groundwater 1 groundwater flows slowly through the voids between grains or the cracks in solid rock....

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Groundwater 1 Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory observations. Here, for example, is an experiment to measure head loss in an aquifer.

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Page 1: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

Groundwater 1Groundwater 1

Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory observations. Here, for example, is an experiment to measure head loss in an aquifer.

Page 2: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

Darcy’s Law• Henri Darcy established empirically that the energy

lost ∆h in water flowing through a permeable formation is proportional to the length of the sediment column ∆L.

• The constant of proportionality K is called the hydraulic conductivity . The Darcy Velocity VD:

VD = – K (∆h/∆L)

and since Q = VD A ( where A = total area) Q = – KA (dh/dL)

Page 3: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

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Darcy’s ExperimentDarcy’s Experiment

2. Head difference doesn’t change with inclination of the sand filter

3. Again, Darcy related reduced flow rate to head loss and length of column through a constant of proportionality K,V = Q/A = -K dh / dL

1. Velocities small, V ~ 0, so:

Piezometers before and after sand. Pipe is full, so

flow rate is constant

Page 4: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

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L 0.58 mdiam. 0.35 mn 0.38

A 0.096211 m2

CalcExperiment Duration Q dp Ratio K K

No. (min) L/min (m) V/dp (m/min) cm/s1 25 3.6 1.11 3.25 0.019552 3.26E-022 20 7.65 2.36 3.24 0.019541 3.26E-023 15 12 4 3 0.018085 3.01E-024 18 14.28 4.9 2.91 0.017568 2.93E-025 17 15.2 5.02 3.03 0.018253 3.04E-026 17 21.8 7.63 2.86 0.017224 2.87E-027 11 23.41 8.13 2.88 0.017359 2.89E-028 15 24.5 8.58 2.85 0.017214 2.87E-029 13 27.8 9.86 2.82 0.016997 2.83E-0210 10 29.4 10.89 2.7 0.016275 2.71E-02

Darcy’s Data (One set of 10 experiments)

1.Darcy collected data with his apparatus, then …

Page 5: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

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Plotted it. Note the strong coefficient of determination R2 .

Page 6: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

Darcy’s allows an estimate of:

• The velocity or flow rate moving within the aquiferThe velocity or flow rate moving within the aquifer• The average time of travel from the head of the aquifer to a The average time of travel from the head of the aquifer to a point located downstreampoint located downstream• Very important for prediction of contaminant plume arrivalVery important for prediction of contaminant plume arrival

Confined Aquifer

Page 7: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

Darcy & Seepage Velocity

• Darcy velocity VD is a fictitious velocity since it assumes that flow occurs across the entire cross-section of the sediment sample. Flow actually takes place only through interconnected pore channels (voids), at the seepage velocity VS.

A = total areaAv voids

Page 8: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

Darcy & Seepage Velocities

• From the Continuity Eqn. Q = constant• “Pipe running full” means “Inputs = Outputs”

• Q = A VD = AV Vs

– Where: Q = flow rate A = total cross-sectional area of        material

AV = area of voids Vs =

seepage velocity VD = Darcy velocity

Since A > AV , and Q = constant, Vs > VD

Pinch hose, reduce area, water goes faster

Page 9: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

Darcy & Seepage Velocity: Porosity

• Q = A VD = AV Vs ,therefore VS = VD ( A/AV)

• Multiplying both sides by the length of the medium (L) divided by itself, L / L = 1

• VS = VD ( AL / AVL ) = VD ( VolT / VolV ) we get volumes

• Where:VolT = total volume

VolV = void volume

• By definition, Volv / VolT = n, the sediment

porosity

So the actual velocity: VS = VD / n

Page 10: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

Turbulence and Reynolds Number• The path a water molecule takes is called a streamline.

In laminar flow, streamlines do not cross, and the viscous forces due to hydrogen bonds are important.

• In turbulent flow acceleration and large scale motion away from a smooth path is important (this is the familiar inertial force F = ma) and streamlines cross.

• We could take the ratio of inertial to viscous forces. When this number is “large,” inertial forces are more important, and flows are turbulent.

• This ratio is known as the Reynolds number Re:

Page 11: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

Viscosity• Viscosity is a fluid’s resistance to flow.

• Dynamic viscosity , units Pa·s = N·s/m2, or kg/(m·s)is determined experimentally. If a fluid with a viscosity of one Pa·s is placed between two plates, and one plate is pushed sideways with a shear stress of one Pascal, it moves a distance equal to the thickness of the layer between the plates in one second.

• Kinematic viscosity , is the dynamic viscosity divided by the density. The SI unit of ν is m2/s.

Page 12: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

Recall the ratio of Kinetic/Potential Energy (KE/PE) is the Froude Number FrFr = V / sqrt( g L) we saw last time.

Reynolds: Inertial/Viscous forces

Page 13: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

Limitations of Darcy’s Equation

1. For Reynold’s Number, Re, > 10 or where the flow is turbulent, as in the immediate vicinity of pumped wells.

2. Where water flows through extremely fine-grained materials (colloidal clay)

Q = – KA (dh/dL) q = – Ky (dh/dL)

Darcy’s Law works Darcy’s Law works for 1.0 < Re < 10for 1.0 < Re < 10

Page 14: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

Example 1

• A confined aquifer has a source of recharge.

• K for the aquifer is 50 m/day, and porosity n is 0.2.

• The piezometric head in two wells 1000 m apart is

55 m and 50 m respectively, from a common datum.

• The average thickness of the aquifer is 30 m, and

the average width of the aquifer is 5 km = 5000m.

Q = KA (dh/dL)The hydraulic conductivityK is a velocity, length / time

and n = Vol voids/ Vol total

A piezometer is a small-diameter observation well used to measure the piezometric head of groundwater in aquifers. Piezometric head is measured as a water surface elevation, expressed in units of length.

Page 15: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

Example 1 Compute:• a) the rate of flow through the aquifer• (b) the average time of travel from the head of the

aquifer to a point 4 km downstream

Q = KA (dh/dL)

Page 16: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

Example 1 Solution

• Cross-Sectional area= 30(5000) = 1.5 x 105 m2

• Hydraulic gradient dh/dL= (55-50)/1000 = 5 x 10-3

• Find Rate of Flow for K = 50 m/day

Q = (50 m/day) (1.5 x 105 m2) ( 5 x 10-3)

Q = 37,500 m3/day • Darcy Velocity: V = Q/A • = (37,500m3/day) / (1.5 x 105 m2) = 0.25m/day

Q = KA (dh/dL)

Page 17: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

And • Seepage Velocity: Vs = VD/n = (0.25) / (0.2) =

1.25 m/day (about 4.1 ft/day)

• Time to travel 4 km downstream: T = (4000m) / (1.25m/day) = 3200 days or 8.77 years

• This example shows that water moves very slowly underground.

Lesson: Groundwater moves very slowly

Page 18: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

Example 2

Confining LayerAquifer

30 ft

• A channel runs almost parallel to a river, and they are 2000 ft apart.

• The water level in the river is at an elevation of 120 ft . The channel is at an elevation of 110ft.

• A pervious formation averaging 30 ft thick and with hydraulic conductivity K of 0.25 ft/hr joins them.

• Determine the flow rate Q of seepage from the river to the channel.

Page 19: Groundwater 1 Groundwater flows slowly through the voids between grains or the cracks in solid rock. Much of our knowledge depends on field and laboratory

Example 2: Confined Aquifer

• Consider 1-ft (i.e. unit) lengths of the river and small channel. Q = KA [(h1 – h2) / L]

• Where:A = (30 x 1) = 30 ft2

K = (0.25 ft/hr) (24 hr/day) = 6 ft/day

• Therefore,Q = [6ft/day (30ft2) (120 – 110ft)] /

2000ft Q = 0.9 ft3/day for each 1-foot length