Chapter 2 FLUID STATICS by Amat Sairin Demun

Similar documents
Headwater elevation water surface elevation just. Tailwater elevation water surface elevation just

Middle East Technical University Department of Mechanical Engineering ME 305 Fluid Mechanics I Fall 2018 Section 4 (Dr.

Tutorial 5 Relative equilibrium

Assistant Lecturer Anees Kadhum AL Saadi

γ water = 62.4 lb/ft 3 = 9800 N/m 3

Fluid Mechanics. Chapter Three: Fluid Statics. Dr. Amer Khalil Ababneh

Trigonometry. terminal ray

Module 3: Hydrostatic forces on submerged bodies Lecture 7: Calculation of horizontal component, buoyancy. Forces on submerged bodies (continued)

Chapter 3: Fluid Statics. 3-1 Pressure 3-2 Fluid Statics 3-3 Buoyancy and Stability 3-4 Rigid-Body Motion

5.8. Solving Three-Dimensional Problems by Using Trigonometry. LEARN ABOUT the Math. Matt s Solution. 328 Chapter 5

How can you compare lengths between the customary and metric systems? 6 ft. ACTIVITY: Customary Measure History

FC-CIV HIDRCANA: Channel Hydraulics Flow Mechanics Review Fluid Statics

HURRICANE SANDY LIMITED REEVALUATION REPORT UNION BEACH, NEW JERSEY DRAFT ENGINEERING APPENDIX SUB APPENDIX E OVERTOPPING & FAILURE ANALYSIS

γ water = 62.4 lb/ft 3 = 9800 N/m 3


ME 305 Fluid Mechanics I. Chapter 2 Fluid Statics

Danyal Education :,I. Unit 6 Pressure. A 1500kgm3 C 800kgm3. B 1000kgm3. D 500kgm3 ( ) D the packet has a small hole that allowed air to leak in.

3 1 PRESSURE. This is illustrated in Fig. 3 3.

Density and Specific Gravity

This chapter deals with forces applied by fluids at rest or in rigid-body

Homework of chapter (3)

Pressure Measurement

Lesson 12: Fluid statics, Continuity equation (Sections ) Chapter 9 Fluids

Areas of Trapezoids, Rhombuses, and Kites. To find the area of a trapezoid, rhombus, or kite

Chapter 13 Fluids. Copyright 2009 Pearson Education, Inc.

kpa := 1000 Pa p atm := 101 kpa := i is inside o is outside effects are small. R gas := M gas 1000 mol

Unit A-2: List of Subjects

Department of Civil & Geological Engineering GEOE Engineering Geology

Chapter 3 PRESSURE AND FLUID STATICS

Objectives deals with forces applied by fluids at rest or in rigid-body motion.

Pressure Measurement

PRESSURE. Pressure: A normal force exerted by a fluid per unit area

. In an elevator accelerating upward (A) both the elevator accelerating upward (B) the first is equations are valid

COURSE NUMBER: ME 321 Fluid Mechanics I Fluid statics. Course teacher Dr. M. Mahbubur Razzaque Professor Department of Mechanical Engineering BUET

Are You Ready? Pythagorean Theorem

and its weight (in newtons) when located on a planet with an acceleration of gravity equal to 4.0 ft/s 2.

APPENDICES STRANDJACK WEDGES Friction coefficients, micro slip and handling

Physics 20 Lesson 20 Uniform Circular Motion Vertical Plane

1. The principle of fluid pressure that is used in hydraulic brakes or lifts is that:

Planar Projectile Motion OBJECTIVES

Irrigation &Hydraulics Department lb / ft to kg/lit.

Contents PROOF. 1 Hydrostatics 1. 2 Pressure measurement 35. Preface to third edition. Acknowledgements. Principal notation.

Concept of Fluid. Density. Pressure: Pressure in a Fluid. Pascal s principle. Buoyancy. Archimede s Principle. Forces on submerged surfaces

Chapter 9 Fluids and Buoyant Force

Additional Information

Applications of Bernoulli s principle. Principle states that areas with faster moving fluids will experience less pressure

Assumptions 1 At specified conditions, air behaves as an ideal gas. 2 The volume of the tire remains constant.

Hours / 100 Marks Seat No.

When a uniform pressure acts on a flat plate of area A and a force F pushes the plate, then the pressure p is : p = F/A

Chapter 10 Fluids. Which has a greater density? Ch 10: Problem 5. Ch 10: Problem Phases of Matter Density and Specific Gravity

Sight Distance. The availability of sufficient sight distance for the driver to see ahead is critical to the design of a safe highway.

3. A fluid is forced through a pipe of changing cross section as shown. In which section would the pressure of the fluid be a minimum?

Comments on Homework. Quiz. Class 3 - Pressure. Atmospheric Pressure. 2. Gauge vs. Absolute Pressure. 1. Definitions. Temperature conversion

Lecture 19 Fluids: density, pressure, Pascal s principle and Buoyancy.

IMO REVIEW OF THE INTACT STABILITY CODE. Sample calculations using a wind criterion. Submitted by Germany. Resolution A.749 (18) and MSC.

Hydrostatic Force on a Submerged Surface

Sample Problems. Lecture Notes Motion Problems page 1

2. describe the airflow in high- and low-pressure systems, and explain how these motions create weather (pp );

Old-Exam.Questions-Ch-14 T072 T071

Properties of Fluids SPH4C

THERMODYNAMICS, HEAT AND MASS TRANSFER TUTORIAL NO: 1 (SPECIFIC VOLUME, PRESSURE AND TEMPERATURE)

Static Fluids. **All simulations and videos required for this package can be found on my website, here:

Third measurement MEASUREMENT OF PRESSURE

Quadratic Modeling Exercises

ME 425: AERODYNAMICS

KNOWN: Mass, pressure, temperature, and specific volume of water vapor.

PRESSURE. 7. Fluids 2

PHYSICS - CLUTCH CH 17: FLUID MECHANICS.

Experiment 8: Minor Losses

Fluid Statics. AP Physics 2

PHYS 101 Previous Exam Problems

AP B Fluids Practice Problems. Multiple Choice. Slide 2 / 43. Slide 1 / 43. Slide 4 / 43. Slide 3 / 43. Slide 6 / 43. Slide 5 / 43

Pressure is defined as force per unit area. Any fluid can exert a force

Variation of Pressure with Depth in a Fluid *

CVEN 311 Fluid Dynamics Fall Semester 2011 Dr. Kelly Brumbelow, Texas A&M University. Final Exam

BERMAD Irrigation. IR-100 hyflow Basic Valve. Basic Valve.

Comparison of the South Dakota Road Profiler with Other Rut Measurement Methods

1. Air is blown through a pipe AB at a rate of 15 litre per minute. The cross-sectional area of broad

1Photograph courtesy of A. F. Hasler [Ref. 7].2

1. All fluids are: A. gases B. liquids C. gases or liquids D. non-metallic E. transparent ans: C

2 Available: 1390/08/02 Date of returning: 1390/08/17 1. A suction cup is used to support a plate of weight as shown in below Figure. For the conditio

Gauge Pressure, Absolute Pressure, and Pressure Measurement

Comments on Homework. Class 4 - Pressure. Atmospheric Pressure. Gauge vs. Absolute Pressure. 2. Gauge vs. Absolute Pressure. 1.

Name. Student I.D.. Section:. Use g = 10 m/s 2

FLUID MECHANICS. Fluid Statics BUOYANCY. Fig. Buoyancy CENTER OF BUOYANCY

Young s modulus measurement of wood and CFRP

Unit code: H/ QCF level: 5 Credit value: 15 OUTCOME 3 - STATIC AND DYNAMIC FLUID SYSTEMS TUTORIAL 2 - STATIC FLUID SYSTEMS

EFFECTS OF DESIGN PARAMETERS ON WIND SPEED FOR LARGE THREE-BLADED UPWIND HORIZONTAL AXIS WIND TURBINE

Lab. Manual. Fluid Mechanics. The Department of Civil and Architectural Engineering

ACTIVITY 1: Buoyancy Problems. OBJECTIVE: Practice and Reinforce concepts related to Fluid Pressure, primarily Buoyancy

Phys101 Lectures Fluids I. Key points: Pressure and Pascal s Principle Buoyancy and Archimedes Principle. Ref: 10-1,2,3,4,5,6,7.

FLUID MECHANICS Time: 1 hour (ECE-301) Max. Marks :30

Chapter 2 Pressure Distribution in a Fluid

Fluids. James H Dann, Ph.D. Say Thanks to the Authors Click (No sign in required)

Ch. 4 Motion in One direction Ch 6. Pressure in Fluids and Atmospheric Pressure Ch. 7. Up-thrust in Fluids Ch. 8. Floatation and Relative Density

*Definition of Cosine

General Technical Data and Calculations

TABLE OF CONTENTS...2 APPENDIX A ANCHORHEADS...3 APPENDIX B WEDGE PROPERTIES...5 APPENDIX C

Exam Question 9: Hydrostatics. March 6, Applied Mathematics: Lecture 8. Brendan Williamson. Introduction. Density, Weight and Volume

Unit 7. Pressure in fluids

Transcription:

Capter FLUID STTICS by mat Sairin Demun Learning Outomes Upon ompleting tis apter, te students are expeted to be able to: 1. Calulate te pressure in pipes by using piezometers and manometers.. Calulate te ydrostati pressure fore for submerged plane surfaes (magnitude, loation and diretion and te related reation fore) inlined or vertial position.. Calulate te ydrostati pressure fore for submerged urved surfaes (magnitude, loation and diretion and te related reation fore). Study on non-moving fluid fluid at rest..1) Pressure Density Heigt Relationsip Pressure unit = N/m or Pa or Bar 1 kpa = 1 kn/m = 1000 Pa = 1000 N/m 1 Bar = 100 kpa P g = vertial eigt downward from te fluid surfae (m). If te fluid is gas or air, te pressure at all plaes are te same te pressure NOT depends on eigt. If someone says te pressure is 5 m Merury, means tat te pressure is: 1. 5710009. 81 0. 05 P g = 6.66 kpa.) Relationsip Between bsolute and Gauge Pressure P abs P gauge P atm atmosperi pressure = 101. kpa = 760 mm Hg

.) Pressure Measurements Various types of equipments used to measure pressure. 1. Barometer to measure atmosperi pressure.. neroid to measure air pressure in tyres.. Bourdon to measure fluid pressure. Bourdon pressure gauge to measure pressure of fluid in a pipe.. Piezometer to measure fluid pressure in pipes. 5. Manometers to measure fluid pressure in pipes, if piezometri tube is not pratial (pressure too ig) Te following figures sow examples of manometers.

SIMPLE MNOMETER DIFFERENTIL MNOMETER Calulation Proedures: 1. Divide te manometer into setions aording to te known vertial eigt.. Draw an arrow pointing DOWNWRD for ea of te setion.. For ea drawn arrow, mark (+) or ( ) sign. (+) for te arrow tat te diretion LEDS to te point were te pressure is to be known (referene point). ( ) for te arrow tat te diretion LEVES te referene point. If te sign is (+), te pressure for te arrow is +g and if te sign is ( ), te pressure for te arrow is g ; were is te vertial eigt of te setion ontaining te arrow wile is te fluid density in te manometer were te arrow is loated.. Canel two pressure wi ave te same magnitude but opposite diretion. Same magnitude means tat tey ave te same eigt and te same fluid density,. 5. Sum up all of te pressures taking te pressure at te referene point as te eading. If te manometer end is open, te pressure at te end is zero. If te manometer end is anoter pipe (for differential manometer), add (+) te pressure value.

.) Hydrostati Pressure Fore on Submerged Plane Surfaes Hydrostati pressure is te fore due to te fluid ating on te submerged plane surfae. Fore = Pressure x rea F = P = g unit = Newton (N) or kg.m/s Fore is a vetor tat must ave items: 1. Magnitude. Loation of at. Diretion n inlined submerged plane surfae, B is as sown in te following figure. Note:- C = Center of gravity of te Submerged Surfae G = Center of gravity of te wole Plane Surfae P = Center of Pressure (te plae were te pressure fore ats) Magnitude: F g = rea of te submerged surfae (m ). = Vertial eigt from te fluid surfae to te enter of gravity of te submerged plane surfae (C) (m). Loation: F is ating on te enter of pressure tat is at a vertial distane p from te fluid surfae were: I sin p were: = I =? te inlined angle (see figure) Moment of inertia about te orizontal line troug te enter of gravity of te submerged surfae (m ) see Table.1 Diretion: F ats at te plane surfae perpendiular (90 0 ) to te wetted surfae.

.5) Hydrostati Pressure Fore on Submerged Curved Surfaes Curved surfaes B submerged in a fluid are as sown in te following figures. Compare bot figures and spot te differenes. Two fore omponents: Horizontal fore and Vertial fore. 1) Horizontal Component, F H (a) Magnitude: F H is te fore equivalent to te fore ating on te vertial plane surfae projeted from te urved surfae (te retangular image). F H g = = area of te vertial plane surfae projeted from te urved surfae (area of te retangular image). vertial eigt from te fluid surfae to te enter of gravity of te vertial plane surfae projeted from te urved surfae (te image). (b) Loation: F H ats orizontally at te urved surfae troug te enter of pressure of te vertial plane surfae projeted from te urved surfae, tat is at te vertial eigt p from te fluid surfae, were: p I beause sin 90 0 = 1 (vertial plane surfae) I = Moment of inertia about te orizontal line troug te enter of te plane surfae projeted from te urved surfae. (m ) See Table.1. and is as (a) above.

) Vertial Component, F V (a) Magnitude: F V is te fore equivalent to te weigt of te fluid above te urved surfae. F V gv were, V = fluid volume above te urved surfae (m ) up to te fluid surfae line. (b) Loation: F V ats vertially at te urved surfae troug te enter of gravity of te fluid volume above te urved surfae (up to te fluid surfae), tat is at te orizontal distane x from a referene vertial line, were: x 1 x1 1 x ) Resultant Fore, F 1 = rea of sape 1 = rea of sape x 1 = orizontal distane from te enter of gravity of area 1 to te referene vertial line. x = orizontal distane from te enter of gravity of area to te referene vertial line. Te resultant fore of omponents F H and F V is: Magnitude: Loation: Diretion: F F H F V F ats at te urved surfae troug te intersetion point of F H and F V lines. F ats at an angle from orizontal; tan 1 F F V H.6 Te HSTTIC Computer Program HSTTIC stands for HydroSTTIC is a medium sized exeutable omputer program to solve any ydrostati pressure fore problem. It is developed by Mr. mat Sairin Demun using MS DOS based Fortran programming language. It is able to alulate te pressure fore and te reation fore of fluid ating on a submerged plane and urved surfaes. Te students an opy te file from Mr. mat Sairin Demun at no ost. To run te omputer program, te students will ave to double lik te HSTTIC file and just follow te instrutions appear on te omputer sreen. If you ave diffiulties running te omputer program, please feel free to ontat Mr. mat Sairin Demun.

TBLE.1: Geometri Properties of Plane Surfaes I I y Sape Sket rea, Lo.of M. of Inertia, I or I Centroid y b Retangle = b b I x 1 Triangle b y b I 6 Cirle d d y d I 6 Semiirle d 8 d I r y 18 I 6.8610 d Ellipse b y b I 6 Semi b Ellipse Parabola b y b x 8 y 5 b I 16 b I 7 8b I 175 Quadrant d 16 r y r x I d I 56.10 d Trapezoid a b y a b a b a ab b I 6 a b