Hydrology & Irrigation. Civil Engineering

Size: px
Start display at page:

Download "Hydrology & Irrigation. Civil Engineering"

Transcription

1 Hdrolog & Irrigation For Civil Engineering B wwwthegateacadeco

2 Sllabus Sllabus for Hdrolog & Irrigation Hdrolog: Hdrologic Ccle, Precipitation, Evaporation, Evapo-Transpiration, Watershed, Infiltration, Unit Hdrographs, Hdrograph nalsis, Flood Estiation and outing, eservoir Capacit, eservoir and Channel outing, Surface un-off Models, Ground Water Hdrolog - Stead State Well Hdraulics and quifers; pplication of Darc s Law Irrigation: Dut, Delta, Estiation of Evapo-Transpiration; Crop Water equireents; Design of Lined and Unlined Canals, Head Works, Gravit Das and Spillwas; Design of Weirs on Pereable Foundation; Tpes of Irrigation Sstes, Irrigation Methods; Water Logging and Drainage; Canal egulator Works, Cross-Drainage Structures, Outlets and Escapes nalsis of GTE Papers Year Percentage of Marks Overall Percentage % : , info@thegateacadeco Copright reserved Web:wwwthegateacadeco

3 Contents Contents Chapter Page No # 1 Open Channel Flow 1 15 Introduction 1 Tpes of Channel 1 9 Pressure Distribution Hdraulic Jup #2 Irrigation Introduction Flow Irrigation ssignent 22 nswer Kes & Explanations 22 #3 Water equireents of Crops Definition Dut at Various Places Optiu Utilization of Irrigation Water #4 Soil Moisture Irrigation elationship Introduction 28 Field Capacit Solved Exaples #5 Sedient Transport and Design of Irrigation Channels Sedient Transport Mechanics of Sedient Transport Water Logging Control Tube Wells Design of Channels Kenned s egie Theor Lindle s egie Theor Design of Irrigation Channel b Lace s egie Theor Causes of Failure of Weir or Barrage on Pereable Foundation Bligh s Creep Theor for Seepage Flow Lane s Weighted Creep Theor 57 Khosla s Theor and Concept of Flow Nets Exit Gradient 67 ssignent 68 nswer Kes & Explanations 69 : , info@thegateacadeco Copright reserved Web:wwwthegateacadeco i

4 Contents #6 Hdrolog Introduction 70 Hdrologic Ccle Water Budget Equation World Water Quantities 74 Precipitation Measureent of Precipitation Preparation of Data Frequenc of Point ainfall Evaporation Variation of ET/PET Measureent of Infiltration Stage Discharge elationships Measureent of Velocit Hdrograph and unoff Base Flow Separation S Curve Technique Floods Estiation Well Hdraulics Saturation Foration Well Hdraulics Introduction Stead Flow in Open Well ssignent nswer Kes & Explanations Module Test Test Questions nswer Kes & Explanations 131 eference Books 132 : , info@thegateacadeco Copright reserved Web:wwwthegateacadeco ii

5 CHPTE 1 "In order to succeed ou ust fail so that ou know what not to do the next tie" nthon J D'ngelo Open Channel Flow Learning Objectives fter reading this chapter, ou will know: 1 Tpes of Channel 2 General Tpes of Flow in Open Channels 3 Geoetrical Paraeters of an Open Channel Flow 4 Pressure Distribution 5 Hdraulic Jup Introduction n open channel is a sloped liquid flow passage having solid boundaries with the top surface open to gaseous atosphere The top surface of the channel, called free surface which is the surface of contact between the flowing liquid and the overling gas, its subjected to constant pressure throughout its length and breadth In the pipe, flow occurs due to pressure gradient, but for open channel flow, it happens ostl for gravit The cross-section section for pipe flow is ostl circular but for open channel flow the cross-section can be of an geoetr Tpes of Channel 1 Open and Closed Channels: Open channels are also called uncovered channels have no cover at the top and it is copletel open to atosphere Close channel are called covered channels, have cover or roof at the top In other words the closed channel is a closed passage which does not run full, so that the liquid has free surface in contact with air ir occupies the space between the liquid surface and the top cover 2 Natural and rtificial Channels 3 Prisatic and Non-Prisatic Channels: channel having the sae flow cross-section throughout its length and having a constant botto flow is called prisatic channel 4 Exponential and Non-Exponential Channels: Depending on the tpe of cross-section of the channel, it is classified as exponential and non-exponential channels In case of an exponential channel, the cross-section area is prescribed b the equation K, where is the sectional area, is the depth of flow, k and n are the experiental constant The exaples of exponential channels are rectangular, triangular and parabolic channels For non-exponential channels, exaples are trapezoidal and circular channel : , info@thegateacadeco Copright reserved Web:wwwthegateacadeco 1

6 General Tpes of Flow in Open Channels Open Channel Flow 1 Stead and Unstead Flow If the flow characteristic of an open channel do not change with tie, then it is stead flow and if it is changing with flow, then it is unstead flow For ste low For unste low N t N t 2 Unifor and Non-Unifor Flow When the flow characteristics does not change with space, then it is unifor flow or else it is non-unifor flow N N Uni or low or non uni or low s s The non-unifor flow is further classified into two tpes (i) VF- apidl Varied Flow (ii) GVF- Graduall Varied Flow VF: It is defined as that flow in which the depth of flow changes abruptl over a sall length of a channel 3 Lainar and Turbulent Flow VD enol s nu er L D h r teristi Length h r teristi Diension For n open h nnel D is the h r uli r ius whi h is e ine P L in r Flow Tr nsition l Flow Turnulent Flow s Wette re Wette perieters 4 Subcritical, Critical and Super Critical Flow V F (Foru e No) Where V is the velo it o low g D D is the hdraulic depth T ue to gr vit rea : , info@thegateacadeco Copright reserved Web:wwwthegateacadeco 2

7 Open Channel Flow D T Froude no is the ratio of inertia force and gravit force Interti For e F Gr vit For e I F Sub critical flow/tranquil flow/ Steaing flow I F Then it is critical flow I F Super critical flow/apid flow/shooting flow Geoetrical Paraeters of an Open Channel Flow Free Liquid Surface d h Channel Botto 1 Depth of Flow (): It is the vertical distance b/w the lowest point in the channel section and the ree liqui sur e it is enote 2 Depth of Flow Section (d): It is the actual depth of the channel easured noral to the direction o low It is enote s 3 Top Width (T): It is the width of the channel at the free surface open to the atosphere it is enote T 4 Hdraulic Depth (D): T The h r uli epth or i erent se tion re (i) e t ngul r () (ii) Tri ngul r ( ) (iii) Tr pezoi l ( (iv) P r oli (v) ir ul r r sin ( sin 5 Wetted rea: () For ectangular (B) For Triangular (C) For Parabolic ) (D) For Trapezoidal ( ) (E) Circular ( sin ) ) l : , info@thegateacadeco Copright reserved Web:wwwthegateacadeco 3

8 Open Channel Flow 6 Wetted Perieter: The length of the channel boundar which coes in contact with the flowing liquid is called wetted perieter and it is denoted b P (a) ectangular (b) Circular r (c) P r oli (d) Trin gul r (e) Tr pezoi l 7 Hdraulic adius: 8 Bed Slope of Channel: The inclination of the channel bed with the horizontal is the bed slope of channel it is denoted b so for a unifor flow, since the bed slope and liquid surface slope are sae, then it is denoted b S S sin where, h is the vertical disp and this relation is valid for when is ver sall where, sin t n 9 Section Factor: Section factor for critical flow is the product of wetted area and the square root of hdraulic depth It is denoted b D ( ) T ( ) e t ngul r ( ) Tri ngul r ( ) P r oli T ( ) ( ) Tr pezoi l (e) ir ul r [( )] ( ) sin *r ( sin )+ For Discharge Equation for Unifor Flow in Open Channel 1 The Chez equation, V = S C hez s onst nt P To find out the value of c, (a) Kutter s Forul ( ) H ( ) Where n roughness o e i ient zin Forul ( ) For sooth sur e For rough sur e ( ) n M nning s Forul : , info@thegateacadeco Copright reserved Web:wwwthegateacadeco 4

9 Open Channel Flow 2 M nning s Equ tion V n S here the value of n = 01 for sooth surface = 004 for rough surface Channel of ost efficient cross-section n open channel of given slope, roughness and area if flow is said to be hdraulicall efficient or ost econoic section, when it carries the axiu discharge For hez s equ tion or given slope n roughness velocit is axiu when hdraulic radius is iniu Further for a given area hdraulic radius is axiu when wetted perieter is iniu ectangular Channel For ectangular channel Trapezoidal Channel ( ) b 1 Circular Channel D here D i b Exaple: Find the bed slope in channels of the following sections having top width 5 and unifor depth 2 Take the discharge value as 003 se n hez s onst nt s Find out for 1 ectangular channel 2 Triangular 3 Trapezoidal channel with side slope 1H:3V Q se T Solution: (i) ectangular V S P S : , info@thegateacadeco Copright reserved Web:wwwthegateacadeco 5

10 Open Channel Flow (ii) Triangular P T Q S P T P PS QS (iii) Trapezoidal (b+2 )=T b Exaple: The cross-section of a navigation channel is shown in figure deterine the discharge through the channel if the depth of flow in 12 the channel has a slope of 1 in 2000 and the hez s onst nt is Solution: I J D E F G H S V S : , info@thegateacadeco Copright reserved Web:wwwthegateacadeco 6

Water Flow in Open Channels

Water Flow in Open Channels The Islamic Universit of Gaza Facult of Engineering Civil Engineering Department Hdraulics - ECIV 33 Chapter 6 Water Flow in Open Channels Introduction An open channel is a duct in which the liquid flows

More information

STEADY UNIFORM FLOW IN OPEN CHANNEL

STEADY UNIFORM FLOW IN OPEN CHANNEL 11/4/018 School of Environmental Engineering STEY UNIFORM FLOW IN OEN CHNNEL ZULKRNIN BIN HSSN COURSE OUTCOMES CO1: ble to analyze and design the steady flow in pipeline (O1) CO: ble to analyze and design

More information

Uniform Flow in Open Channels

Uniform Flow in Open Channels 1 UNIT 2 Uniform Flow in Open Channels Lecture-01 Introduction & Definition Open-channel flow, a branch of hydraulics, is a type of liquid flow within a conduit with a free surface, known as a channel.

More information

Closed duct flows are full of fluid, have no free surface within, and are driven by a pressure gradient along the duct axis.

Closed duct flows are full of fluid, have no free surface within, and are driven by a pressure gradient along the duct axis. OPEN CHANNEL FLOW Open channel flow is a flow of liquid, basically water in a conduit with a free surface. The open channel flows are driven by gravity alone, and the pressure gradient at the atmospheric

More information

presented by Umut Türker Open Channel Flow

presented by Umut Türker Open Channel Flow presented by Umut Türker Open Channel Flow What is open channel flow? Open channel flow is a flow which has a free surface and flows due to the gravitational effect What is open channel flow? Open channel

More information

Presented by: Civil Engineering Academy

Presented by: Civil Engineering Academy Presented by: Civil Engineering Academy Open-Channel Flow Uniform Flow (See CERM Ch. 19) Characterized by constant depth volume, and cross section. It can be steady or unsteady Non-uniform Flow *Not on

More information

Closed duct flows are full of fluid, have no free surface within, and are driven by a pressure gradient along the duct axis.

Closed duct flows are full of fluid, have no free surface within, and are driven by a pressure gradient along the duct axis. OPEN CHANNEL FLOW Open channel flow is a flow of liquid, basically water in a conduit with a free surface. The open channel flows are driven by gravity alone, and the pressure gradient at the atmospheric

More information

DISTRIBUTION OF THE HYDRAULIC PARAMETERS AT RIVER BENDS

DISTRIBUTION OF THE HYDRAULIC PARAMETERS AT RIVER BENDS DISTRIBUTION OF THE HYDRAULIC PARAMETERS AT RIVER BENDS Isa Issa Oran *, Riyad Hassan Al-Anbari ** and Walaa Khalil Ali *** * Assist. Professor, Foundation of Technical Education ** Assist. Professor,

More information

Hydraulics Part: Open Channel Flow

Hydraulics Part: Open Channel Flow Hydraulics Part: Open Channel Flow Tutorial solutions -by Dr. K.N. Dulal Uniform flow 1. Show that discharge through a channel with steady flow is given by where A 1 and A 2 are the sectional areas of

More information

NPTEL Quiz Hydraulics

NPTEL Quiz Hydraulics Introduction NPTEL Quiz Hydraulics 1. An ideal fluid is a. One which obeys Newton s law of viscosity b. Frictionless and incompressible c. Very viscous d. Frictionless and compressible 2. The unit of kinematic

More information

Local energy losses at positive and negative steps in subcritical open channel flows

Local energy losses at positive and negative steps in subcritical open channel flows Local energ losses at positive and negative steps in subcritical open channel flows Nura Denli Toka and A Burcu Altan-Sakara* Middle East Technical niversit, Department of Civil Engineering, 63, Ankara,

More information

NOTES ON OPEN CHANNEL FLOW

NOTES ON OPEN CHANNEL FLOW NOTES ON OPEN CHANNEL FLOW Prof. Marco Pilotti DICATAM, niversità degli Studi di Brescia Profili di moto permanente in un canale e in una serie di due canali - Boudine, 86 OPEN CHANNEL FLOW: uniform motion

More information

THE EFFECT OF SOLID PARTICLE SIZE UPON TIME AND SEDIMENTATION RATE

THE EFFECT OF SOLID PARTICLE SIZE UPON TIME AND SEDIMENTATION RATE Bulletin of the Transilvania University of Braşov Series II: Forestry Wood Industry Agricultural Food Engineering Vol. 5 (54) No. 1-1 THE EFFECT OF SOLID PARTICLE SIZE UPON TIME AND SEDIMENTATION RATE

More information

28.2 Classification of Jumps

28.2 Classification of Jumps 28.2 Classification of Jumps As mentioned earlier, the supercritical flow Froude number influences the characteristics of the hydraulic jump. Bradley and Peterka, after extensive experimental investigations,

More information

CHAPTER 07 CANAL DESIGN

CHAPTER 07 CANAL DESIGN CHAPTER 07 CANAL DESIGN Dr. M. R. Kabir Professor and Head, Department of Civil Engineering University of Asia Pacific (UAP), Dhaka LECTURE 17 Canal Design Types Canal Design Drainage Channel Design Irrigation

More information

Lecture Note for Open Channel Hydraulics

Lecture Note for Open Channel Hydraulics Chapter -one Introduction to Open Channel Hydraulics 1.1 Definitions Simply stated, Open channel flow is a flow of liquid in a conduit with free space. Open channel flow is particularly applied to understand

More information

Spine Fin Efficiency A Three Sided Pyramidal Fin of Equilateral Triangular Cross-Sectional Area

Spine Fin Efficiency A Three Sided Pyramidal Fin of Equilateral Triangular Cross-Sectional Area Proceedings of the 006 WSEAS/IASME International Conference on Heat and Mass Transfer, Miai, Florida, USA, January 18-0, 006 (pp13-18) Spine Fin Efficiency A Three Sided Pyraidal Fin of Equilateral Triangular

More information

Celal S. Konor Release 1.1 (identical to 1.0) 3/21/08. 1-Hybrid isentropic-sigma vertical coordinate and governing equations in the free atmosphere

Celal S. Konor Release 1.1 (identical to 1.0) 3/21/08. 1-Hybrid isentropic-sigma vertical coordinate and governing equations in the free atmosphere Celal S. Konor Release. (identical to.0) 3/2/08 -Hybrid isentropic-siga vertical coordinate governing equations in the free atosphere This section describes the equations in the free atosphere of the odel.

More information

UNIFORM FLOW CRITICAL FLOW GRADUALLY VARIED FLOW

UNIFORM FLOW CRITICAL FLOW GRADUALLY VARIED FLOW UNIFORM FLOW CRITICAL FLOW GRADUALLY VARIED FLOW Derivation of uniform flow equation Dimensional analysis Computation of normal depth UNIFORM FLOW 1. Uniform flow is the flow condition obtained from a

More information

Ocean 420 Physical Processes in the Ocean Project 1: Hydrostatic Balance, Advection and Diffusion Answers

Ocean 420 Physical Processes in the Ocean Project 1: Hydrostatic Balance, Advection and Diffusion Answers Ocean 40 Physical Processes in the Ocean Project 1: Hydrostatic Balance, Advection and Diffusion Answers 1. Hydrostatic Balance a) Set all of the levels on one of the coluns to the lowest possible density.

More information

Ch 12: Variations on Backpropagation

Ch 12: Variations on Backpropagation Ch 2: Variations on Backpropagation The basic backpropagation algorith is too slow for ost practical applications. It ay take days or weeks of coputer tie. We deonstrate why the backpropagation algorith

More information

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING Urban Drainage: Hydraulics. Solutions to problem sheet 2: Flows in open channels

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING Urban Drainage: Hydraulics. Solutions to problem sheet 2: Flows in open channels DEPRTMENT OF CIVIL ND ENVIRONMENTL ENGINEERING Urban Drainage: Hydraulics Solutions to problem sheet 2: Flows in open channels 1. rectangular channel of 1 m width carries water at a rate 0.1 m 3 /s. Plot

More information

Daniel López Gaxiola 1 Student View Jason M. Keith

Daniel López Gaxiola 1 Student View Jason M. Keith Suppleental Material for Transport Process and Separation Process Principles Chapter Principles of Moentu Transfer and Overall Balances In fuel cells, the fuel is usually in gas or liquid phase. Thus,

More information

SEM-2016(01HI CIVIL ENGINEERING. Paper Answer all questions. Question No. 1 does not have internal choice,

SEM-2016(01HI CIVIL ENGINEERING. Paper Answer all questions. Question No. 1 does not have internal choice, Roll No. Candidate should write his/her Roll No. here. Total No. of Questions : 5 No. of Printed Pages : 8 SEM-2016(01HI CIVIL ENGINEERING Paper - 11 Time : 3 Hours ] [ Total Marks : 300 Instructions to

More information

Chapter 4 FORCES AND NEWTON S LAWS OF MOTION PREVIEW QUICK REFERENCE. Important Terms

Chapter 4 FORCES AND NEWTON S LAWS OF MOTION PREVIEW QUICK REFERENCE. Important Terms Chapter 4 FORCES AND NEWTON S LAWS OF MOTION PREVIEW Dynaics is the study o the causes o otion, in particular, orces. A orce is a push or a pull. We arrange our knowledge o orces into three laws orulated

More information

CE 6403 APPLIED HYDRAULIC ENGINEERING UNIT - III RAPIDLY VARIED FLOW

CE 6403 APPLIED HYDRAULIC ENGINEERING UNIT - III RAPIDLY VARIED FLOW CE 6 APPLIED HYDRAULIC ENGINEERING UNIT - III RAPIDLY VARIED FLOW Application of the energy equation for RVF - Critical epth an velocity - Critical, Sub-critical an Super-critical flow - Application of

More information

1. Open Channel Hydraulics

1. Open Channel Hydraulics Open Channel Flow. Open Channel Hydraulics.... Definition and differences between pipe flow and open channel flow.... Types of flow.... Properties of open channels...4.4 Fundamental equations... 5.4. The

More information

Created by Simpo PDF Creator Pro (unregistered version)

Created by Simpo PDF Creator Pro (unregistered version) 2 nd Semester TRANSITIONS STRUCTURES 1 of 9 A transition is a local change in cross-section which produces a variation of flow from one uniform state to another due to the change in cross sections of channels.

More information

Open Channel Flow Part 2. Ch 10 Young, notes, handouts

Open Channel Flow Part 2. Ch 10 Young, notes, handouts Open Channel Flow Part 2 Ch 10 Young, notes, handouts Uniform Channel Flow Many situations have a good approximation d(v,y,q)/dx=0 Uniform flow Look at extended Bernoulli equation Friction slope exactly

More information

Experiment 7 Energy Loss in a Hydraulic Jump

Experiment 7 Energy Loss in a Hydraulic Jump Experiment 7 Energ Loss in a Hdraulic Jump n Purpose: The purpose of this experiment is to examine the transition from supercritical (rapid) flow to subcritical (slow) flow in an open channel and to analze

More information

Measuring Temperature with a Silicon Diode

Measuring Temperature with a Silicon Diode Measuring Teperature with a Silicon Diode Due to the high sensitivity, nearly linear response, and easy availability, we will use a 1N4148 diode for the teperature transducer in our easureents 10 Analysis

More information

Hydraulics Prof. Dr. Arup Kumar Sarma Department of Civil Engineering Indian Institute of Technology, Guwahati

Hydraulics Prof. Dr. Arup Kumar Sarma Department of Civil Engineering Indian Institute of Technology, Guwahati Hydraulics Prof. Dr. Arup Kumar Sarma Department of Civil Engineering Indian Institute of Technology, Guwahati Module No. # 04 Gradually Varied Flow Lecture No. # 07 Rapidly Varied Flow: Hydraulic Jump

More information

Visualization of flow pattern over or around immersed objects in open channel flow.

Visualization of flow pattern over or around immersed objects in open channel flow. EXPERIMENT SEVEN: FLOW VISUALIZATION AND ANALYSIS I OBJECTIVE OF THE EXPERIMENT: Visualization of flow pattern over or around immersed objects in open channel flow. II THEORY AND EQUATION: Open channel:

More information

Lecture 10: River Channels

Lecture 10: River Channels GEOG415 Lecture 10: River Channels 10-1 Importance of channel characteristics Prediction of flow was the sole purpose of hydrology, and still is a very important aspect of hydrology. - Water balance gives

More information

OPEN CHANNEL FLOW. One-dimensional - neglect vertical and lateral variations in velocity. In other words, Q v = (1) A. Figure 1. One-dimensional Flow

OPEN CHANNEL FLOW. One-dimensional - neglect vertical and lateral variations in velocity. In other words, Q v = (1) A. Figure 1. One-dimensional Flow OPEN CHANNEL FLOW Page 1 OPEN CHANNEL FLOW Open Channel Flow (OCF) is flow with one boundary exposed to atmospheric pressure. The flow is not pressurized and occurs because of gravity. Flow Classification

More information

1 Branch: CIVIL ENGINEERING Sub: HYDRAULICS AND HYDRAULIC MACHINERY Date: 11/03/2017

1 Branch: CIVIL ENGINEERING Sub: HYDRAULICS AND HYDRAULIC MACHINERY Date: 11/03/2017 G.PULLAIAH COLLEGE OF ENGINEERING & TECHNOLOGY (AT) II B.Tech Objective Paper I MID EXAM 1 Branch: CIVIL ENGINEERING Sub: HYDRAULICS AND HYDRAULIC MACHINERY Date: 11/03/2017 Time: 20 min Max.Marks:10 Roll

More information

Fluid Mechanics Prof. S.K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

Fluid Mechanics Prof. S.K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Fluid Mechanics Prof. S.K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Lecture - 42 Flows with a Free Surface Part II Good morning. I welcome you to this session

More information

2. Which of the following best describes the relationship between force and potential energy?

2. Which of the following best describes the relationship between force and potential energy? Work/Energy with Calculus 1. An object oves according to the function x = t 5/ where x is the distance traveled and t is the tie. Its kinetic energy is proportional to (A) t (B) t 5/ (C) t 3 (D) t 3/ (E)

More information

Advanced Hydraulics Prof. Dr. Suresh A. Kartha Department of Civil Engineering Indian Institute of Technology, Guwahati

Advanced Hydraulics Prof. Dr. Suresh A. Kartha Department of Civil Engineering Indian Institute of Technology, Guwahati Advanced Hydraulics Prof. Dr. Suresh A. Kartha Department of Civil Engineering Indian Institute of Technology, Guwahati Module - 2 Uniform Flow Lecture - 1 Introduction to Uniform Flow Good morning everyone,

More information

Dr. Muhammad Ali Shamim ; Internal 652

Dr. Muhammad Ali Shamim ; Internal 652 Dr. Muhammad Ali Shamim ali.shamim@uettaxila.edu.pk 051-904765; Internal 65 Channel Tranistions A channel transition is defined as change in channel cross section e.g. change in channel width and/or channel

More information

PHYS 1443 Section 003 Lecture #22

PHYS 1443 Section 003 Lecture #22 PHYS 443 Section 003 Lecture # Monda, Nov. 4, 003. Siple Bloc-Spring Sste. Energ of the Siple Haronic Oscillator 3. Pendulu Siple Pendulu Phsical Pendulu orsion Pendulu 4. Siple Haronic Motion and Unifor

More information

UNCERTAINTIES IN THE APPLICATION OF ATMOSPHERIC AND ALTITUDE CORRECTIONS AS RECOMMENDED IN IEC STANDARDS

UNCERTAINTIES IN THE APPLICATION OF ATMOSPHERIC AND ALTITUDE CORRECTIONS AS RECOMMENDED IN IEC STANDARDS Paper Published on the16th International Syposiu on High Voltage Engineering, Cape Town, South Africa, 2009 UNCERTAINTIES IN THE APPLICATION OF ATMOSPHERIC AND ALTITUDE CORRECTIONS AS RECOMMENDED IN IEC

More information

Running Water Earth - Chapter 16 Stan Hatfield Southwestern Illinois College

Running Water Earth - Chapter 16 Stan Hatfield Southwestern Illinois College Running Water Earth - Chapter 16 Stan Hatfield Southwestern Illinois College Hydrologic Cycle The hydrologic cycle is a summary of the circulation of Earth s water supply. Processes involved in the hydrologic

More information

OBJECTIVES INTRODUCTION

OBJECTIVES INTRODUCTION M7 Chapter 3 Section 1 OBJECTIVES Suarize data using easures of central tendency, such as the ean, edian, ode, and idrange. Describe data using the easures of variation, such as the range, variance, and

More information

UNIVERSITY OF BOLTON WESTERN INTERNATIONAL COLLEGE FZE. BEng (HONS) IN CIVIL ENGINEERING SEMESTER ONE EXAMINATION 2016/2017 GROUND AND WATER STUDIES 1

UNIVERSITY OF BOLTON WESTERN INTERNATIONAL COLLEGE FZE. BEng (HONS) IN CIVIL ENGINEERING SEMESTER ONE EXAMINATION 2016/2017 GROUND AND WATER STUDIES 1 OCD59 UNIVERSITY OF BOLTON WESTERN INTERNATIONAL COLLEGE FZE BEng (HONS) IN CIVIL ENGINEERING SEMESTER ONE EXAMINATION 2016/2017 GROUND AND WATER STUDIES 1 MODULE NO: CIE4009 Date: Saturday 14 January

More information

Problem Set 14: Oscillations AP Physics C Supplementary Problems

Problem Set 14: Oscillations AP Physics C Supplementary Problems Proble Set 14: Oscillations AP Physics C Suppleentary Probles 1 An oscillator consists of a bloc of ass 050 g connected to a spring When set into oscillation with aplitude 35 c, it is observed to repeat

More information

Efficiency of an Expansive Transition in an Open Channel Subcritical Flow

Efficiency of an Expansive Transition in an Open Channel Subcritical Flow DUET Journal Vol., Issue, June of an Expansive Transition in an Open Channel Subcritical Flow B. C. Basak and M. Alauddin Department of Civil Engineering Dhaka University of Engineering & Technology, Gazipur,

More information

XI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.com

XI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.com XI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K affan_414@live.co https://prootephysics.wordpress.co [MOTION] CHAPTER NO. 3 In this chapter we are going to discuss otion in one diension in which we

More information

The full procedure for drawing a free-body diagram which isolates a body or system consists of the following steps. 8 Chapter 3 Equilibrium

The full procedure for drawing a free-body diagram which isolates a body or system consists of the following steps. 8 Chapter 3 Equilibrium 8 Chapter 3 Equilibriu all effect on a rigid bod as forces of equal agnitude and direction applied b direct eternal contact. Eaple 9 illustrates the action of a linear elastic spring and of a nonlinear

More information

Spread footing verification Input data

Spread footing verification Input data Unite Kingo Sprea footing verification Input ata Project Date : 0.0.07 Settings Stanar - EN 997 - DA Materials an stanars Concrete structures : Coefficients EN 99-- : Classification Source CPT : Classification

More information

P = 2Rθ. The previous Manning formulas are used to predict V o and Q for uniform flow when the above expressions are substituted for A, P, and R h.

P = 2Rθ. The previous Manning formulas are used to predict V o and Q for uniform flow when the above expressions are substituted for A, P, and R h. Uniform Flow in a Partly Full, Circular Pipe Fig. 10.6 shows a partly full, circular pipe with uniform flow. Since frictional resistance increases with wetted perimeter, but volume flow rate increases

More information

Physics 140 D100 Midterm Exam 2 Solutions 2017 Nov 10

Physics 140 D100 Midterm Exam 2 Solutions 2017 Nov 10 There are 10 ultiple choice questions. Select the correct answer for each one and ark it on the bubble for on the cover sheet. Each question has only one correct answer. (2 arks each) 1. An inertial reference

More information

For more Study Material and Latest Questions related to IIT-JEE visit

For more Study Material and Latest Questions related to IIT-JEE visit or ore Study Material and Latest Questions related to IIT-JEE visit www. ICTION Introduction If we slide or try to slide a body over a surface, the otion is resisted by a bonding between the body and the

More information

Supplementary Information for Design of Bending Multi-Layer Electroactive Polymer Actuators

Supplementary Information for Design of Bending Multi-Layer Electroactive Polymer Actuators Suppleentary Inforation for Design of Bending Multi-Layer Electroactive Polyer Actuators Bavani Balakrisnan, Alek Nacev, and Elisabeth Sela University of Maryland, College Park, Maryland 074 1 Analytical

More information

CE 6403 APPLIED HYDRAULIC ENGINEERING UNIT - II GRADUALLY VARIED FLOW

CE 6403 APPLIED HYDRAULIC ENGINEERING UNIT - II GRADUALLY VARIED FLOW CE 6403 APPLIED HYDRAULIC ENGINEERING UNIT - II GRADUALLY VARIED FLOW Dynamic equations of gradually varied and spatially varied flows - Water surface flow profile classifications: Hydraulic Slope, Hydraulic

More information

NAME NUMBER SEC. PHYCS 101 SUMMER 2001/2002 FINAL EXAME:24/8/2002. PART(I) 25% PART(II) 15% PART(III)/Lab 8% ( ) 2 Q2 Q3 Total 40%

NAME NUMBER SEC. PHYCS 101 SUMMER 2001/2002 FINAL EXAME:24/8/2002. PART(I) 25% PART(II) 15% PART(III)/Lab 8% ( ) 2 Q2 Q3 Total 40% NAME NUMER SEC. PHYCS 101 SUMMER 2001/2002 FINAL EXAME:24/8/2002 PART(I) 25% PART(II) 15% PART(III)/Lab 8% ( ) 2.5 Q1 ( ) 2 Q2 Q3 Total 40% Use the followings: Magnitude of acceleration due to gravity

More information

Oscillatory Hydromagnetic Couette Flow in a Rotating System with Induced Magnetic Field *

Oscillatory Hydromagnetic Couette Flow in a Rotating System with Induced Magnetic Field * CHAPTER-4 Oscillator Hdroagnetic Couette Flow in a Rotating Sste with Induced Magnetic Field * 4. Introduction Lainar flow within a channel or duct in the absence of agnetic field is a phenoenon which

More information

Module 2 Lecture 9 Permeability and Seepage -5 Topics

Module 2 Lecture 9 Permeability and Seepage -5 Topics Module 2 Lecture 9 Permeability and Seepage -5 Topics 1.2.7 Numerical Analysis of Seepage 1.2.8 Seepage Force per Unit Volume of Soil Mass 1.2.9 Safety of Hydraulic Structures against Piping 1.2.10 Calculation

More information

Stage Discharge Tabulation for Only Orifice Flow

Stage Discharge Tabulation for Only Orifice Flow Stage Discharge Tabulation for Only Orifice Flow DEPTH STAGE DISCHARGE (meters) (feet) (meters) (feet) (m 3 /s) (ft 3 /s) 0 0.20 0.40 0.60 0.80 1.00 1.20 1.40 1.60 1.80 2.00 0.7 1.3 2.0 2.6 3.3 3.9 4.6

More information

1 (40) Gravitational Systems Two heavy spherical (radius 0.05R) objects are located at fixed positions along

1 (40) Gravitational Systems Two heavy spherical (radius 0.05R) objects are located at fixed positions along (40) Gravitational Systes Two heavy spherical (radius 0.05) objects are located at fixed positions along 2M 2M 0 an axis in space. The first ass is centered at r = 0 and has a ass of 2M. The second ass

More information

y 2 = 1 + y 1 This is known as the broad-crested weir which is characterized by:

y 2 = 1 + y 1 This is known as the broad-crested weir which is characterized by: CEE 10 Open Channel Flow, Dec. 1, 010 18 8.16 Review Flow through a contraction Critical and choked flows The hydraulic jump conservation of linear momentum y = 1 + y 1 1 + 8Fr 1 8.17 Rapidly Varied Flows

More information

Block designs and statistics

Block designs and statistics Bloc designs and statistics Notes for Math 447 May 3, 2011 The ain paraeters of a bloc design are nuber of varieties v, bloc size, nuber of blocs b. A design is built on a set of v eleents. Each eleent

More information

Designing for the Road User. Maximum Spiral Transition Lengths

Designing for the Road User. Maximum Spiral Transition Lengths IPENZ Transportation Conference 11 October 2006 Queenstown, New Zealand Designing for the Road User Maxiu Spiral Transition Lengths K H M Weale Northern Region Technical Developent Leader MWH New Zealand

More information

Lecture #8-3 Oscillations, Simple Harmonic Motion

Lecture #8-3 Oscillations, Simple Harmonic Motion Lecture #8-3 Oscillations Siple Haronic Motion So far we have considered two basic types of otion: translation and rotation. But these are not the only two types of otion we can observe in every day life.

More information

SEDIMENTATION INTRODUCTION

SEDIMENTATION INTRODUCTION SEDIMENTATION INTRODUCTION Sedimentation is removal of particulate materials suspended in water by quiescent settling due to gravity Commonly used unit operation in water and wastewater treatment plants

More information

Chemistry 432 Problem Set 11 Spring 2018 Solutions

Chemistry 432 Problem Set 11 Spring 2018 Solutions 1. Show that for an ideal gas Cheistry 432 Proble Set 11 Spring 2018 Solutions P V 2 3 < KE > where is the average kinetic energy of the gas olecules. P 1 3 ρ v2 KE 1 2 v2 ρ N V P V 1 3 N v2 2 3 N

More information

Advanced Hydraulics Prof. Dr. Suresh. A. Kartha Department of Civil Engineering Indian Institute of Technology, Guwahati

Advanced Hydraulics Prof. Dr. Suresh. A. Kartha Department of Civil Engineering Indian Institute of Technology, Guwahati Advanced Hydraulics Prof. Dr. Suresh. A. Kartha Department of Civil Engineering Indian Institute of Technology, Guwahati Module - 2 Uniform Flows Lecture - 4 Uniform Flow in Compound Sections Concept of

More information

Open Channel Flow - General. Hydromechanics VVR090

Open Channel Flow - General. Hydromechanics VVR090 Open Channel Flow - General Hydromechanics VVR090 ppt by Magnus Larson; revised by Rolf L Jan 2014, Feb 2015 SYNOPSIS 1. Introduction and Applications 2. The History of Open Channel Flow 3. Flow Classification

More information

Chem/Biochem 471 Exam 3 12/18/08 Page 1 of 7 Name:

Chem/Biochem 471 Exam 3 12/18/08 Page 1 of 7 Name: Che/Bioche 47 Exa /8/08 Pae of 7 Please leave the exa paes stapled toether. The forulas are on a separate sheet. This exa has 5 questions. You ust answer at least 4 of the questions. You ay answer ore

More information

Experiment 2: Hooke s Law

Experiment 2: Hooke s Law COMSATS Institute of Inforation Technology, Islaabad Capus PHYS-108 Experient 2: Hooke s Law Hooke s Law is a physical principle that states that a spring stretched (extended) or copressed by soe distance

More information

Lecture Outlines PowerPoint. Chapter 5 Earth Science 11e Tarbuck/Lutgens

Lecture Outlines PowerPoint. Chapter 5 Earth Science 11e Tarbuck/Lutgens Lecture Outlines PowerPoint Chapter 5 Earth Science 11e Tarbuck/Lutgens 2006 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors

More information

Open Channel Flow - General. Open Channel Flow

Open Channel Flow - General. Open Channel Flow Open Channel Flow - General Hydromechanics VVR090 Open Channel Flow Open channel: a conduit for flow which has a free surface Free surface: interface between two fluids of different density Characteristics

More information

Physics 11 HW #6 Solutions

Physics 11 HW #6 Solutions Physics HW #6 Solutions Chapter 6: Focus On Concepts:,,, Probles: 8, 4, 4, 43, 5, 54, 66, 8, 85 Focus On Concepts 6- (b) Work is positive when the orce has a coponent in the direction o the displaceent.

More information

U V. r In Uniform Field the Potential Difference is V Ed

U V. r In Uniform Field the Potential Difference is V Ed SPHI/W nit 7.8 Electric Potential Page of 5 Notes Physics Tool box Electric Potential Energy the electric potential energy stored in a syste k of two charges and is E r k Coulobs Constant is N C 9 9. E

More information

EFFECT OF WALL REINFORCEMENTS, APPLIED LATERAL FORCES AND VERTICAL AXIAL LOADS ON SEISMIC BEHAVIOR OF CONFINED CONCRETE MASONRY WALLS

EFFECT OF WALL REINFORCEMENTS, APPLIED LATERAL FORCES AND VERTICAL AXIAL LOADS ON SEISMIC BEHAVIOR OF CONFINED CONCRETE MASONRY WALLS EFFECT OF WALL REINFORCEMENTS, APPLIED LATERAL FORCES AND VERTICAL AXIAL LOADS ON SEISMIC BEHAVIOR OF CONFINED CONCRETE MASONRY WALLS 984 Koji YOSHIMURA 1, Kenji KIKUCHI 2, Masauki KUROKI 3, Lizhen LIU

More information

Surface Water and Stream Development

Surface Water and Stream Development Surface Water and Stream Development Surface Water The moment a raindrop falls to earth it begins its return to the sea. Once water reaches Earth s surface it may evaporate back into the atmosphere, soak

More information

SPH4U. Conservation of Energy. Review: Springs. More Spring Review. 1-D Variable Force Example: Spring. Page 1. For a spring we recall that F x = -kx.

SPH4U. Conservation of Energy. Review: Springs. More Spring Review. 1-D Variable Force Example: Spring. Page 1. For a spring we recall that F x = -kx. -D Variable Force Exaple: Spring SPH4U Conseration of Energ For a spring we recall that F x = -kx. F(x) x x x relaxe position -kx F = - k x the ass F = - k x Reiew: Springs Hooke s Law: The force exerte

More information

P10.5 Water flows down a rectangular channel that is 4 ft wide and 3 ft deep. The flow rate is 15,000 gal/min. Estimate the Froude number of the flow.

P10.5 Water flows down a rectangular channel that is 4 ft wide and 3 ft deep. The flow rate is 15,000 gal/min. Estimate the Froude number of the flow. P10.5 Water flows down a rectangular channel that is 4 ft wide and ft deep. The flow rate is 15,000 gal/min. Estimate the Froude number of the flow. Solution: Convert the flow rate from 15,000 gal/min

More information

USEFUL HINTS FOR SOLVING PHYSICS OLYMPIAD PROBLEMS. By: Ian Blokland, Augustana Campus, University of Alberta

USEFUL HINTS FOR SOLVING PHYSICS OLYMPIAD PROBLEMS. By: Ian Blokland, Augustana Campus, University of Alberta 1 USEFUL HINTS FOR SOLVING PHYSICS OLYMPIAD PROBLEMS By: Ian Bloland, Augustana Capus, University of Alberta For: Physics Olypiad Weeend, April 6, 008, UofA Introduction: Physicists often attept to solve

More information

Chapter 10 Atmospheric Forces & Winds

Chapter 10 Atmospheric Forces & Winds Chapter 10 Atospheric Forces & Winds Chapter overview: Atospheric Pressure o Horizontal pressure variations o Station vs sea level pressure Winds and weather aps Newton s 2 nd Law Horizontal Forces o Pressure

More information

Year 12 Physics Holiday Work

Year 12 Physics Holiday Work Year 1 Physics Holiday Work 1. Coplete questions 1-8 in the Fields assessent booklet and questions 1-3 In the Further Mechanics assessent booklet (repeated below in case you have lost the booklet).. Revise

More information

Advanced Hydraulics Prof. Dr. Suresh A Kartha Department of Civil Engineering Indian Institute of Technology, Guwahati

Advanced Hydraulics Prof. Dr. Suresh A Kartha Department of Civil Engineering Indian Institute of Technology, Guwahati Advanced Hydraulics Prof. Dr. Suresh A Kartha Department of Civil Engineering Indian Institute of Technology, Guwahati Module - 2 Uniform Flows Lecture - 6 Design of Channels for Uniform Flow (Refer Slide

More information

9. Flood Routing. chapter Two

9. Flood Routing. chapter Two 9. Flood Routing Flow routing is a mathematical procedure for predicting the changing magnitude, speed, and shape of a flood wave as a function of time at one or more points along a watercourse (waterway

More information

Chapter 4 Transport of Pollutants

Chapter 4 Transport of Pollutants 4- Introduction Phs. 645: Environmental Phsics Phsics Department Yarmouk Universit hapter 4 Transport of Pollutants - e cannot avoid the production of pollutants. hat can we do? - Transform pollutants

More information

Support Vector Machines MIT Course Notes Cynthia Rudin

Support Vector Machines MIT Course Notes Cynthia Rudin Support Vector Machines MIT 5.097 Course Notes Cynthia Rudin Credit: Ng, Hastie, Tibshirani, Friedan Thanks: Şeyda Ertekin Let s start with soe intuition about argins. The argin of an exaple x i = distance

More information

SPATIAL AND TEMPORAL DISTRIBUTIONS OF MIGRATION IN BIO-RETENTION SYSTEMS

SPATIAL AND TEMPORAL DISTRIBUTIONS OF MIGRATION IN BIO-RETENTION SYSTEMS Li, Y.-Q., et al.: Spatial and Teporal Distributions of Moisture THERMAL SCIENCE, Year 04, Vol. 8, No. 5, pp. 557-56 557 SPATIAL AND TEMPORAL DISTRIBUTIONS OF MIGRATION IN BIO-RETENTION SYSTEMS by Yu-Qi

More information

E0 370 Statistical Learning Theory Lecture 6 (Aug 30, 2011) Margin Analysis

E0 370 Statistical Learning Theory Lecture 6 (Aug 30, 2011) Margin Analysis E0 370 tatistical Learning Theory Lecture 6 (Aug 30, 20) Margin Analysis Lecturer: hivani Agarwal cribe: Narasihan R Introduction In the last few lectures we have seen how to obtain high confidence bounds

More information

2002 University of Porto, Faculty of Engineering (FEUP)

2002 University of Porto, Faculty of Engineering (FEUP) Holberg H, Ahtila P. Drying phenoenon in a fixed bed under the bio fuel ulti stage drying. In: Oliveira A, Afonso C, Riffat S, editors. Proceedings of the st International Conference on Sustainable Energy

More information

Hydraulics for Urban Storm Drainage

Hydraulics for Urban Storm Drainage Urban Hydraulics Hydraulics for Urban Storm Drainage Learning objectives: understanding of basic concepts of fluid flow and how to analyze conduit flows, free surface flows. to analyze, hydrostatic pressure

More information

What about water... What about open channel flow... Continuity Equation. HECRAS Basic Principles of Water Surface Profile Computations

What about water... What about open channel flow... Continuity Equation. HECRAS Basic Principles of Water Surface Profile Computations What about water... HECRA Basic Principles o Water urace Proile Computations b G. Parodi WR ITC The Netherlands Incompressible luid must increase or decrease its velocit and depth to adjust to the channel

More information

1 k. 1 m. m A. AP Physics Multiple Choice Practice Work-Energy

1 k. 1 m. m A. AP Physics Multiple Choice Practice Work-Energy AP Physics Multiple Choice Practice Wor-Energy 1. A ass attached to a horizontal assless spring with spring constant, is set into siple haronic otion. Its axiu displaceent fro its equilibriu position is

More information

Particle dynamics Physics 1A, UNSW

Particle dynamics Physics 1A, UNSW 1 Particle dynaics Physics 1A, UNSW Newton's laws: S & J: Ch 5.1 5.9, 6.1 force, ass, acceleration also weight Physclips Chapter 5 Friction - coefficients of friction Physclips Chapter 6 Hooke's Law Dynaics

More information

Newton's Laws. Lecture 2 Key Concepts. Newtonian mechanics and relation to Kepler's laws The Virial Theorem Tidal forces Collision physics

Newton's Laws. Lecture 2 Key Concepts. Newtonian mechanics and relation to Kepler's laws The Virial Theorem Tidal forces Collision physics Lecture 2 Key Concepts Newtonian echanics and relation to Kepler's laws The Virial Theore Tidal forces Collision physics Newton's Laws 1) An object at rest will reain at rest and an object in otion will

More information

Fluvial Dynamics. M. I. Bursik ublearns.buffalo.edu October 26, Home Page. Title Page. Contents. Page 1 of 18. Go Back. Full Screen. Close.

Fluvial Dynamics. M. I. Bursik ublearns.buffalo.edu October 26, Home Page. Title Page. Contents. Page 1 of 18. Go Back. Full Screen. Close. Page 1 of 18 Fluvial Dynamics M. I. Bursik ublearns.buffalo.edu October 26, 2008 1. Fluvial Dynamics We want to understand a little of the basic physics of water flow and particle transport, as so much

More information

Effect of Polymer Solutions on Efflux Time for Two Exit Pipe System

Effect of Polymer Solutions on Efflux Time for Two Exit Pipe System Effect of Polyer Solutions on Efflux Tie for Two Exit Pipe Syste Abstract: A. UMA DEVI a, D.V. PADMA a & CH. V. SUBBARAO a a Departent of Cheical Engineering, MVGR College of Engineering, Vizianagara-535005,

More information

12 SWAT USER S MANUAL, VERSION 98.1

12 SWAT USER S MANUAL, VERSION 98.1 12 SWAT USER S MANUAL, VERSION 98.1 CANOPY STORAGE. Canopy storage is the water intercepted by vegetative surfaces (the canopy) where it is held and made available for evaporation. When using the curve

More information

LECTURE NOTES - VIII. Prof. Dr. Atıl BULU

LECTURE NOTES - VIII. Prof. Dr. Atıl BULU LECTURE NOTES - VIII «LUID MECHNICS» Istanbul Technical Universit College of Civil Engineering Civil Engineering Department Hdraulics Division CHPTER 8 DIMENSIONL NLYSIS 8. INTRODUCTION Dimensional analsis

More information

MAKE SURE TA & TI STAMPS EVERY PAGE BEFORE YOU START

MAKE SURE TA & TI STAMPS EVERY PAGE BEFORE YOU START Laboratory Section: Last Revised on Deceber 15, 2014 Partners Naes: Grade: EXPERIMENT 8 Electron Beas 0. Pre-Laboratory Work [2 pts] 1. Nae the 2 forces that are equated in order to derive the charge to

More information

Question number 1 to 8 carries 2 marks each, 9 to 16 carries 4 marks each and 17 to 18 carries 6 marks each.

Question number 1 to 8 carries 2 marks each, 9 to 16 carries 4 marks each and 17 to 18 carries 6 marks each. IIT-JEE5-PH-1 FIITJEE Solutions to IITJEE 5 Mains Paper Tie: hours Physics Note: Question nuber 1 to 8 carries arks each, 9 to 16 carries 4 arks each and 17 to 18 carries 6 arks each. Q1. whistling train

More information

NEET-UG 2013 TEST PAPER WITH SOLUTIONS (HELD ON SUNDAY 05 th MAY, 2013)

NEET-UG 2013 TEST PAPER WITH SOLUTIONS (HELD ON SUNDAY 05 th MAY, 2013) 9. In Young's double slit experient, the slits are apart and are illuinated by photons of two wavelengths = Å and = Å. t what iniu distance fro the coon central bright fringe on the screen fro the slit

More information