)<br />

porosity ranges<br />

well-sorted gravel or sand! 25-50% porosity<br />

poorly-sorted gravel and sand! 20-35%<br />

silt or clay! 33-60%<br />

effective porosity<br />

However, not all <strong>of</strong> the water in pore spaces is available (can drain out). Some water is<br />

held by capillary forces (capillary water) and some by electrostatic forces<br />

(hygroscopic water). The available water is called gravitational water because it is<br />

able to drain out <strong>of</strong> the rock under the force <strong>of</strong> gravity.<br />

The effective porosity is less than the total porosity because <strong>of</strong> these forces that retain<br />

water in the pores spaces.


The term specific yield (Sy) is another term for effective porosity, but is commonly used<br />

when referring to an aquifer rather than individual samples.<br />

Specific retention (Sr) refers to the portion <strong>of</strong> the total porosity that is not available due<br />

to capillary and electrostatic forces.<br />

porosity = specific yield + specific retention<br />

η = S y + S r<br />

Fine sediments like clay and silt have a high porosity but also a high specific retention<br />

and low specific yield. Capillary and electrostatic forces become very important in fine<br />

sediments where the pores spaces are very small. Clay minerals have electrostatic<br />

forces that attract large amounts <strong>of</strong> water (dipolar molecule).<br />

Coarse sediments like sand and gravel have a lower porosity than fine sediments but<br />

high specific yield and low specific retention because the void spaces are larger and<br />

electrostatic attractions are much less. A much smaller proportion <strong>of</strong> water in voids is in<br />

close contact to the grains. Coarse and medium sand generally has the greatest<br />

specific yield because the void spaces are still relatively large, but they have greater<br />

porosity than gravel (cobbles & boulders).<br />

determination <strong>of</strong> effective porosity/specific yield<br />

For a saturated sediment or rock sample, the effective porosity can be determined as:<br />

which is<br />

η e<br />

=<br />

void volume saturated weight − drained weight<br />

×<br />

total volume saturated weight − dried weight<br />

η e<br />

= porosity ×<br />

gravitational water weight<br />

total water weight<br />

Then multiply by 100% to express as a percent.<br />

Knowing the average specific yield in an aquifer and the volume <strong>of</strong> the aquifer, one can<br />

calculate the total amount <strong>of</strong> water held in storage that could be extracted. Weʼll see<br />

that later.


II) Groundwater Ease <strong>of</strong> Flow (<strong>Permeability</strong> - Hydraulic Conductivity (k), etc.)<br />

Darcy's Law<br />

Darcy (1856) reported on experiments comparing the rate <strong>of</strong> flow <strong>of</strong> water through sand<br />

(used for water filtration). He varied the slope (head loss over a certain length) <strong>of</strong><br />

various sizes <strong>of</strong> sand packed in a cylinder.<br />

Darcy determined that in a permeable medium, the flow velocity is:<br />

- directly proportional to the head loss<br />

- inversely proportional to the length (distance)<br />

V d<br />

∝ H L<br />

where Vd is the Darcy velocity, H is the head loss or difference in the height <strong>of</strong> the water<br />

table or potentiometric surface, and L is the length or distance between observation<br />

points. This is the "rise over the run" or the slope <strong>of</strong> the water table or potentiometric<br />

surface. This slope is also known as the hydraulic gradient. So the groundwater flow<br />

velocity is proportional to the slope <strong>of</strong> the water table or potentiometric surface.<br />

The constant <strong>of</strong> proportionality is called the hydraulic conductivity (K), which is<br />

analogous to the permeability.<br />

V d<br />

= K H L<br />

Darcy Velocity = (hydraulic conductivity) (hydraulic gradient)<br />

Note on groundwater velocity: Because not all <strong>of</strong> the groundwater is flowing (some is<br />

held by capillary and electrostatic forces) the true velocity (Vt) or seepage velocity is<br />

greater than the Darcy velocity (Vd). The true velocity is equal to the Darcy velocity<br />

divided by the effective porosity<br />

V t = V d / η e<br />

Additionally, groundwater does not flow in straight paths but rather flows around grains<br />

through connected void spaces. The velocity <strong>of</strong> the individual water molecules in their<br />

sinuous paths is faster yet. A complete treatment <strong>of</strong> Vt would ideally include the<br />

sinuosity, but the sinuosity is difficult to quantify.


The hydraulic conductivity has units <strong>of</strong> distance per time (like velocity). The hydraulic<br />

gradient is a ratio and has no units (length divided by length cancels units).<br />

Since the discharge (Q; volume <strong>of</strong> water flowing through a medium in a given amount<br />

<strong>of</strong> time) is equal to the flow velocity times the cross sectional area through which it flows<br />

(Q = VA), Darcy's Law becomes:<br />

Q = KA H L<br />

discharge = (hydraulic conductivity) (cross-sectional area) (hydraulic gradient)<br />

fluid properties effect on discharge: The rate <strong>of</strong> flow depends not just on the<br />

properties <strong>of</strong> the permeable media, but also the properties <strong>of</strong> the fluid. Flow depends<br />

on the specific gravity (density) and viscosity (resistance to flow) <strong>of</strong> the fluid. The<br />

density and the viscosity <strong>of</strong> water both increase with increasing temperature (aside<br />

from the density peak for water at 4 °C).<br />

Petroleum, another common fluid that flows through permeable media, is more viscous<br />

than water.<br />

intrinsic permeability: Since the hydraulic conductivity (K) in Darcyʼs Law depends<br />

not only on the properties <strong>of</strong> the porous media but also <strong>of</strong> the viscous fluid, another<br />

measure is needed to define the properties <strong>of</strong> the media alone.<br />

Factoring out the characteristics <strong>of</strong> the fluid (specific gravity and viscosity) one can<br />

define a property <strong>of</strong> the permeable media alone.<br />

intrinsic permeability,<br />

K i<br />

= K µ γ<br />

where μ (mu) is the fluidʼs viscosity; γ (gamma) is the fluidʼs specific gravity<br />

It has been shown that for sandy sediments (d 10 between 0.1 and 3 mm)<br />

intrinsic permeability, K i = Cd 2 10<br />

where C and d 10 relate to the shape and size <strong>of</strong> the pore spaces<br />

C is the shape coefficient; d 10 is the characteristic grain size<br />

and more generally, K i = Cd j 50<br />

where C is the shape coefficient; d 50 is the mean grain size;<br />

j is an exponent


permeability increases as the size <strong>of</strong> sediments (size <strong>of</strong> void spaces) increases<br />

permeability decreases as the degree <strong>of</strong> sorting decreases<br />

(and smaller particles fill spaces between larger particles)<br />

coarse sediments have lower porosity (less proportional void space)<br />

but higher permeability (larger voids - easier flow)<br />

fine sediments have higher porosity<br />

but lower permeability<br />

measuring permeability: permeameters<br />

the rate that water will flow through porous materials (hydraulic conductivity) can be<br />

determined by measuring the discharge <strong>of</strong> water through a sample <strong>of</strong> known<br />

diameter with the water supply at a known hydraulic head (constant or decreasing)<br />

constant head permeameters are used for high hydraulic conductivity samples<br />

falling head permeameters are used for low hydraulic conductivity samples

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