27.11.2014 Views

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 ...

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

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

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!