water movement in soil and rocks. two principles to remember:
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Water Movement in Soil and Rocks
Water Movement in Soil and Rocks
Two Principles to Remember:
Water Movement in Soil and Rocks
1. Darcy’s Law
Two Principles to Remember:
Water Movement in Soil and Rocks
1. Darcy’s Law
2. Continuity Equation:mass in = mass out + change in storage
Two Principles to Remember:
“my name’s Bubba!”
Water Movement in Soil and Rocks
I. Critical in Engineering and Environmental GeologyA. Dams, Reservoirs, Levees, etc.
“ Pore Pressure”
Water Movement in Soil and Rocks
I. Critical in Engineering and Environmental GeologyA. Dams, Reservoirs, Levees, etc.B. Groundwater Contamination
Landfills Leaking UndergroundStorage Tanks
SurfaceSpills
Water Movement in Soil and Rocks
I. Critical in Engineering and Environmental GeologyA. Dams, Reservoirs, Levees, etc.B. Groundwater ContaminationC. Foundations
- Strength and Stability
I. Critical in Engineering and Environmental GeologyA. Dams, Reservoirs, Levees, etc.B. Groundwater ContaminationC. Foundations
- Strength and Stability
II. Water Flow in a Porous Medium
A. Goal: Determine the permeability of the
engineering material
II. Water Flow in a Porous Medium
A. Goal: Determine the permeability of the
engineering material
Porosity Permeability
II. Water Flow in a Porous Medium
A. Goal: Determine the permeability of the
engineering material
Porosity PermeabilityPermeability (def) the ease at which water can move through rock or soil
Porosity (def) % of total rock that isoccupied by voids.
II. Water Flow in a Porous Medium
B. The Bernoulli EquationA Demonstration:
II. Water Flow in a Porous Medium
B. The Bernoulli EquationA Demonstration:
Bernoulli's Principle states that as the speed of a moving fluid increases, the pressure within the fluid decreases.
II. Water Flow in a Porous Medium
B. The Bernoulli Equation
1. Components of Bernoulli
Total Energy = velocity energy + potential energy + pressure energy
II. Water Flow in a Porous Medium
B. The Bernoulli Equation
1. Components of Bernoulli
Total Energy = velocity energy + potential energy + pressure energy
Total Head = velocity head + elevation head + pressure head
II. Water Flow in a Porous Medium
B. The Bernoulli Equation
1. Components of Bernoulli
Total Energy = velocity energy + potential energy + pressure energy
Total Head = velocity head + elevation head + pressure head
h = v2/2g + z + P/ρg
Where: h = total hydraulic head (units of length)v = velocityg = gravitational constantz = elevation above some datumP = pressure (where P = ρg*Δh) ρ = fluid density
II. Water Flow in a Porous Medium
B. The Bernoulli Equation
1. Components of Bernoulli
Total Energy = velocity energy + potential energy + pressure energy
Total Head = velocity head + elevation head + pressure head
h = v2/2g + z + P/ρg
Where: h = total hydraulic head (units of length)v = velocityg = gravitational constantz = elevation above some datumP = pressure (where P = ρg*Δh) ρ = fluid density
A quick problem……
At a place where g = 9.80 m/s2, the fluid pressure is 1500 N/m2, the distance above a reference elevation is 0.75 m, and the fluid density is 1.02 103 kg/m3. The fluid is moving at a velocity of 1* 10-6 m/s. Find the hydraulic head at this point.
h= v2/2g + z + P/g
At a place where g = 9.80 m/s2, the fluid pressure is 1500 N/m2, the distance above a reference elevation is 0.75 m, and the fluid density is 1.02 103 kg/m3 . The fluid is moving at a velocity of 1* 10-6 m/s. Find the hydraulic head at this point.
h= v2/2g + z + P/g
(1*10-6 m/s)2 + +0.75 m + 1500 {(kg-m)/s2}m2
2 * 9.80 m/s2 9.80 m/s2 * 1.02 103 kg/m3
At a place where g = 9.80 m/s2, the fluid pressure is 1500 N/m2, the distance above a reference elevation is 0.75 m, and the fluid density is 1.02 103 kg/m3 . The fluid is moving at a velocity of 1* 10-6 m/s. Gravity is 9.8 m/s2.Find the hydraulic head at this point.
h= v2/2g + z + P/g
(1*10-6 m/s)2 + +0.75 m + 1500 {(kg-m)/s2}m2
2 * 9.80 m/s2 9.80 m/s2 * 1.02 103 kg/m3
5.10 * 10-14 m + 0.75 m + 0.15 m = 0.90 m = hydraulic head
II. Water Flow in a Porous Medium
B. The Bernoulli Equation
1. Components of Bernoulli
Total Energy = velocity energy + potential energy + pressure energy
Total Head = velocity head + elevation head + pressure head
h = v2/2g + z + P/ρg Total Head = velocity head + elevation head + pressure head h = zero + z + Ψ
Where: h = total hydraulic headz = elevation headΨ = pressure head
II. Water Flow in a Porous Medium
C. Darcy‘s LawHenri Darcy (1856)
Developed an empirical relationship of the discharge of water through porous mediums.
II. Water Flow in a Porous Medium
C. Darcy‘s Law
1. The experiment
K
II. Water Flow in a Porous MediumC. Darcy‘s Law
2. The results• unit discharge α permeability• unit discharge α head loss• unit discharge α hydraulic gradient
Also…..
II. Water Flow in a Porous MediumC. Darcy‘s Law
2. The equation
v = Ki
II. Water Flow in a Porous MediumC. Darcy‘s Law
2. The equation
v = Kiwhere v = specific discharge (discharge per cross sectional area) (L/T) * also called the Darcy Velocity * function of the porous medium and
fluid
Darcy’s Law:
v = Ki
where v = specific discharge (discharge per unit area) (L/T)
K = hydraulic conductivity (L/T); also referred
to as coefficient of permeability
i = hydraulic gradient, where
i = dh/dl (unitless variable)
Darcy’s Law:
v = Ki
where v = specific discharge (discharge per unit area) (L/T)
K = hydraulic conductivity (L/T); also referred
to as coefficient of permeability
i = hydraulic gradient, where
i = dh/dl (unitless variable)
Darcy’s Law:
v = Ki
where v = specific discharge (discharge per unit area) (L/T)
K = hydraulic conductivity (L/T); also referred
to as coefficient of permeability
i = hydraulic gradient, where
i = dh/dl (unitless variable)
v = K dh
dl
Darcy’s Law:
v = Ki
where v = specific discharge (discharge per unit area) (L/T)
K = hydraulic conductivity (L/T); also referred
to as coefficient of permeability
i = hydraulic gradient, where
i = dh/dl (unitless variable)
v = K dh
dl
If Q = VA, then
Q = A K dh
dl
Darcy’s Law:
The exposed truth: these are only APPARENT velocities and discharges
Q = A K dh
dl
Vs.
v = K dh
dlQ = VA
Darcy’s Law:
The exposed truth: these are only APPARENT velocities and discharges
QL = A K dh
ne dlvL = K dh
ne dl
Where ne effective porosity VL = ave linear velocity (seepage velocity) QL = ave linear discharge (seepage discharge)
Both of these variablestake into account that not all of the area is available for fluid flow(porosity is less than 100%)
Find the specific discharge and average linear velocity of a pipe filled with sand with the following measurements.
K = 1* 10-4 cm/sdh = 1.0dl = 100Area = 75 cm2
Effective Porosity = 0.22
Find the specific discharge and average linear velocity of a pipe filled with sand with the following measurements.
K = 1* 10-4 cm/sdh = 1.0dl = 100Area = 75 cm2
Effective Porosity = 0.22
VL =-Kdh V =-Kdh nedl dl
V = 1 * 10-6 cm/sec VL = 4.55 * 10-6 cm/sec
How much would it move in one year?4.55 * 10-6 cm * 3.15 * 107 sec * 1 meter = 1.43 meters for VL
sec year 100 cm 0.315 m for V
II. Water Flow in a Porous MediumC. Darcy‘s Law
3. The Limits
Equation assumes ‘Laminar Flow’; which is usually the case for flow through soils.
C. Darcy‘s Law4. Some Representative Values for Hydraulic Conductivity
II. Water Flow in a Porous Medium
D. Laboratory Determination of Permeability
II. Water Flow in a Porous Medium
D. Laboratory Determination of Permeability
1. Constant Head Permeameter
Q = A K dh
dlQ* dl= K
A dh
Example Problem:
Q = A K dh
dlQ* dl= K
A dh
Given: •Soil 6 inches diameter, 8 inches thick.•Hydraulic head = 16 inches•Flow of water = 766 lbs for 4 hrs, 15 minutes•Unit weight of water = 62.4 lbs/ft3
Find the hydraulic conductivity in units of ft per minute
Example Problem:
Q* dl= K
A dh
Example Problem:
Q* dl= K
A dh
II. Water Flow in a Porous Medium
D. Laboratory Determination of Permeability
2. Falling Head Permeameter
More common for fine grained soils
II. Water Flow in a Porous Medium
D. Laboratory Determination of Permeability
2. Falling Head Permeameter
E. Field Methods for Determining Permeability
In one locality: “Perk rates that are less than 15 minutes per inch or greater than 105 are unacceptable measurements. “
E. Field Methods for Determining Permeability
1. Double Ring Infiltrometer
E. Field Methods for Determining Permeability
2. Johnson Permeameter
E. Field Methods for Determining Permeability
1. Slug Test (Bail Test) also referred to as the Hzorslev Method
K = r2 ln(L/R) 2LT0.37
Where:r = radius of wellR = radius of bore holeL = length of screened sectionT0.37 = the time it take for the water level to rise or fall to 37% of the
initial change
Example Problem:
K = r2 ln(L/R) 2LT0.37
Where:r = radius of wellR = radius of bore hole (well casing)L = length of screened sectionT0.37 = the time it take for the water level to rise or fall to 37% of the
initial change
A slug test is performed by injecting water into a piezometer finished in coarse sand. The inside diameter of both the well screen and well casing is 2 inches. The wellscreen is 10 feet in length. The data of the well recovery is shown below. Determine K from this test.
Time since
Injection
(sec) H (ft) h/ho
0 0.88 1.000
1 0.6 0.682
2 0.38 0.432
3 0.21 0.239
4 0.12 0.136
5 0.06 0.068
6 0.04 0.045
7 0.02 0.023
8 0.01 0.011
9 0 0.000
Hzorslev Method
0.01
0.1
1
0 1 2 3 4 5 6 7 8 9 10
Time (s)
h/h
o
0.01
0.1
1
0 1 2 3 4 5 6 7 8 9 10
Time (s)
h/h
oHzorslev Method
Example Problem:
K = r2 ln(L/R) 2LT0.37
Where:r = radius of wellR = radius of bore hole (well casing)L = length of screened sectionT0.37 = the time it take for the water level to rise or fall to 37% of the
initial change
A slug test is performed by injecting water into a piezometer finished in coarse sand. The inside diameter of both the well screen and well casing is 2 inches. The wellscreen is 10 feet in length. The data of the well recovery is shown below. Determine K from this test.
Example Problem:
K = r2 ln(L/R) 2LT0.37
Where:r = radius of wellR = radius of bore hole (well casing)L = length of screened sectionT0.37 = the time it take for the water level to rise or fall to 37% of the
initial change
A slug test is performed by injecting water into a piezometer finished in coarse sand. The inside diameter of both the well screen and well casing is 2 inches. The wellscreen is 10 feet in length. The data of the well recovery is shown below. Determine K from this test.
K = (0.083 ft)2 ln(10 ft/ (0.083 ft) 2(10ft)(2.3 sec)
Example Problem:
K = r2 ln(L/R) 2LT0.37
Where:r = radius of wellR = radius of bore hole (well casing)L = length of screened sectionT0.37 = the time it take for the water level to rise or fall to 37% of the
initial change
A slug test is performed by injecting water into a piezometer finished in coarse sand. The inside diameter of both the well screen and well casing is 2 inches. The wellscreen is 10 feet in length. The data of the well recovery is shown below. Determine K from this test.
K = (0.083 ft)2 ln(10 ft/ (0.083 ft) 2(10ft)(2.3 sec)
K = 7.18 * 10-4 ft/s
K = 62.0 ft/day
E. Field Methods for Determining Permeability
4. Pump Test also referred to as the Thiem Method
K = Q* ln(r1/r2) π(h1
2 – h22)
K = Q* ln(r1/r2) π(h1
2 – h22)
III. Flow Nets
III. Flow Nets
A. Overview• one of the most powerful tools for the analysis
of groundwater flow.• provides a solution to the Continuity Equation
for 2-D, steady state, boundary value problem.
III. Flow Nets
A. Overview• one of the most powerful tools for the analysis
of groundwater flow.• provides a solution to the Continuity Equation
for 2-D, steady state, boundary value problem.
Continuity Equation:mass in = mass out + change in storage
d2h + d2h = 0 gives the rate of change of dx2 dy2 h in 2 dimensions
• Composed of 2 sets of lines– equipotential lines (connect points of equal
hydraulic head)– flow lines (pathways of water as it moves
through the aquifer.
d2h + d2h = 0 gives the rate of change of dx2 dy2 h in 2 dimensions
FLOW NETS
III. Flow Nets
B. To solve, need to know:– have knowledge of the region of flow– boundary conditions along the perimeter of the
region– spatial distribution of hydraulic head in region.
Q’ = Kph f
Where:Q’ = Discharge per unit depth of
flow net (L3/t/L)K = Hydraulic Conductivity (L/t)p = number of flow tubesh = head loss (L)f = number of equipotential drops
Q’ = Kph f
Where:Q’ = Discharge per unit depth of flow net (L3/t/L)K = Hydraulic Conductivity (L/t) = 1 * 10-4 m/sp = number of flow tubesh = head loss (L)f = number of equipotential drops
50 m32 m
Q’ = (1 * 10-4 m/s)(5)(18m) = Kph = 1 * 10-3 m3/s/m thickness 9 f
Where:Q’ = Discharge per unit depth of flow net (L3/t/L)K = Hydraulic Conductivity (L/t) = 1 * 10-4 m/sp = number of flow tubes = 5h = head loss (L) = 18 mf = number of equipotential drops = 9
50 m32 m
Derivations
• These are extra slides in the case you want to see how the equations are created, or derived…..
K = Q* ln(r2/r1) π*(h2
2 – h12)