Darcy law Figure from Hornberger et al.

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Darcy law Darcy law

Figure from Hornberger et al. (1998) Generalization of Darcy’s column  h/L = hydraulic  Figure from Hornberger et al. (1998) Generalization of Darcy’s column h/L = hydraulic gradient q = Q/AQ is proportional to h/L

Figure from Hornberger et al. (1998)Darcy’s data for two different sands Figure from Hornberger et al. (1998)Darcy’s data for two different sands

Darcy’s Law • Henri Darcy established empirically that the flux of water through a permeable formationDarcy’s Law • Henri Darcy established empirically that the flux of water through a permeable formation is proportional to the distance between top and bottom of the soil column. • The constant of proportionality is called the hydraulic conductivity (K). • V = Q/A, V – ∆h, and V 1/∆L

 V = – K (∆h/∆L)  and since  Q = VA (A = total V = – K (∆h/∆L) and since Q = VA (A = total area) Q = – KA (dh/d. L)Darcy’s Law

Hydraulic Conductivity • K represents a measure of the ability for flow through porous media: Hydraulic Conductivity • K represents a measure of the ability for flow through porous media: • Gravels — 0. 1 to 1 cm/sec • Sands — 10 -2 to 10 -3 cm/sec • Silts — 10 -4 to 10 -5 cm/sec • Clays — 10 -7 to 10 -9 cm/sec

Figure from Hornberger et al. (1998)Range in hydraulic conductivity, K 13 orders of magnitude Figure from Hornberger et al. (1998)Range in hydraulic conductivity, K 13 orders of magnitude

Conditions • Darcy’s Law holds for: 1.  Saturated flow and unsaturated flow 2.  Steady-stateConditions • Darcy’s Law holds for: 1. Saturated flow and unsaturated flow 2. Steady-state and transient flow 3. Flow in aquifers and aquitards 4. Flow in homogeneous and heterogeneous systems 5. Flow in isotropic or anisotropic media 6. Flow in rocks and granular media

Darcy Velocity • V is the specific discharge ( Darcy velocity).  • (–) indicates thatDarcy Velocity • V is the specific discharge ( Darcy velocity). • (–) indicates that V occurs in the direction of the decreasing head. • Specific discharge has units of velocity. • The specific discharge is a macroscopic concept, and is easily measured. It should be noted that Darcy’s velocity is different ….

Darcy Velocity • . . . from the microscopic velocities associated with the actual paths ifDarcy Velocity • . . . from the microscopic velocities associated with the actual paths if individual particles of water as they wind their way through the grains of sand. • The microscopic velocities are real, but are probably impossible to measure.

Darcy & Seepage Velocity • Darcy velocity is a fictitious velocity since it assumes that flowDarcy & Seepage Velocity • Darcy velocity is a fictitious velocity since it assumes that flow occurs across the entire cross-section of the soil sample. Flow actually takes place only through interconnected pore channels. A = total area. A v voids

Darcy & Seepage Velocity • From the Continuity Eqn:  • Q = A v DDarcy & Seepage Velocity • From the Continuity Eqn: • Q = A v D = A V V s – Where: Q = flow rate A = total cross-sectional area of material AV = area of voids V s = seepage velocity V D = Darcy velocity

Darcy & Seepage Velocity • Therefore:  VS = VD ( A/AV ) • Multiplying bothDarcy & Seepage Velocity • Therefore: VS = VD ( A/AV ) • Multiplying both sides by the length of the medium ( L ) V S = VD ( AL / AV L ) = VD ( VT / VV ) • Where: V T = total volume V V = void volume • By Definition, V v / VT = n , the soil porosity • Thus V S = VD / n

q is a vector q xz q x  1 q z  2 z xzq is a vector q xz q x 1 q z 2 z xz h Kq y h Kq x h Kq zz yy xx q = Q/A In general: K z < K x , K y

z h Kq y h Kq x h Kq zz yy xx   q =z h Kq y h Kq x h Kq zz yy xx q = — K grad h

Vector Form of Darcy’s Law q = - K grad h q = specific discharge (L/T)Vector Form of Darcy’s Law q = — K grad h q = specific discharge (L/T) K = hydraulic conductivity (L/T) grad h = hydraulic gradient (L/L) h = head (L)

q = - K  grad h K is a tensor with 9 components (three ofq = — K grad h K is a tensor with 9 components (three of which are K x , K y , K z )q is a vector with 3 components h is a scalar

Scalar 1 component Magnitude Head , concentration,  temperature Vector 3 components Magnitude and direction SpecificScalar 1 component Magnitude Head , concentration, temperature Vector 3 components Magnitude and direction Specific discharge , (& velocity), mass flux, heat flux Tensor 9 components Magnitude, direction and magnitude changing with direction Hydraulic conductivity , Dispersion coefficient, thermal conductivity

q = - K  grad h. Darcy’s law grad hq equipotential line grad hq Isotropicq = — K grad h. Darcy’s law grad hq equipotential line grad hq Isotropic Kx = Ky = Kz = K Anisotropic Kx, Ky, Kz

Equations of Groundwater Flow • Description of ground water flow is based on: Darcy’s Law ContinuityEquations of Groundwater Flow • Description of ground water flow is based on: Darcy’s Law Continuity Equation — describes conservation of fluid mass during flow through a porous medium; results in a partial differential equation of flow. • Laplace’s Eqn — most important in math

Derivation of 3 -D GW Flow Equation from Darcy’s Law  x Vx y Vy zDerivation of 3 -D GW Flow Equation from Darcy’s Law x Vx y Vy z Vz 0 Mass In — Mass Out = Change in Storage Vx x Vx Vx z y

Derivation of 3 -D GW Flow Equation from Darcy’s Law  x Kx h x Derivation of 3 -D GW Flow Equation from Darcy’s Law x Kx h x y Ky h y z Kz h z 0 Replace V x , Vy , and Vz with Darcy using Kx , Ky , and Kz Divide out constant , and assume K x = K y = K z = K 2 h x 2 2 h y 2 2 h z 20 2 h 0 called. Laplace. Eqn.

Transient Saturated Flow  x Kx h x  y Ky h y  z KzTransient Saturated Flow x Kx h x y Ky h y z Kz h z Ss h t x Vx y Vy z Vz t n A change in h will produce change in and n, replaced with specific storage S s = g( + n ). Note, is the compressibility of aquifer and B is comp of water, therefore,

Transient Saturated Flow  x h x  y h y  z h z Transient Saturated Flow x h x y h y z h z Ss K h t Simplifying by assuming K = constant in all dimensions And assuming that S = S s b , and that T = Kb yields 2 h x 2 2 h y 2 2 h z 2 Ss K h t 2 h S T h t from. Jacob, Theis

Steady State Flow to Well Simplifying by assuming K = constant in all dimensions and assumingSteady State Flow to Well Simplifying by assuming K = constant in all dimensions and assuming that Transmissivity T = Kb and Q = flow rate to well at point (x, y) yields 2 h x 2 2 h y 2 Qx, y T

Example of Darcy’s Law • A confined aquifer has a source of recharge.  • KExample of Darcy’s Law • A confined aquifer has a source of recharge. • K for the aquifer is 50 m/day , and 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 aquifer is 5 km.

Compute:  • a) the rate of flow through the aquifer • (b) the average timeCompute: • 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 • *assume no dispersion or diffusion

The solution • Cross-Sectional area= 30(5)(1000) = 15 x 10 4 m 2 • Hydraulic gradientThe solution • Cross-Sectional area= 30(5)(1000) = 15 x 10 4 m 2 • Hydraulic gradient = (55 -50)/1000 = 5 x 10 -3 • Rate of Flow for K = 50 m/day Q = (50 m/day) (75 x 10 1 m 2 ) = 37, 500 m 3 /day • Darcy Velocity: V = Q/A = (37, 500 m 3 /day) / (15 x 10 4 m 2 ) = 0. 25 m/day

And • Seepage Velocity:     Vs = V/n = (0. 25) / (0.And • Seepage Velocity: Vs = V/n = (0. 25) / (0. 2) = 1. 25 m/day (about 4. 1 ft/day) • Time to travel 4 km downstream: T = 4(1000 m) / (1. 25 m/day) = 3200 days or 8. 77 years • This example shows that water moves very slowly underground.

Limitations of the Darcian Approach 1. For Reynold’s Number, Re,  10 or where the flowLimitations of the Darcian Approach 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)

Darcy’s Law: Example 2 • A channel runs almost parallel to a river, and they areDarcy’s Law: Example 2 • 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 and 110 ft in the channel. • A pervious formation averaging 30 ft thick and with K of 0. 25 ft/hr joins them. • Determine the rate of seepage or flow from the river to the channel.

Confined Aquifer Confining Layer Aquifer 30 ft Confined Aquifer Confining Layer Aquifer 30 ft

Example 2 • Consider a 1 -ft length of river (and channel). Q = KA [(hExample 2 • Consider a 1 -ft length of river (and channel). Q = KA [(h 1 – h 2 ) / L] • Where: A = (30 x 1) = 30 ft 2 K = (0. 25 ft/hr) (24 hr/day) = 6 ft/day • Therefore, Q = [6 (30) (120 – 110)] / 2000 = 0. 9 ft 3 /day/ft length = 0. 9 ft 2 /day

Permeameters Constant Head Falling Head Permeameters Constant Head Falling Head

Constant head Permeameter • Apply Darcy’s Law to find K: V/t = Q = KA(h/L) or:Constant head Permeameter • Apply Darcy’s Law to find K: V/t = Q = KA(h/L) or: K = (VL) / (Ath) • Where: V = volume flowing in time t A = cross-sectional area of the sample L = length of sample h = constant head • t = time of flow