3. Gradually-Varied Flow

Size: px
Start display at page:

Download "3. Gradually-Varied Flow"

Transcription

1 5/6/18 3. Gradually-aried Flow Normal Flow vs Gradually-aried Flow Normal Flow /g EGL (energy grade line) iction slope Geometric slope S Normal flow: Downslope component of weigt balances bed friction Uniform dept ( dept ) and velocity Bed slope or geometric slope (S ) is te same as te slope of te total ead line or friction slope ( ) Preferred dept, to wic flow tends given sufficient fetc 1

2 5/6/18 Gradually-aried Flow GF RF GF RF GF RF GF RF GF UF sluice gate ydraulic jump weir cange of slope Gradually-varied flow (GF): Component of weigt does not balance bed friction Geometric slope (S ) is different from friction slope ( ) Dept canges wit distance Te gradually-varied-flow equation gives te cange of dept wit distance Gradually-aried-Flow Equation 1 Assumptions: Small slopes Quasi-1d Hydrostatic pressure Depends on: Difference between geometric and friction slopes (S ) Sub- or supercritical flow () Derivation of te Gradually- aried Flow Equation

3 5/6/18 Derivation of te GF Equation (1) Total ead: H zs zb g g H z b E z s z b cos g dh dzb Define: GF equation (specific-energy form): dh dz b S d x friction slope geometric slope S S f Derivation of te GF Equation () Specific energy: E g Q E ga Q da 3 ga Q bs (1 ) 3 ga (1 ) g d S (1 S f ) GF equation (dept form): Q A da b s d A b s 1 S d x bs A Finding te iction Slope 3

4 5/6/18 Finding te iction Slope, 1 Quasi-uniform-flow assumption: rate of energy loss is te same as uniform flow of te same dept. 1 R n n S 4/3 R / 3 1/ n Q 4/3 R A function of dept f, greater dept lower velocity smaller smaller dept iger velocity greater Profile Classification Slope Classification Critical dept c : dept at wic = 1. Normal dept : dept of uniform flow. e.g. wide cannel: c ( q / g ) 1/ 3 ( nq / S ) 3/ 5 (For a given discarge) a slope is: steep, if te dept is less tan te critical dept (i.e. te flow is supercritical) mild, if te dept is greater tan te critical dept (i.e. te flow is subcritical) 4

5 5/6/18 Canging Dept 1 S > if and only if is greater tan dept 1 > if and only if is greater tan critical dept dept decreasing if and only if lies between and critical depts. Water-Profile Classification caracters (e.g. S1, M3 etc.): S, C, M, H, A (Steep, Critical, Mild, Horizontal, Adverse) 1,, 3 (were lies wit respect to c and ) Type Symbol Definition Sketces Examples S1 > c > c S1 Hydraulic jump upstream wit obstruction or reservoir controlling water level downstream. STEEP ( flow supercritical) S c > > n S S3 Cange to steeper slope. S3 c > > Cange to less steep slope. CRITICAL C1 > c = c= n C1 (undesirable; undular unsteady C3 flow) C3 c = > M1 > > c n M1 Obstruction or reservoir controlling water level downstream. MILD ( flow M > > c c M Approac to free overfall. subcritical) M3 M3 > c > Hydraulic jump downstream; cange from steep to mild slope or downstream of sluice. HORIZONTAL H > c H Approac to free overfall. (limiting mild c slope; ) H3 c > H3 Hydraulic jump downstream; cange from steep to orizontal or downstream of sluice. A > c A ADERSE (upslope) c A3 A3 c > 5

6 5/6/18 Qualitative Examples of Open- Cannel-Flow Beaviour Control Points Definition: locations at wic tere is a known relationsip between dept and flow rate (stage-discarge relationsip) Examples: Critical flow points: weir, venturi, free overfall,... Sluices Entry/exit from reservoir Hydraulic jump A control point often yields a boundary condition from wic to start a GF calculation General Principles Supercritical controlled by upstream conditions. Subcritical controlled by downstream conditions. Given a long-enoug fetc te flow will try to revert to flow. A ydraulic jump occurs between regions of supercritical and subcritical gradually-varied flow at te point were te jump condition for te sequent depts is correct. Were te slope is mild (i.e. te flow is subcritical), and any downstream control is far away, a ydraulic jump can be assumed to jump directly to te dept. 6

7 5/6/18 Qualitative Examples: Weir (Mild Slope) M1 1 c WEIR M3 ydraulic jump Qualitative Examples: Sluice Mild slope M1 1 M3 ydraulic jump Steep slope S1 1 S3 Qualitative Examples: Flow om Reservoir Mild slope RESEROIR Steep slope RESEROIR c S 7

8 5/6/18 Qualitative Examples M1 Flow into reservoir (mild slope) RESEROIR ee overfall (mild slope) M c critical Numerical Solution of te GF Equation Te GF Equation Tree forms: Total ead: Specific energy: Dept: dh d x S S 1 f 8

9 5/6/18 Solving Te GF Equation 1 Impossible to solve analytically (in most circumstances) Find depts 1,, 3, at discrete points x 1, x, x 3, approximated by Δ Δx were Δ i1 i Δx x i1 x i Starting Point and Direction 1 Start at a control point. Proceed: Forward in x if supercritical (upstream control); flow Backward in x if subcritical (downstream control). flow Types of Metod 1 1. Standard-step metods Solve for dept i at fixed distance intervals Δx x x x x. Direct-step metods Solve for distance x i at fixed eigt intervals Δ 1 S x x 1 x x 3 9

10 5/6/18 Standard-Step Metod: Total Head x x x x dh H zb g H i H i Δx S ( S 1 f, i f, i1 Adjust dept i+1 (iteratively) at eac step until LHS = RHS. ) Direct-Step Metod: Specific Energy x x 1 x x 3 S d x E g 1 S ΔE Δx ( S ) av ΔE E i E 1 i Direct-Step Metod: Dept x x 1 x x3 1 1 S Δx av Δ Write n S f R 4/3 g as functions of 1

11 5/6/18 Example A long, wide cannel as a slope of 1:747 wit a Manning s n of.15 m 1/3 s. It carries a discarge of.5 m 3 s 1 per metre widt, and tere is a free overfall at te downstream end. An undersot sluice is placed a certain distance upstream of te free overfall wic determines te nature of te flow between sluice and overfall. Te dept just downstream of te sluice is.5 m. (a) Determine te critical dept and dept. (b) Sketc, wit explanation, te two possible gradually-varied flows between sluice and overfall. (c) Calculate te particular distance between sluice and overfall wic determines te boundary between tese two flows. Use one step in te gradually-varied-flow equation. Direct-Step Metod: Reprise x x 1 x x S Δx av Δ 1 /3 R S n g 1/ n S f R 4/3 Q A A b s Example A sluice gate discarges water at 9 m 3 s 1 into a 6 m wide rectangular cannel laid on a slope of.4 wit n =.15 m 1/3 s. Te dept at te vena contracta is.15 m. (a) Find te and critical depts. (b) Compute te position of te ydraulic jump, assuming dept downstream. Use one step in te GF equation. 11

12 5/6/18 Example An undersot sluice is used to control te flow of water in a long wide cannel of slope.3 and Manning s rougness coefficient.1 m 1/3 s. Te flow rate in te cannel is m 3 s 1 per metre widt. (a) Calculate te dept and critical dept in te cannel and sow tat te cannel is ydrodynamically steep at tis flow rate. (b) Te dept of flow just downstream of te sluice is.4 m. Assuming no ead losses at te sluice calculate te dept just upstream of te sluice. (c) Sketc te dept profile along te cannel, indicating clearly any flow transitions brougt about by te sluice and indicating were water dept is increasing or decreasing. (d) Use steps in te gradually-varied flow equation to determine ow far upstream of te sluice a ydraulic jump will occur. 1

Part 2: Introduction to Open-Channel Flow SPRING 2005

Part 2: Introduction to Open-Channel Flow SPRING 2005 Part : Introduction to Open-Cannel Flow SPRING 005. Te Froude number. Total ead and specific energy 3. Hydraulic jump. Te Froude Number Te main caracteristics of flows in open cannels are tat: tere is

More information

NOTES ON OPEN CHANNEL FLOW

NOTES ON OPEN CHANNEL FLOW NOTES ON OPEN CANNEL FLOW Prof. Marco Pilotti Facoltà di Ingegneria, Università degli Studi di Brescia Profili di moto permanente in un canale e in una serie di due canali - Boudine, 86 OPEN CANNEL FLOW:

More information

3. GRADUALLY-VARIED FLOW (GVF) AUTUMN EGL (energy grade line) weir change of slope

3. GRADUALLY-VARIED FLOW (GVF) AUTUMN EGL (energy grade line) weir change of slope 3. GRADUALLY-ARIED FLOW (GF) AUTUMN 17 3.1 Normal Flow vs Gradually-aried Flow /g EGL (eergy grade lie) ictio slope Geometric slope S I ormal flow te dowslope compoet of weigt balaces bed frictio. As a

More information

Gradually Varied Flow I+II. Hydromechanics VVR090

Gradually Varied Flow I+II. Hydromechanics VVR090 Gradually Varied Flow I+II Hydromechanics VVR090 Gradually Varied Flow Depth of flow varies with longitudinal distance. Occurs upstream and downstream control sections. Governing equation: dy dx So Sf

More information

Open Channel Hydraulic

Open Channel Hydraulic Open Cannel Hydraulic Julien Caucat Associate Professor - Grenoble INP / ENSE3 - LEGI UMR 5519 julien.caucat@grenoble-inp.fr Winter session - 2015/2016 julien.caucat@grenoble-inp.fr Open Cannel Hydraulic

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

Introduction to Derivatives

Introduction to Derivatives Introduction to Derivatives 5-Minute Review: Instantaneous Rates and Tangent Slope Recall te analogy tat we developed earlier First we saw tat te secant slope of te line troug te two points (a, f (a))

More information

Hydromechanics: Course Summary

Hydromechanics: Course Summary Hydromechanics: Course Summary Hydromechanics VVR090 Material Included; French: Chapters to 9 and 4 + Sample problems Vennard & Street: Chapters 8 + 3, and (part of it) Roberson & Crowe: Chapter Collection

More information

Precalculus Test 2 Practice Questions Page 1. Note: You can expect other types of questions on the test than the ones presented here!

Precalculus Test 2 Practice Questions Page 1. Note: You can expect other types of questions on the test than the ones presented here! Precalculus Test 2 Practice Questions Page Note: You can expect oter types of questions on te test tan te ones presented ere! Questions Example. Find te vertex of te quadratic f(x) = 4x 2 x. Example 2.

More information

Chapter 1 Functions and Graphs. Section 1.5 = = = 4. Check Point Exercises The slope of the line y = 3x+ 1 is 3.

Chapter 1 Functions and Graphs. Section 1.5 = = = 4. Check Point Exercises The slope of the line y = 3x+ 1 is 3. Capter Functions and Graps Section. Ceck Point Exercises. Te slope of te line y x+ is. y y m( x x y ( x ( y ( x+ point-slope y x+ 6 y x+ slope-intercept. a. Write te equation in slope-intercept form: x+

More information

A PHYSICAL MODEL STUDY OF SCOURING EFFECTS ON UPSTREAM/DOWNSTREAM OF THE BRIDGE

A PHYSICAL MODEL STUDY OF SCOURING EFFECTS ON UPSTREAM/DOWNSTREAM OF THE BRIDGE A PHYSICA MODE STUDY OF SCOURING EFFECTS ON UPSTREAM/DOWNSTREAM OF THE BRIDGE JIHN-SUNG AI Hydrotec Researc Institute, National Taiwan University Taipei, 1617, Taiwan HO-CHENG IEN National Center for Hig-Performance

More information

Parshall Flume Discharge Relation under Free Flow Condition

Parshall Flume Discharge Relation under Free Flow Condition Journal omepage: ttp://www.journalijar.com INTERNATIONAL JOURNAL OF ADVANCED RESEARCH RESEARCH ARTICLE Parsall Flume Discarge Relation under Free Flow Condition 1 Jalam Sing, 2 S.K.Mittal, and 3 H.L.Tiwari

More information

REVIEW LAB ANSWER KEY

REVIEW LAB ANSWER KEY REVIEW LAB ANSWER KEY. Witout using SN, find te derivative of eac of te following (you do not need to simplify your answers): a. f x 3x 3 5x x 6 f x 3 3x 5 x 0 b. g x 4 x x x notice te trick ere! x x g

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

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

Hydraulic Evaluation of Discharge Over Rock Closing Dams on the Upper Mississippi River

Hydraulic Evaluation of Discharge Over Rock Closing Dams on the Upper Mississippi River ydraulic Evaluation of Discarge Over Rock Closing Dams on te Upper Mississippi River Jon endrickson, P.E. Senior ydraulic Engineer, St Paul District Introduction Prototype data was used for calibrating

More information

Critical control in transcritical shallow-water flow over two obstacles

Critical control in transcritical shallow-water flow over two obstacles Lougboroug University Institutional Repository Critical control in transcritical sallow-water flow over two obstacles Tis item was submitted to Lougboroug University's Institutional Repository by te/an

More information

Section 15.6 Directional Derivatives and the Gradient Vector

Section 15.6 Directional Derivatives and the Gradient Vector Section 15.6 Directional Derivatives and te Gradient Vector Finding rates of cange in different directions Recall tat wen we first started considering derivatives of functions of more tan one variable,

More information

Bob Brown Math 251 Calculus 1 Chapter 3, Section 1 Completed 1 CCBC Dundalk

Bob Brown Math 251 Calculus 1 Chapter 3, Section 1 Completed 1 CCBC Dundalk Bob Brown Mat 251 Calculus 1 Capter 3, Section 1 Completed 1 Te Tangent Line Problem Te idea of a tangent line first arises in geometry in te context of a circle. But before we jump into a discussion of

More information

Bed form characteristics in a live bed alluvial channel

Bed form characteristics in a live bed alluvial channel Scientia Iranica A (2014) 21(6), 1773{1780 Sarif University of Tecnology Scientia Iranica Transactions A: Civil Engineering www.scientiairanica.com Bed form caracteristics in a live bed alluvial cannel

More information

2.2 Derivative. 1. Definition of Derivative at a Point: The derivative of the function f x at x a is defined as

2.2 Derivative. 1. Definition of Derivative at a Point: The derivative of the function f x at x a is defined as . Derivative. Definition of Derivative at a Point: Te derivative of te function f at a is defined as f fa fa a lim provided te limit eists. If te limit eists, we sa tat f is differentiable at a, oterwise,

More information

The Derivative The rate of change

The Derivative The rate of change Calculus Lia Vas Te Derivative Te rate of cange Knowing and understanding te concept of derivative will enable you to answer te following questions. Let us consider a quantity wose size is described by

More information

Numerical Differentiation

Numerical Differentiation Numerical Differentiation Finite Difference Formulas for te first derivative (Using Taylor Expansion tecnique) (section 8.3.) Suppose tat f() = g() is a function of te variable, and tat as 0 te function

More information

Distribution of reynolds shear stress in steady and unsteady flows

Distribution of reynolds shear stress in steady and unsteady flows University of Wollongong Researc Online Faculty of Engineering and Information Sciences - Papers: Part A Faculty of Engineering and Information Sciences 13 Distribution of reynolds sear stress in steady

More information

Chapters 19 & 20 Heat and the First Law of Thermodynamics

Chapters 19 & 20 Heat and the First Law of Thermodynamics Capters 19 & 20 Heat and te First Law of Termodynamics Te Zerot Law of Termodynamics Te First Law of Termodynamics Termal Processes Te Second Law of Termodynamics Heat Engines and te Carnot Cycle Refrigerators,

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

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

1. Which one of the following expressions is not equal to all the others? 1 C. 1 D. 25x. 2. Simplify this expression as much as possible.

1. Which one of the following expressions is not equal to all the others? 1 C. 1 D. 25x. 2. Simplify this expression as much as possible. 004 Algebra Pretest answers and scoring Part A. Multiple coice questions. Directions: Circle te letter ( A, B, C, D, or E ) net to te correct answer. points eac, no partial credit. Wic one of te following

More information

f a h f a h h lim lim

f a h f a h h lim lim Te Derivative Te derivative of a function f at a (denoted f a) is f a if tis it exists. An alternative way of defining f a is f a x a fa fa fx fa x a Note tat te tangent line to te grap of f at te point

More information

Math 102 TEST CHAPTERS 3 & 4 Solutions & Comments Fall 2006

Math 102 TEST CHAPTERS 3 & 4 Solutions & Comments Fall 2006 Mat 102 TEST CHAPTERS 3 & 4 Solutions & Comments Fall 2006 f(x+) f(x) 10 1. For f(x) = x 2 + 2x 5, find ))))))))) and simplify completely. NOTE: **f(x+) is NOT f(x)+! f(x+) f(x) (x+) 2 + 2(x+) 5 ( x 2

More information

2.11 That s So Derivative

2.11 That s So Derivative 2.11 Tat s So Derivative Introduction to Differential Calculus Just as one defines instantaneous velocity in terms of average velocity, we now define te instantaneous rate of cange of a function at a point

More information

Calculus I Homework: The Derivative as a Function Page 1

Calculus I Homework: The Derivative as a Function Page 1 Calculus I Homework: Te Derivative as a Function Page 1 Example (2.9.16) Make a careful sketc of te grap of f(x) = sin x and below it sketc te grap of f (x). Try to guess te formula of f (x) from its grap.

More information

1 The concept of limits (p.217 p.229, p.242 p.249, p.255 p.256) 1.1 Limits Consider the function determined by the formula 3. x since at this point

1 The concept of limits (p.217 p.229, p.242 p.249, p.255 p.256) 1.1 Limits Consider the function determined by the formula 3. x since at this point MA00 Capter 6 Calculus and Basic Linear Algebra I Limits, Continuity and Differentiability Te concept of its (p.7 p.9, p.4 p.49, p.55 p.56). Limits Consider te function determined by te formula f Note

More information

Week #15 - Word Problems & Differential Equations Section 8.2

Week #15 - Word Problems & Differential Equations Section 8.2 Week #1 - Word Problems & Differential Equations Section 8. From Calculus, Single Variable by Huges-Hallett, Gleason, McCallum et. al. Copyrigt 00 by Jon Wiley & Sons, Inc. Tis material is used by permission

More information

Time (hours) Morphine sulfate (mg)

Time (hours) Morphine sulfate (mg) Mat Xa Fall 2002 Review Notes Limits and Definition of Derivative Important Information: 1 According to te most recent information from te Registrar, te Xa final exam will be eld from 9:15 am to 12:15

More information

2.8 The Derivative as a Function

2.8 The Derivative as a Function .8 Te Derivative as a Function Typically, we can find te derivative of a function f at many points of its domain: Definition. Suppose tat f is a function wic is differentiable at every point of an open

More information

MAT 145. Type of Calculator Used TI-89 Titanium 100 points Score 100 possible points

MAT 145. Type of Calculator Used TI-89 Titanium 100 points Score 100 possible points MAT 15 Test #2 Name Solution Guide Type of Calculator Used TI-89 Titanium 100 points Score 100 possible points Use te grap of a function sown ere as you respond to questions 1 to 8. 1. lim f (x) 0 2. lim

More information

1 Limits and Continuity

1 Limits and Continuity 1 Limits and Continuity 1.0 Tangent Lines, Velocities, Growt In tion 0.2, we estimated te slope of a line tangent to te grap of a function at a point. At te end of tion 0.3, we constructed a new function

More information

Math 34A Practice Final Solutions Fall 2007

Math 34A Practice Final Solutions Fall 2007 Mat 34A Practice Final Solutions Fall 007 Problem Find te derivatives of te following functions:. f(x) = 3x + e 3x. f(x) = x + x 3. f(x) = (x + a) 4. Is te function 3t 4t t 3 increasing or decreasing wen

More information

Comment on Experimental observations of saltwater up-coning

Comment on Experimental observations of saltwater up-coning 1 Comment on Experimental observations of saltwater up-coning H. Zang 1,, D.A. Barry 2 and G.C. Hocking 3 1 Griffit Scool of Engineering, Griffit University, Gold Coast Campus, QLD 4222, Australia. Tel.:

More information

Solutions Manual for Precalculus An Investigation of Functions

Solutions Manual for Precalculus An Investigation of Functions Solutions Manual for Precalculus An Investigation of Functions David Lippman, Melonie Rasmussen 1 st Edition Solutions created at Te Evergreen State College and Soreline Community College 1.1 Solutions

More information

= 0 and states ''hence there is a stationary point'' All aspects of the proof dx must be correct (c)

= 0 and states ''hence there is a stationary point'' All aspects of the proof dx must be correct (c) Paper 1: Pure Matematics 1 Mark Sceme 1(a) (i) (ii) d d y 3 1x 4x x M1 A1 d y dx 1.1b 1.1b 36x 48x A1ft 1.1b Substitutes x = into teir dx (3) 3 1 4 Sows d y 0 and states ''ence tere is a stationary point''

More information

Section 2.7 Derivatives and Rates of Change Part II Section 2.8 The Derivative as a Function. at the point a, to be. = at time t = a is

Section 2.7 Derivatives and Rates of Change Part II Section 2.8 The Derivative as a Function. at the point a, to be. = at time t = a is Mat 180 www.timetodare.com Section.7 Derivatives and Rates of Cange Part II Section.8 Te Derivative as a Function Derivatives ( ) In te previous section we defined te slope of te tangent to a curve wit

More information

Combining functions: algebraic methods

Combining functions: algebraic methods Combining functions: algebraic metods Functions can be added, subtracted, multiplied, divided, and raised to a power, just like numbers or algebra expressions. If f(x) = x 2 and g(x) = x + 2, clearly f(x)

More information

qwertyuiopasdfghjklzxcvbnmqwerty uiopasdfghjklzxcvbnmqwertyuiopasd fghjklzxcvbnmqwertyuiopasdfghjklzx cvbnmqwertyuiopasdfghjklzxcvbnmq

qwertyuiopasdfghjklzxcvbnmqwerty uiopasdfghjklzxcvbnmqwertyuiopasd fghjklzxcvbnmqwertyuiopasdfghjklzx cvbnmqwertyuiopasdfghjklzxcvbnmq qwertyuiopasdfgjklzxcbnmqwerty uiopasdfgjklzxcbnmqwertyuiopasd fgjklzxcbnmqwertyuiopasdfgjklzx cbnmqwertyuiopasdfgjklzxcbnmq Projectile Motion Quick concepts regarding Projectile Motion wertyuiopasdfgjklzxcbnmqwertyui

More information

(4.2) -Richardson Extrapolation

(4.2) -Richardson Extrapolation (.) -Ricardson Extrapolation. Small-O Notation: Recall tat te big-o notation used to define te rate of convergence in Section.: Suppose tat lim G 0 and lim F L. Te function F is said to converge to L as

More information

Average Rate of Change

Average Rate of Change Te Derivative Tis can be tougt of as an attempt to draw a parallel (pysically and metaporically) between a line and a curve, applying te concept of slope to someting tat isn't actually straigt. Te slope

More information

HEADLOSS ESTIMATION. Mekanika Fluida 1 HST

HEADLOSS ESTIMATION. Mekanika Fluida 1 HST HEADLOSS ESTIMATION Mekanika Fluida HST Friction Factor : Major losses Laminar low Hagen-Poiseuille Turbulent (Smoot, Transition, Roug) Colebrook Formula Moody diagram Swamee-Jain 3 Laminar Flow Friction

More information

MATH1151 Calculus Test S1 v2a

MATH1151 Calculus Test S1 v2a MATH5 Calculus Test 8 S va January 8, 5 Tese solutions were written and typed up by Brendan Trin Please be etical wit tis resource It is for te use of MatSOC members, so do not repost it on oter forums

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

Section 3: The Derivative Definition of the Derivative

Section 3: The Derivative Definition of the Derivative Capter 2 Te Derivative Business Calculus 85 Section 3: Te Derivative Definition of te Derivative Returning to te tangent slope problem from te first section, let's look at te problem of finding te slope

More information

Click here to see an animation of the derivative

Click here to see an animation of the derivative Differentiation Massoud Malek Derivative Te concept of derivative is at te core of Calculus; It is a very powerful tool for understanding te beavior of matematical functions. It allows us to optimize functions,

More information

VARIED FLOW IN OPEN CHANNELS

VARIED FLOW IN OPEN CHANNELS Chapter 15 Open Channels vs. Closed Conduits VARIED FLOW IN OPEN CHANNELS Fluid Mechanics, Spring Term 2011 In a closed conduit there can be a pressure gradient that drives the flow. An open channel has

More information

Chapter 4: Non uniform flow in open channels

Chapter 4: Non uniform flow in open channels Chapter 4: Non uniform flow in open channels Learning outcomes By the end of this lesson, students should be able to: Relate the concept of specific energy and momentum equations in the effect of change

More information

University of Alabama Department of Physics and Astronomy PH 101 LeClair Summer Exam 1 Solutions

University of Alabama Department of Physics and Astronomy PH 101 LeClair Summer Exam 1 Solutions University of Alabama Department of Pysics and Astronomy PH 101 LeClair Summer 2011 Exam 1 Solutions 1. A motorcycle is following a car tat is traveling at constant speed on a straigt igway. Initially,

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

Lecture XVII. Abstract We introduce the concept of directional derivative of a scalar function and discuss its relation with the gradient operator.

Lecture XVII. Abstract We introduce the concept of directional derivative of a scalar function and discuss its relation with the gradient operator. Lecture XVII Abstract We introduce te concept of directional derivative of a scalar function and discuss its relation wit te gradient operator. Directional derivative and gradient Te directional derivative

More information

MVT and Rolle s Theorem

MVT and Rolle s Theorem AP Calculus CHAPTER 4 WORKSHEET APPLICATIONS OF DIFFERENTIATION MVT and Rolle s Teorem Name Seat # Date UNLESS INDICATED, DO NOT USE YOUR CALCULATOR FOR ANY OF THESE QUESTIONS In problems 1 and, state

More information

Some Review Problems for First Midterm Mathematics 1300, Calculus 1

Some Review Problems for First Midterm Mathematics 1300, Calculus 1 Some Review Problems for First Midterm Matematics 00, Calculus. Consider te trigonometric function f(t) wose grap is sown below. Write down a possible formula for f(t). Tis function appears to be an odd,

More information

A = h w (1) Error Analysis Physics 141

A = h w (1) Error Analysis Physics 141 Introduction In all brances of pysical science and engineering one deals constantly wit numbers wic results more or less directly from experimental observations. Experimental observations always ave inaccuracies.

More information

1 Power is transferred through a machine as shown. power input P I machine. power output P O. power loss P L. What is the efficiency of the machine?

1 Power is transferred through a machine as shown. power input P I machine. power output P O. power loss P L. What is the efficiency of the machine? 1 1 Power is transferred troug a macine as sown. power input P I macine power output P O power loss P L Wat is te efficiency of te macine? P I P L P P P O + P L I O P L P O P I 2 ir in a bicycle pump is

More information

. h I B. Average velocity can be interpreted as the slope of a tangent line. I C. The difference quotient program finds the exact value of f ( a)

. h I B. Average velocity can be interpreted as the slope of a tangent line. I C. The difference quotient program finds the exact value of f ( a) Capter Review Packet (questions - ) KEY. In eac case determine if te information or statement is correct (C) or incorrect (I). If it is incorrect, include te correction. f ( a ) f ( a) I A. represents

More information

Polynomial Functions. Linear Functions. Precalculus: Linear and Quadratic Functions

Polynomial Functions. Linear Functions. Precalculus: Linear and Quadratic Functions Concepts: definition of polynomial functions, linear functions tree representations), transformation of y = x to get y = mx + b, quadratic functions axis of symmetry, vertex, x-intercepts), transformations

More information

Poisson Equation in Sobolev Spaces

Poisson Equation in Sobolev Spaces Poisson Equation in Sobolev Spaces OcMountain Dayligt Time. 6, 011 Today we discuss te Poisson equation in Sobolev spaces. It s existence, uniqueness, and regularity. Weak Solution. u = f in, u = g on

More information

Fluids and Buoyancy. 1. What will happen to the scale reading as the mass is lowered?

Fluids and Buoyancy. 1. What will happen to the scale reading as the mass is lowered? Fluids and Buoyancy. Wat will appen to te scale reading as te mass is lowered? M Using rcimedes Principle: any body fully or partially submerged in a fluid is buoyed up by a force equal to te weigt of

More information

Derivative as Instantaneous Rate of Change

Derivative as Instantaneous Rate of Change 43 Derivative as Instantaneous Rate of Cange Consider a function tat describes te position of a racecar moving in a straigt line away from some starting point Let y s t suc tat t represents te time in

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

. Compute the following limits.

. Compute the following limits. Today: Tangent Lines and te Derivative at a Point Warmup:. Let f(x) =x. Compute te following limits. f( + ) f() (a) lim f( +) f( ) (b) lim. Let g(x) = x. Compute te following limits. g(3 + ) g(3) (a) lim

More information

LIMITS AND DERIVATIVES CONDITIONS FOR THE EXISTENCE OF A LIMIT

LIMITS AND DERIVATIVES CONDITIONS FOR THE EXISTENCE OF A LIMIT LIMITS AND DERIVATIVES Te limit of a function is defined as te value of y tat te curve approaces, as x approaces a particular value. Te limit of f (x) as x approaces a is written as f (x) approaces, as

More information

A general articulation angle stability model for non-slewing articulated mobile cranes on slopes *

A general articulation angle stability model for non-slewing articulated mobile cranes on slopes * tecnical note 3 general articulation angle stability model for non-slewing articulated mobile cranes on slopes * J Wu, L uzzomi and M Hodkiewicz Scool of Mecanical and Cemical Engineering, University of

More information

absolute gauge atmospheric 2

absolute gauge atmospheric 2 Pressure and Manometers. Wat will be te (a) te gauge pressure and (b) te absolute pressure of water at dept m below te surface? ρ water 000 kg/m, and p atmospere 0kN/m. [7.7 kn/m, 8.7 kn/m ] a) b) p gauge

More information

Higher Derivatives. Differentiable Functions

Higher Derivatives. Differentiable Functions Calculus 1 Lia Vas Higer Derivatives. Differentiable Functions Te second derivative. Te derivative itself can be considered as a function. Te instantaneous rate of cange of tis function is te second derivative.

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

Continuous formulation for bottom friction in free surface flows modelling

Continuous formulation for bottom friction in free surface flows modelling River Basin Management V 81 Continuous formulation for bottom friction in free surface flows modelling O. Maciels 1, S. Erpicum 1, B. J. Dewals 1, 2, P. Arcambeau 1 & M. Pirotton 1 1 HACH Unit, Department

More information

Derivatives of Exponentials

Derivatives of Exponentials mat 0 more on derivatives: day 0 Derivatives of Eponentials Recall tat DEFINITION... An eponential function as te form f () =a, were te base is a real number a > 0. Te domain of an eponential function

More information

7.1 Using Antiderivatives to find Area

7.1 Using Antiderivatives to find Area 7.1 Using Antiderivatives to find Area Introduction finding te area under te grap of a nonnegative, continuous function f In tis section a formula is obtained for finding te area of te region bounded between

More information

MATH 3208 MIDTERM REVIEW. (B) {x 4 x 5 ; x ʀ} (D) {x x ʀ} Use the given functions to answer questions # 3 5. determine the value of h(7).

MATH 3208 MIDTERM REVIEW. (B) {x 4 x 5 ; x ʀ} (D) {x x ʀ} Use the given functions to answer questions # 3 5. determine the value of h(7). MATH 08 MIDTERM REVIEW. If () = (f + g)() wat is te domain of () { 5 4 ; ʀ} { 4 4 ; ʀ} { 4 5 ; ʀ} { ʀ}. Given p() = and g() = wic function represents k() k() = p() g() + + Use te given functions to answer

More information

Function Composition and Chain Rules

Function Composition and Chain Rules Function Composition and s James K. Peterson Department of Biological Sciences and Department of Matematical Sciences Clemson University Marc 8, 2017 Outline 1 Function Composition and Continuity 2 Function

More information

Mathematics 105 Calculus I. Exam 1. February 13, Solution Guide

Mathematics 105 Calculus I. Exam 1. February 13, Solution Guide Matematics 05 Calculus I Exam February, 009 Your Name: Solution Guide Tere are 6 total problems in tis exam. On eac problem, you must sow all your work, or oterwise torougly explain your conclusions. Tere

More information

1. Consider the trigonometric function f(t) whose graph is shown below. Write down a possible formula for f(t).

1. Consider the trigonometric function f(t) whose graph is shown below. Write down a possible formula for f(t). . Consider te trigonometric function f(t) wose grap is sown below. Write down a possible formula for f(t). Tis function appears to be an odd, periodic function tat as been sifted upwards, so we will use

More information

1. State whether the function is an exponential growth or exponential decay, and describe its end behaviour using limits.

1. State whether the function is an exponential growth or exponential decay, and describe its end behaviour using limits. Questions 1. State weter te function is an exponential growt or exponential decay, and describe its end beaviour using its. (a) f(x) = 3 2x (b) f(x) = 0.5 x (c) f(x) = e (d) f(x) = ( ) x 1 4 2. Matc te

More information

Applied Linear Statistical Models. Simultaneous Inference Topics. Simultaneous Estimation of β 0 and β 1 Issues. Simultaneous Inference. Dr.

Applied Linear Statistical Models. Simultaneous Inference Topics. Simultaneous Estimation of β 0 and β 1 Issues. Simultaneous Inference. Dr. Applied Linear Statistical Models Simultaneous Inference Dr. DH Jones Simultaneous Inference Topics Simultaneous estimation of β 0 and β 1 Bonferroni Metod Simultaneous estimation of several mean responses

More information

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

Section 2.1 The Definition of the Derivative. We are interested in finding the slope of the tangent line at a specific point.

Section 2.1 The Definition of the Derivative. We are interested in finding the slope of the tangent line at a specific point. Popper 6: Review of skills: Find tis difference quotient. f ( x ) f ( x) if f ( x) x Answer coices given in audio on te video. Section.1 Te Definition of te Derivative We are interested in finding te slope

More information

How to Find the Derivative of a Function: Calculus 1

How to Find the Derivative of a Function: Calculus 1 Introduction How to Find te Derivative of a Function: Calculus 1 Calculus is not an easy matematics course Te fact tat you ave enrolled in suc a difficult subject indicates tat you are interested in te

More information

Chezy s Resistance Coefficient in a Circular Conduit

Chezy s Resistance Coefficient in a Circular Conduit Send Orders for eprints to reprints@bentamscience.ae Te Open Civil Engineering Journal 2015 9 187-195 187 Cezy s esistance Coefficient in a Circular Conduit Open Access Bacir Acour esearc Laboratory in

More information

158 Calculus and Structures

158 Calculus and Structures 58 Calculus and Structures CHAPTER PROPERTIES OF DERIVATIVES AND DIFFERENTIATION BY THE EASY WAY. Calculus and Structures 59 Copyrigt Capter PROPERTIES OF DERIVATIVES. INTRODUCTION In te last capter you

More information

The derivative function

The derivative function Roberto s Notes on Differential Calculus Capter : Definition of derivative Section Te derivative function Wat you need to know already: f is at a point on its grap and ow to compute it. Wat te derivative

More information

Differential Calculus (The basics) Prepared by Mr. C. Hull

Differential Calculus (The basics) Prepared by Mr. C. Hull Differential Calculus Te basics) A : Limits In tis work on limits, we will deal only wit functions i.e. tose relationsips in wic an input variable ) defines a unique output variable y). Wen we work wit

More information

Laboratories of Applied Hydrodynamics and Hydraulic Constructions

Laboratories of Applied Hydrodynamics and Hydraulic Constructions Flood routing Laboratories of Applied Hydrodynamics and Hydraulic Constructions AIMS : Unsteady computation of floods in any comple network of rivers Any natural cross-sections Eplicit computation of floodplains

More information

Order of Accuracy. ũ h u Ch p, (1)

Order of Accuracy. ũ h u Ch p, (1) Order of Accuracy 1 Terminology We consider a numerical approximation of an exact value u. Te approximation depends on a small parameter, wic can be for instance te grid size or time step in a numerical

More information

11.6 DIRECTIONAL DERIVATIVES AND THE GRADIENT VECTOR

11.6 DIRECTIONAL DERIVATIVES AND THE GRADIENT VECTOR SECTION 11.6 DIRECTIONAL DERIVATIVES AND THE GRADIENT VECTOR 633 wit speed v o along te same line from te opposite direction toward te source, ten te frequenc of te sound eard b te observer is were c is

More information

lim 1 lim 4 Precalculus Notes: Unit 10 Concepts of Calculus

lim 1 lim 4 Precalculus Notes: Unit 10 Concepts of Calculus Syllabus Objectives: 1.1 Te student will understand and apply te concept of te limit of a function at given values of te domain. 1. Te student will find te limit of a function at given values of te domain.

More information

4.2 - Richardson Extrapolation

4.2 - Richardson Extrapolation . - Ricardson Extrapolation. Small-O Notation: Recall tat te big-o notation used to define te rate of convergence in Section.: Definition Let x n n converge to a number x. Suppose tat n n is a sequence

More information

NCCI: Simple methods for second order effects in portal frames

NCCI: Simple methods for second order effects in portal frames NCC: Simple metods for second order effects in portal frames NCC: Simple metods for second order effects in portal frames NCC: Simple metods for second order effects in portal frames Tis NCC presents information

More information

Continuity and Differentiability Worksheet

Continuity and Differentiability Worksheet Continuity and Differentiability Workseet (Be sure tat you can also do te grapical eercises from te tet- Tese were not included below! Typical problems are like problems -3, p. 6; -3, p. 7; 33-34, p. 7;

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

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

5.1 We will begin this section with the definition of a rational expression. We

5.1 We will begin this section with the definition of a rational expression. We Basic Properties and Reducing to Lowest Terms 5.1 We will begin tis section wit te definition of a rational epression. We will ten state te two basic properties associated wit rational epressions and go

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