HONR 297 Environmental Models

Slides:



Advertisements
Similar presentations
Yhd Subsurface Hydrology
Advertisements

Introduction to Environmental Engineering Lecture 15 Water Supply and Groundwater.
28.1 The Hydrologic Cycle Hydrological cycle: natural circulation of water from the oceans to the air, then to the ground, then to the oceans and then.
EXAMPLE 4 Solve a multi-step problem ICE SCULPTURES
Philip B. Bedient Civil & Environmental Engineering Rice University
Water Movement in Soil and Rocks. Two Principles to Remember:
Properties of Aquifers
Groundwater 40x larger than lakes+rivers
tures/water_level.swf In the low permeability case the water is pumped primarily from.
Watershed Hydrology, a Hawaiian Prospective; Groundwater Ali Fares, PhD Evaluation of Natural Resource Management, NREM 600 UHM-CTAHR-NREM.
ESS 454 Hydrogeology Instructor: Michael Brown
8. Permeability (Das, chapter 7)
Geol 220: GROUNDWATER HYDROLOGY Co-Lecturers: Dave Goorahoo and Richard Soppe Lecture 1- Introduction to Hydrology Jan 28, 2002.
Integration Work as an Application. The BIG Question Did you prepare for today? If so, estimate the time you spent preparing and write it down on your.
Ground Water Hydrology Introduction
HONR 297 Environmental Models Chapter 2: Ground Water 2.3: Typical Quantitative Issues.
Soil Water Reading: Applied Hydrology Sections 4.1 and 4.2 Topics
HONR 297 Environmental Models
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.
Lab 10 - Soil Water Movement Flow Model Experiment 1 –Red dye is added to the waste lagoon and to a well in the unconfined aquifer. –Green dye is added.
Soil water flow and Darcy’s Law. Laminar flow in a tube Poiseuille’s Law, ~1840: where: Q = volume of flow per unit time (m 3 s -1 ) r = radius of the.
Objectives Copyright © 2009 Pearson Education, Inc. Publishing as Pearson Addison-Wesley More with Formulas 1. Use the formula P = 2l + 2w to find the.
Lecture Notes Applied Hydrogeology
Figure (p. 235) (a) Cross-section through an unsaturated porous medium; (b) Control volume for development of the continuity equation in an unsaturated.
Ch. 2: Describing Motion: Kinematics in One Dimension.
Example Suppose a firework is launched with an upward velocity of about 80 ft/sec from a height of 224 feet. Its height in feet, h(t), after t seconds.
Darcy’s Law and Flow CIVE Darcy allows an estimate of: the velocity or flow rate moving within the aquifer the average time of travel from the head.
Water Supply and Treatment. Average Precipitation.
Chapter 6 The Definite Integral.  Antidifferentiation  Areas and Riemann Sums  Definite Integrals and the Fundamental Theorem  Areas in the xy-Plane.
Review: 6.5h Mini-Quiz 1.Solve: An object is dropped from a cliff 480 ft above the ground. Find the time t (in sec) for the object to reach the ground.
Dimensional Analysis Part 2 Chapter 2 Section 2 Units of Measurement.
HONR 297 Environmental Models Chapter 3: Air Quality Modeling 3.5: One-Dimensional Diffusion.
Problem Solving in Geometry. Geometry Geometry is about the space you live in and the shapes that surround you. For thousands of years, people have studied.
1.5 Use a Problem Solving Plan Objective: To be able to use a problem solving plan to solve problems Warm-up: 1.Mr. Lu is planting trees around.
SOME NOTES ON MORPHODYNAMIC MODELING OF VENICE LAGOON Gary Parker, Spring, 2004 Venice Lagoon was formed by the action of deposition of mud and sand from.
Copyright © Cengage Learning. All rights reserved.
THE HYDROLOGIC CYCLE 2: GROUNDWATER. The Hydrologic Cycle - Fresh Water Storage Reservoir % of Total Fresh Water Glaciers (Frozen)76% Groundwater22% Rivers.
HONR 297 Environmental Models Chapter 3: Air Quality Modeling 3.6: Two-Dimensional Diffusion.
Chapter 34 Water On Our World. Hydrologic Cycle.
The Derivative Objective: We will explore tangent lines, velocity, and general rates of change and explore their relationships.
1.4 Setting Up Equations; Applications. Verbal Description Language of Math Mathematical Problem Solution Real Problem.
The Prototype Plume Busters Software: A New Tool for Computer Assisted Instruction P. Allen Macfarlane, Geoffery Bohling, Margaret Townsend Kansas Geological.
Lecture 20 Ground Water (3) Ground water movement
Darcy’s Law Philip B. Bedient Civil and Environmental Engineering Rice University.
CE 3354 Engineering Hydrology Lecture 21: Groundwater Hydrology Concepts – Part 1 1.
HONR 297 Environmental Models
HONR 297 Environmental Models
Soil Physics David Zumr room: b608 Lecture (and seminar) notes will be available: -
Chapter 5 Section 4. EXAMPLE 1 Find a common monomial factor Factor the polynomial completely. a. x 3 + 2x 2 – 15x Factor common monomial. = x(x + 5)(x.
PreCalculus 10-R Unit 10 – Trigonometric Applications Review Problems.
Soil Water Balance Reading: Applied Hydrology Sections 4.3 and 4.4
1 Permeability. 2 Soil Permeability- Definition It is a property of soil that allows the flow of fluid through its interconnected void space OR It is.
Properties of Aquifers
Chapter1:Static pressure in soil due to water.
Groundwater Review Aquifers and Groundwater Porosity
EXAMPLE 4 Solve a multi-step problem ICE SCULPTURES
Lecture 20 Ground Water (3) Ground water movement
Some Quiz Questions Unit: Subsurface Flow.
Find: y1 Q=400 [gpm] 44 Sand y2 y1 r1 r2 unconfined Q
28.1 The Hydrologic Cycle Hydrological cycle: natural circulation of water from the oceans to the air, then to the ground, then to the oceans and then.
Philip B. Bedient Civil and Environmental Engineering Rice University
Find: c(x,t) [mg/L] of chloride
PERMEABILITY . Some slides in this section are from NExT PERF Short Course Notes, Some slides appear to have been obtained from unknown primary sources.
PERMEABILITY . Some slides in this section are from NExT PERF Short Course Notes, Some slides appear to have been obtained from unknown primary sources.
Some Quiz Questions Unit: Subsurface Flow.
Find: hmax [m] L hmax h1 h2 L = 525 [m]
Chapter 6 The Definite Integral
Chapter 11 Fluids.
Philip B. Bedient Civil and Environmental Engineering Rice University
Presentation transcript:

HONR 297 Environmental Models Chapter 2: Ground Water 2.5: The Interstitial Velocity Equation

What we Know so Far Recall that we are trying to answer two general questions related to ground water flow. How much water flows through an aquifer? The velocity of water in the aquifer. So far, we’ve seen how to answer the first question via Darcy’s Law. For the second question, let’s consider some “experiments”!

Experimental Set-up Side View End View 1 m Ground Water Flow Direction In the experiments that follow, we will use the set-up above as our base case. The tube through which ground water flows will have a square cross section, with dimensions 1 m by 1 m, with cross-sectional area one square meter. For the end view, we are looking at water flowing out at us!

Experiment 1 Side View End View 1 m Ground Water Flow Direction 10 m Suppose water is flowing through the tube at a rate of ten cubic meters per minute. Then the total amount of water in a ten-meter long piece of tube would have to flow out of the right end in one minute. Question: What would the water’s speed (or velocity) need to be for this to be accomplished? Answer: The water would have to be moving at a speed of 10 m/min.

Experiment 2 Side View End View 1 m 20 m Suppose water is flowing through the tube at a rate of ten cubic meters per minute, but half of the original flow pathway has been blocked. Now, the total amount of water in a 20-meter long piece of tube would have to flow out of the right end in one minute. Question: What would the water’s speed (or velocity) need to be for this to be accomplished? Answer: The water would have to be moving at a speed of 20 m/min.

Experiment 3 Side View End View 1 m 20 m Suppose instead of the half of the original flow pathway being blocked, as in the second experiment, now we fill the tube with geologic material (such as gravel or sand). If the open spaces or voids in the tube comprise 50 percent of the available open space, then again half of the pathway will be blocked. Thus, if water is flowing through the tube at a rate of ten cubic meters per minute, we are in essentially the same situation as in the second experiment! Again, the total amount of water in a 20-meter long piece of tube would have to flow out of the right end in one minute, so the water’s velocity would have to be 20 m/min. Here, we are talking about net flow of all of the water in the flow direction – due to the gravel or sand, some of the water droplets may not move to the right in straight lines, so they’d have to actually be moving faster, as all the water in the 20-foot piece of tube must make it out in 1 minute!

Porosity Definition The porosity of a geologic material is the fraction of the bulk volume that is actually open spaces or voids. We denote porosity with the Greek letter eta (η). Note: Examples of open spaces or voids include spaces between particles in soil or open fractures in solid rock. The geologic material in Experiment 3 would have porosity 50% or 0.5. Typical porosity values are shown in Table 2.1 in our text, p. 26.

Experiment 4 Suppose we put sand in the tube with a porosity of 0.25. Side View End View 1 m 32 m Suppose we put sand in the tube with a porosity of 0.25. Question: What would the water’s velocity need to be if the flow rate is measured to be 8 m^3/min? Answer: In order to get 8 cubic meters of water in the tube’s open spaces, since only 25% of the tube has open space, we’d need the tube’s length to be 4*8 = 32 m. It follows that the water’s velocity would need to be 32 m/min.

Fluid Velocity Looking at the examples above, we see that in order to determine fluid velocity in an aquifer, all we need to do is look at the volumetric flow rate per unit cross- sectional area (for example, one square meter) and divide by the porosity. Check that this works in each case above!

Flux Definition From Darcy’s Law, flux is given by The volumetric fluid flow rate per unit cross-sectional area is known as flux and denoted q. From Darcy’s Law, flux is given by q = Q/A = (K i A)/A = K i. (1) Note that units of flux q are [q] = (length^3 per time) per length^2 which reduce to length/time … (check!). It follows from (1) and our experimental examples that the velocity of ground water in an aquifer is given by ν = q/η = K i /η. (2)

Interstitial Velocity Equation Definition: The interstitial velocity equation is ν = (K i)/η where ν = the effective fluid velocity along the axis of the flow pathway; K = the hydraulic conductivity of the aquifer material; η = the porosity of the medium.

Example 1 Note that to compute interstitial velocity, all we need to know about an aquifer are its hydraulic gradient (which depends on measurements taken from the aquifer via monitoring wells) and its hydraulic conductivity and porosity, which depend on the aquifer’s material make-up. Recall Example 1 from the section on Darcy’s Law where we found the volumetric flow rate for an aquifer – let’s try to find the velocity of the ground water in this aquifer, assuming that the aquifer’s porosity is 40%.

Example 1 Example 1 (from Darcy’s Law Notes): Imagine an underground sand aquifer that is 40 feet thick, 200 feet wide, and has a hydraulic conductivity of 25 ft/day. Two test wells 750 feet apart are drilled into the aquifer, along the axis of flow, and the measured head values at these wells were found to be 120 and 114 feet, respectively. Solution: From this information, we see that K = 25 ft/day i = Δh/L = (120 ft -114 ft)/750 ft = (6 ft)/(750 ft) η = 0.40 Thus, ν = K i/ η = = ((25 ft/day)(6 ft)/(750 ft))/(0.40) = 0.5 ft/day

Example 2 Since velocity = distance/time, it follows that time = distance/velocity. Thus if we know the interstitial velocity of an aquifer’s ground water, we can figure out how long it takes for the ground water to travel a given distance! For example, the ground water in the Example 1 aquifer will travel 2 miles in ((2 miles)/(0.5 ft/day))(5280 ft/mile) = 21,120 days = (21,120 days)/(365 days/yr) ≈ 58 years

Homework Read Sections 2.5 and 2.6 in Hadlock.

References Charles Hadlock, Mathematical Modeling in the Environment, Chapter 2, Section 5.