Flow to Wells – 1 Steady flow to a well in a confined aquifer

Slides:



Advertisements
Similar presentations
Request Dispatching for Cheap Energy Prices in Cloud Data Centers
Advertisements

SpringerLink Training Kit
Luminosity measurements at Hadron Colliders
From Word Embeddings To Document Distances
Choosing a Dental Plan Student Name
Virtual Environments and Computer Graphics
Chương 1: CÁC PHƯƠNG THỨC GIAO DỊCH TRÊN THỊ TRƯỜNG THẾ GIỚI
THỰC TIỄN KINH DOANH TRONG CỘNG ĐỒNG KINH TẾ ASEAN –
D. Phát triển thương hiệu
NHỮNG VẤN ĐỀ NỔI BẬT CỦA NỀN KINH TẾ VIỆT NAM GIAI ĐOẠN
Điều trị chống huyết khối trong tai biến mạch máu não
BÖnh Parkinson PGS.TS.BS NGUYỄN TRỌNG HƯNG BỆNH VIỆN LÃO KHOA TRUNG ƯƠNG TRƯỜNG ĐẠI HỌC Y HÀ NỘI Bác Ninh 2013.
Nasal Cannula X particulate mask
Evolving Architecture for Beyond the Standard Model
HF NOISE FILTERS PERFORMANCE
Electronics for Pedestrians – Passive Components –
Parameterization of Tabulated BRDFs Ian Mallett (me), Cem Yuksel
L-Systems and Affine Transformations
CMSC423: Bioinformatic Algorithms, Databases and Tools
Some aspect concerning the LMDZ dynamical core and its use
Bayesian Confidence Limits and Intervals
实习总结 (Internship Summary)
Current State of Japanese Economy under Negative Interest Rate and Proposed Remedies Naoyuki Yoshino Dean Asian Development Bank Institute Professor Emeritus,
Front End Electronics for SOI Monolithic Pixel Sensor
Face Recognition Monday, February 1, 2016.
Solving Rubik's Cube By: Etai Nativ.
CS284 Paper Presentation Arpad Kovacs
انتقال حرارت 2 خانم خسرویار.
Summer Student Program First results
Theoretical Results on Neutrinos
HERMESでのHard Exclusive生成過程による 核子内クォーク全角運動量についての研究
Wavelet Coherence & Cross-Wavelet Transform
yaSpMV: Yet Another SpMV Framework on GPUs
Creating Synthetic Microdata for Higher Educational Use in Japan: Reproduction of Distribution Type based on the Descriptive Statistics Kiyomi Shirakawa.
MOCLA02 Design of a Compact L-­band Transverse Deflecting Cavity with Arbitrary Polarizations for the SACLA Injector Sep. 14th, 2015 H. Maesaka, T. Asaka,
Hui Wang†*, Canturk Isci‡, Lavanya Subramanian*,
Fuel cell development program for electric vehicle
Overview of TST-2 Experiment
Optomechanics with atoms
داده کاوی سئوالات نمونه
Inter-system biases estimation in multi-GNSS relative positioning with GPS and Galileo Cecile Deprez and Rene Warnant University of Liege, Belgium  
ლექცია 4 - ფული და ინფლაცია
10. predavanje Novac i financijski sustav
Wissenschaftliche Aussprache zur Dissertation
FLUORECENCE MICROSCOPY SUPERRESOLUTION BLINK MICROSCOPY ON THE BASIS OF ENGINEERED DARK STATES* *Christian Steinhauer, Carsten Forthmann, Jan Vogelsang,
Particle acceleration during the gamma-ray flares of the Crab Nebular
Interpretations of the Derivative Gottfried Wilhelm Leibniz
Advisor: Chiuyuan Chen Student: Shao-Chun Lin
Widow Rockfish Assessment
SiW-ECAL Beam Test 2015 Kick-Off meeting
On Robust Neighbor Discovery in Mobile Wireless Networks
Chapter 6 并发:死锁和饥饿 Operating Systems: Internals and Design Principles
You NEED your book!!! Frequency Distribution
Y V =0 a V =V0 x b b V =0 z
Fairness-oriented Scheduling Support for Multicore Systems
Climate-Energy-Policy Interaction
Hui Wang†*, Canturk Isci‡, Lavanya Subramanian*,
Ch48 Statistics by Chtan FYHSKulai
The ABCD matrix for parabolic reflectors and its application to astigmatism free four-mirror cavities.
Measure Twice and Cut Once: Robust Dynamic Voltage Scaling for FPGAs
Online Learning: An Introduction
Factor Based Index of Systemic Stress (FISS)
What is Chemistry? Chemistry is: the study of matter & the changes it undergoes Composition Structure Properties Energy changes.
THE BERRY PHASE OF A BOGOLIUBOV QUASIPARTICLE IN AN ABRIKOSOV VORTEX*
Quantum-classical transition in optical twin beams and experimental applications to quantum metrology Ivano Ruo-Berchera Frascati.
The Toroidal Sporadic Source: Understanding Temporal Variations
FW 3.4: More Circle Practice
ارائه یک روش حل مبتنی بر استراتژی های تکاملی گروه بندی برای حل مسئله بسته بندی اقلام در ظروف
Decision Procedures Christoph M. Wintersteiger 9/11/2017 3:14 PM
Limits on Anomalous WWγ and WWZ Couplings from DØ
Presentation transcript:

Flow to Wells – 1 Steady flow to a well in a confined aquifer Groundwater Hydraulics Daene C. McKinney

Summary Some Information on Wells Steady flow to a well in a confined aquifer

Some Information on Wells

Domestic Hand Pumped Well Domestic dug well with rock curb, concrete seal, and hand pump ~20 m depth > 1 m diameter < 500 m3/day Hand dug well in Beirut, Lebanon Hand dug well in Trets, France

Augers Hand-driven augers ~15 m depth > 20 cm diameter Power-driven augers ~30 m depth > 1 m diameter

Power Auger Auger drilling is done with a helical screw driven into the ground with rotation; cuttings are lifted up the borehole by the screw ~ 30 m depth < 15-90 cm diameter < 500 m3/day

Drilled Well - Cable Tool Traditional way of drilling large diameter water supply wells. The Rig raises and drops the drill string with a heavy carbide tipped drill bit that chisels through the rock and pulverizes the materials. 8 – 60 cm 600 m

Mud/Air Rotary Rotary drilling relies on continuous circular motion of the bit to break rock at the bottom of the hole. Cuttings are removed as drilling fluids circulate through the bit and up the wellbore to the surface.

Drilling Mud Circulation Lift cuttings from the borehole and carry to pit; Cuttings drop out in the pit; Length of drill pipe is added; Film on the borehole wall prevents caving; Seals borehole wall to reduce fluid loss; Cools and cleans bit; and Lubricates bit, bearings, mud pump and drill pipe .

Well Completion After drilling, must “complete” the well Placement of casing Placement of well screen Placement of gravel packing Open hole

Well Construction Well casing Lining to maintain open hole Seals out other water (surface, formations) Structural support against cave-in

Well in Limestone Surface casing From ground surface through unconsolidated upper material

Placing the Pack

Steady Flow to a Well in a Confined Aquifer

Flow to a Well in a Confined Aquifer

Drawdown in a Well Drawdown in a pumped well consists of two components: Aquifer losses Head losses that occur in the aquifer where the flow is laminar Tme-dependent Vary linearly with the well discharge Well losses Aquifer damage during drilling and completion Turbulent friction losses adjacent to well, in the well and pipe

Drawdown to a pumping well in a confined aquifer Uncased hole Screened well Gravel-packed well Bear, 1979, Fig. 8.3

Groundwater Notation Confined aquifer 𝛻∙𝑇𝛻ℎ= 𝜕 𝜕𝑥 𝑇 𝑥 𝜕ℎ 𝜕𝑥 + 𝜕 𝜕𝑦 𝑇 𝑦 𝜕ℎ 𝜕𝑦 =S 𝜕ℎ 𝜕𝑡 General equation, rectangular coordinates 𝛻 2 ℎ= 𝜕 2 ℎ 𝜕 𝑥 2 + 𝜕 2 ℎ 𝜕 𝑦 2 =0 Steady state flow, homogeneous and Isotropic aquifer 𝛻∙𝑇𝛻ℎ= 1 𝑟 𝜕 𝜕𝑟 𝑇 𝑟 𝑟 𝜕ℎ 𝜕𝑟 + 1 𝑟 2 𝜕 𝜕𝜃 𝑇 𝜃 𝜕ℎ 𝜕𝜃 =𝑆 𝜕ℎ 𝜕𝑡 General equation, radial coordinates 𝛻 2 ℎ= 1 𝑟 𝜕 𝜕𝑟 𝑟 𝜕ℎ 𝜕𝑟 + 1 𝑟 2 𝜕 2 ℎ 𝜕 𝜃 2 =0 Steady state flow, homogeneous and Isotropic aquifer

Steady Flow to a Well in a Confined Aquifer 2rw Ground surface Bedrock Confined aquifer Q h0 Pre-pumping head Confining Layer b r1 r2 h2 h1 hw Observation wells Drawdown curve Pumping well Governing equation in radial coordinates 𝛻 2 ℎ= 1 𝑟 𝜕 𝜕𝑟 𝑟 𝜕ℎ 𝜕𝑟 + 1 𝑟 2 𝜕 2 ℎ 𝜕 𝜃 2 = 𝑆 𝑇 𝜕ℎ 𝜕𝑡 Homogeneous and Isotropic aquifer 𝑑 𝑑𝑟 𝑟 𝑑ℎ 𝑑𝑟 =0 Steady state flow

Steady Flow to a Well in a Confined Aquifer 𝑑 𝑑𝑟 𝑟 𝑑ℎ 𝑑𝑟 =0 2rw Ground surface Bedrock Confined aquifer Q h0 Pre-pumping head Confining Layer b r1 r2 h2 h1 hw Observation wells Drawdown curve Pumping well 𝑟 𝑑ℎ 𝑑𝑟 = 𝐶 1 Darcy’s law 𝑄=𝐴𝑞= 2𝜋𝑟𝑏 𝐾 𝑑ℎ 𝑑𝑟 𝑟 𝑑ℎ 𝑑𝑟 = 𝑄 2𝜋𝑏𝐾 =𝐶 1 𝑑ℎ= 𝑄 2𝜋𝑇 𝑑𝑟 𝑟 ℎ= 𝑄 2𝜋𝑇 𝑙𝑛 𝑟 + 𝐶 2

Steady Flow to a Well in a Confined Aquifer ℎ= 𝑄 2𝜋𝑇 𝑙𝑛 𝑟 + 𝐶 2 2rw Ground surface Bedrock Confined aquifer Q h0 Pre-pumping head Confining Layer b r1 r2 h2 h1 hw Observation wells Drawdown curve Pumping well Boundary condition: ℎ= ℎ 1 @ 𝑟= 𝑟 1 ℎ 1 = 𝑄 2𝜋𝑇 𝑙𝑛 𝑟 1 + 𝐶 2 𝐶 2 =ℎ 1 − 𝑄 2𝜋𝑇 𝑙𝑛 𝑟 1 ℎ= 𝑄 2𝜋𝑇 𝑙𝑛 𝑟 + ℎ 1 − 𝑄 2𝜋𝑇 𝑙𝑛 𝑟 1 ℎ= ℎ 1 + 𝑄 2𝜋𝑇 𝑙𝑛 𝑟 𝑟 1

Example - Steady Flow to a Well in a Confined Aquifer Q = 400 m3/hr b = 40 m Two observation wells, h1 = 85.3 m (@ r1 = 25 m) h2 = 89.6 m (@ r2 = 75 m) Find: Transmissivity (T) 2rw Ground surface Bedrock Confined aquifer Q h0 Confining Layer b r1 r2 h2 h1 hw Pumping well ℎ= ℎ 1 + 𝑄 2𝜋𝑇 𝑙𝑛 𝑟 𝑟 1 ℎ 2 = ℎ 1 + 𝑄 2𝜋𝑇 𝑙𝑛 𝑟 2 𝑟 1

Drawdown, s ℎ= ℎ 0 @ 𝑟= 𝑟 0 ℎ= ℎ 0 + 𝑄 2𝜋𝑇 𝑙𝑛 𝑟 𝑟 0 𝑠= ℎ 0 −ℎ ℎ= ℎ 0 @ 𝑟= 𝑟 0 ℎ= ℎ 0 + 𝑄 2𝜋𝑇 𝑙𝑛 𝑟 𝑟 0 𝑠= ℎ 0 −ℎ 𝑠= ℎ 0 − ℎ 0 + 𝑄 2𝜋𝑇 𝑙𝑛 𝑟 𝑟 0 𝑠(𝑟)= 𝑄 2𝜋𝑇 𝑙𝑛 𝑟 0 𝑟

Example - Steady Flow to a Well in a Confined Aquifer 1-m diameter well Q = 113 m3/hr b = 30 m h0= 40 m Two observation wells, h1 = 38.2 m (@ r1 = 15 m) h2 = 39.5 m (@ r2 = 50 m) Find: Head and drawdown at the well 2rw Ground surface Bedrock Confined aquifer Q h0 Confining Layer b r1 r2 h2 h1 hw Pumping well Drawdown ℎ= ℎ 1 + 𝑄 2𝜋𝑇 𝑙𝑛 𝑟 𝑟 1 𝑠 1 = ℎ 0 − ℎ 1 𝑠 2 = ℎ 0 − ℎ 2 𝑠 1 − 𝑠 2 = ℎ 2 − ℎ 1 = 𝑄 2𝜋𝑇 𝑙𝑛 𝑟 2 𝑟 1 𝑇= 𝑄 2𝜋 𝑠 1 − 𝑠 2 𝑙𝑛 𝑟 2 𝑟 1 = 113 𝑚 3 /ℎ𝑟 2𝜋 1.8−0.5 𝑚 𝑙𝑛 50 15 =16.66 𝑚 2 /ℎ𝑟

Example - Steady Flow to a Well in a Confined Aquifer 2rw Ground surface Bedrock Confined aquifer Q h0 Confining Layer b r1 r2 h2 h1 hw Drawdown @ well ℎ= ℎ 1 + 𝑄 2𝜋𝑇 𝑙𝑛 𝑟 𝑟 1 ℎ 𝑤 = ℎ 1 + 𝑄 2𝜋𝑇 𝑙𝑛 𝑟 𝑤 𝑟 1 ℎ 𝑤 =38.2 𝑚+ 113 𝑚 3 /ℎ𝑟 2𝜋 16.66 𝑚 2 /ℎ𝑟 𝑙𝑛 0.5 15 ℎ 𝑤 =34.5 𝑚 Head at the well 𝑠 𝑤 = ℎ 0 −ℎ=40−34.5 𝑚=5.5 𝑚 Drawdown at the well

Flow to a Partially Penetrating Well in a Confined Aquifer

Summary Some Information on Wells Steady flow to a well in a confined aquifer