Find the flow rate of water at 60 F in each pipe. The valve shown in completely closed, neglect minor losses.
|
|
- Nicholas Tucker
- 5 years ago
- Views:
Transcription
1 Kevin Lis Fluid Mechanics MET 330 Test #3 Page Number: 1 1. Purpose #1 Find the flow rate of water at 60 F in each pipe. The valve shown in completely closed, neglect minor losses. 2. Drawing & Diagrams 3. Sources Applied Fluid Mechanics 7 th Edition BlackBoard 4. Design considerations Valve is closed so now water can flow through it, neglect the minor losses. 5. Data and Variables L= 50 Le=0 E= v=1.21*10^-5 D= ft g=32.2 ft/s
2 Kevin Lis Fluid Mechanics MET 330 Test #3 Page Number: 2 6. Procedure First assume the Q in what direction it is going in what pipe. Then Calculate V=Q/A and Nr=V*D/v. Calculate F by taking (0.25)/(LOG(1/(3.7*D/E)+5.74/Nr^0.9)^2). We find k=8*l*f / (pi^2*g*(d)^5). Then h is just Q*k^2 and 2kQ for literally 2kQ. We add the sum up from h and 2kQ from the 5 pipes and divided h / 2kQ to find the Delta Q. Once we have Delta Q we subtract that from the Q assumed and that will give us the Q(n). To find the percentage change we do Q / Delta Q. 7. Calculations & Summary g ft/s 32.2 D ft A ft^ E v Pipe # L Le Q V Nr F k h 2kQ Delta Q Q(n) % Change Materials -Water -Schedule 40, 2 1/2 inch pipe 9. Analysis Use the fluid mechanics software that makes this process a whole lot easier in the future.
3 Kevin Lis Fluid Mechanics MET 330 Test #3 Page Number: 3 1. Purpose #2 Determine the depth when the flow rate of the channel show is 34.7 ft^3/s and has a manning value of 0.04, if the average slope is Drawing & Diagrams 3. Sources Applied Fluid Mechanics 7 th Edition BlackBoard 4. Design considerations The design seems to be safe with the average slope the length of the channel. If outside and available for public to access, would suggest adding a plate or a grid line pattern to protect. 5. Data and Variables n= 0.04 s= Q=34.7 ft^3/s
4 Kevin Lis Fluid Mechanics MET 330 Test #3 Page Number: 4 6. Procedure Calculate the depth by using equation AR^2/3=nQ/1.49S^1/2 then find height (y) in the Area, WP, and R and calculate by iterating the LHS=RHS in excel. 7. Calculations
5 Kevin Lis Fluid Mechanics MET 330 Test #3 Page Number: 5 8. Summary n Q S Constant RHS Y A WP R R^2/3 LHS Materials -Water -Channel 10. Analysis The calculations show that the height should be 3 feet. The design overall as a channel looks right but if you wanted to increase the slope this would make the height less and take up less space.
6 Kevin Lis Fluid Mechanics MET 330 Test #3 Page Number: 6 1. Purpose #4 At the end of a steel pipe there is a valve. When the valve closes all of the sudden there is a pressure increment of 2.81 MPa in the pipe. Find the water velocity for such a pressure increment. 2. Drawing & Diagrams 3. Sources Applied Fluid Mechanics 7 th Edition BlackBoard 4. Design considerations Due to closing the pipe suddenly, this will cause water hammer. Instead slowly close the pipe over time so no water hammering occurs and prevents damage to the pipe or injury from explosion.
7 Kevin Lis Fluid Mechanics MET 330 Test #3 Page Number: 7 5. Data and Variables E=2*10^7 N/cm^2 = 2*10^11 N/m^2 E(o)=2.03*10^5 N/cm^2 = 2.03*10^9 N/m^2 Internal Diameter of pipe= 600 mm = 0.6m Thickness of Pipe= 100 mm = 0.01m Density of water = 1000 kg/m^3 Pressure=2.81 MPa = 2,810,000 Pa 6. Procedure Apply the calculation of P= ρ*v*c. In this case we can solve for C by calculate the square root of E/ ρ divided by the square root of (1+ E(o)*Diameter / E * thickness). After obtaining C we plug it in to the equation and solve for the velocity. Pressure in Pascal's is divided by from C and 1000 from ρ. This gives us meters per second for the velocity.
8 Kevin Lis Fluid Mechanics MET 330 Test #3 Page Number: 8 7. Calculations
9 Kevin Lis Fluid Mechanics MET 330 Test #3 Page Number: 9 8. Summary P/c/ρ= v = 2.5 m/s 2,810,000/ /1000= Materials -Water -Steel Pipe -Valve 10. Analysis The design could either be changed to have a robot or computer controlled valve closing the valve automatically and slow enough to prevent damage. So no accidents can occur due to humans not knowing about water hammer can cause an explosion if closed fast.
10 Kevin Lis Fluid Mechanics MET 330 Test #3 Page Number: Purpose #5 A free steam of water at 180 F is being deflected by a stationary vane (pictured below) through a 130 angel. The cross-sectional area of the stream is constant at 2.95 in^2 throughout the system. When the entering stream has a velocity of 22 ft/sec the horizontal force exerted on the water by the vane is 30.6 lb. Find the stream velocity if the horizontal force is reduced by half? and what is the vertical force? 2. Drawing & Diagrams 3. Sources Applied Fluid Mechanics 7 th Edition BlackBoard
11 Kevin Lis Fluid Mechanics MET 330 Test #3 Page Number: Design considerations Design looks to be safe and accurate to what the diagram provides. 5. Data and Variables A= 2.95 in^2/144 = ft^2 F(Xo)= 30.6 F(Xnew)= 30.6 / 2 = 15.3 lb ρ = slugs/ft^3 6. Procedure First draw diagram of how the vane and forces are working, then set the Y axis going up and the X axis going to the left. I set the equation so Q is split between V and A. F(x) / ρ * A is the LHS and the RHS is V*(V(x(2))-V(x(1))). Convert Area into ft^2. Find LHS by plugging in. Set V(x(2))= V * cos (50) and V(x(1))= -V * cos(0). Assume a V value in excel and iterate until LHS=RHS. Calculate Q with new V= Set V(y(2))= 15.55*sin(130) and V(y(1)=15.55*sin(0). Then calculate F(y)=1.883*0.3185*11.91= 7.15 lb
12 Kevin Lis Fluid Mechanics MET 330 Test #3 Page Number: Calculations
13 Kevin Lis Fluid Mechanics MET 330 Test #3 Page Number: Summary F(Xo) F(Xnew) Q V A p V(x1) V(x2) V(y1) V(y2) LHS RHS Fy (lb) Materials 180 F -Vane 10. Analysis The design could be changed in making the angle more or less, but would consider not making it turn into a full U-turn shape. I would recommend putting a 90 degree vane and then another 90 degree vane inverted, so it can completely make a full turn. Depending on the change in angle you will have to change the velocity in order to keep it flowing correctly.
14 Kevin Lis Fluid Mechanics MET 330 Test #3 Page Number: Purpose #6 The airfoil with the performance characteristics (shown in the figure below) has a chord length of 1.4 m and a span of 6.8 m. The airfoil is part of an airplane moving at a speed of 200 km/hr in the standard atmosphere at 200 m. It was determined that the lift and drag forces are 15.9 kn and 883 N when the angle of attack is 10 degrees. What should the angle of attack if the airplane weighted 25% more? 2. Drawing & Diagrams 3. Sources Applied Fluid Mechanics 7 th Edition BlackBoard
15 Kevin Lis Fluid Mechanics MET 330 Test #3 Page Number: Design considerations The area is the Span of the blade times the Chord depth, as long as this is kept to a certain minimum on the plane it should not affect the cost. 5. Data and Variables b= 6.8 m c= 1.4 m A= 9.52 m^2 V= 200km/hr = 55.5 m/s F(l)= 15.9 kn Appendix E; Table E.3: 200 m ρ=1.202 kg/m^3 6. Procedure Calculate the area first and convert the velocity of km/hr to m/s and plug into equation solving for C(l) using F(l)=C(l)*( ρ*v^2 / 2) *A. Then convert the F(l) kn to N and multiply by 1.25% that will give you the new weight added. Divided that new total by the LHS without C(l) and that will give you the answer. Compare that C(l) calculated into the graph given and intersect it where the angle meets.
16 Kevin Lis Fluid Mechanics MET 330 Test #3 Page Number: Calculations
17 Kevin Lis Fluid Mechanics MET 330 Test #3 Page Number: Summary C(l)= and estimating that located on the Y axis for the graph given, I located the angle of attack to be 12.5 degrees. 9. Materials 200 meters -Plane Material & airfoil 10. Analysis Seemed like a NASA problem, if the area of the Airfoil is increased then the C(l) is dropped lower which makes the angle drop as well, so it is recommended that you either keep the Area constant and add weight or change the area of the airfoil and keep the weight constant in area to have a change in the angle of attack.
AEROSPACE ENGINEERING DEPARTMENT. Second Year - Second Term ( ) Fluid Mechanics & Gas Dynamics
AEROSPACE ENGINEERING DEPARTMENT Second Year - Second Term (2008-2009) Fluid Mechanics & Gas Dynamics Similitude,Dimensional Analysis &Modeling (1) [7.2R*] Some common variables in fluid mechanics include:
More informationS.E. (Mech.) (First Sem.) EXAMINATION, (Common to Mech/Sandwich) FLUID MECHANICS (2008 PATTERN) Time : Three Hours Maximum Marks : 100
Total No. of Questions 12] [Total No. of Printed Pages 8 Seat No. [4262]-113 S.E. (Mech.) (First Sem.) EXAMINATION, 2012 (Common to Mech/Sandwich) FLUID MECHANICS (2008 PATTERN) Time : Three Hours Maximum
More informationPh.D. Qualifying Exam in Fluid Mechanics
Student ID Department of Mechanical Engineering Michigan State University East Lansing, Michigan Ph.D. Qualifying Exam in Fluid Mechanics Closed book and Notes, Some basic equations are provided on an
More information2 Navier-Stokes Equations
1 Integral analysis 1. Water enters a pipe bend horizontally with a uniform velocity, u 1 = 5 m/s. The pipe is bended at 90 so that the water leaves it vertically downwards. The input diameter d 1 = 0.1
More informationConsider a control volume in the form of a straight section of a streamtube ABCD.
6 MOMENTUM EQUATION 6.1 Momentum and Fluid Flow In mechanics, the momentum of a particle or object is defined as the product of its mass m and its velocity v: Momentum = mv The particles of a fluid stream
More informationTutorial 10. Boundary layer theory
Tutorial 10 Boundary layer theory 1. If the velocity distribution law in a laminar boundary layer over a flat plate is assumes to be of the form, determine the velocity distribution law. At y = 0, u= 0
More informationDrag Analysis of a Supermarine. Spitfire Mk V at Cruise Conditions
Introduction to Flight Aircraft Drag Project April 2016 2016 Drag Analysis of a Supermarine Spitfire Mk V at Cruise Conditions Nicholas Conde nicholasconde@gmail.com U66182304 Introduction to Flight Nicholas
More informationCIVE HYDRAULIC ENGINEERING PART I Pierre Julien Colorado State University
CIVE 401 - HYDRAULIC ENGINEERING PART I Pierre Julien Colorado State University Problems with and are considered moderate and those with are the longest and most difficult. In 2018 solve the problems with
More informationGiven the water behaves as shown above, which direction will the cylinder rotate?
water stream fixed but free to rotate Given the water behaves as shown above, which direction will the cylinder rotate? ) Clockwise 2) Counter-clockwise 3) Not enough information F y U 0 U F x V=0 V=0
More informationSPC Aerodynamics Course Assignment Due Date Monday 28 May 2018 at 11:30
SPC 307 - Aerodynamics Course Assignment Due Date Monday 28 May 2018 at 11:30 1. The maximum velocity at which an aircraft can cruise occurs when the thrust available with the engines operating with the
More informationNicholas J. Giordano. Chapter 10 Fluids
Nicholas J. Giordano www.cengage.com/physics/giordano Chapter 10 Fluids Fluids A fluid may be either a liquid or a gas Some characteristics of a fluid Flows from one place to another Shape varies according
More informationPROPERTIES OF FLUIDS
Unit - I Chapter - PROPERTIES OF FLUIDS Solutions of Examples for Practice Example.9 : Given data : u = y y, = 8 Poise = 0.8 Pa-s To find : Shear stress. Step - : Calculate the shear stress at various
More informationFE Fluids Review March 23, 2012 Steve Burian (Civil & Environmental Engineering)
Topic: Fluid Properties 1. If 6 m 3 of oil weighs 47 kn, calculate its specific weight, density, and specific gravity. 2. 10.0 L of an incompressible liquid exert a force of 20 N at the earth s surface.
More informationCOURSE NUMBER: ME 321 Fluid Mechanics I 3 credit hour. Basic Equations in fluid Dynamics
COURSE NUMBER: ME 321 Fluid Mechanics I 3 credit hour Basic Equations in fluid Dynamics Course teacher Dr. M. Mahbubur Razzaque Professor Department of Mechanical Engineering BUET 1 Description of Fluid
More informationCHAPTER 3 ANALYSIS OF NACA 4 SERIES AIRFOILS
54 CHAPTER 3 ANALYSIS OF NACA 4 SERIES AIRFOILS The baseline characteristics and analysis of NACA 4 series airfoils are presented in this chapter in detail. The correlations for coefficient of lift and
More information9. Pumps (compressors & turbines) Partly based on Chapter 10 of the De Nevers textbook.
Lecture Notes CHE 31 Fluid Mechanics (Fall 010) 9. Pumps (compressors & turbines) Partly based on Chapter 10 of the De Nevers textbook. Basics (pressure head, efficiency, working point, stability) Pumps
More information10.52 Mechanics of Fluids Spring 2006 Problem Set 3
10.52 Mechanics of Fluids Spring 2006 Problem Set 3 Problem 1 Mass transfer studies involving the transport of a solute from a gas to a liquid often involve the use of a laminar jet of liquid. The situation
More informationWritten in August 2017 during my holiday in Bulgaria, Sunny Coast
Electric ucted Fan Theory This paper describes a simple theory of a ducted fan. It is assumed that the reader knows what it is an electric ducted fan (EF), how it works, and what it is good for. When I
More informationStability and Control Some Characteristics of Lifting Surfaces, and Pitch-Moments
Stability and Control Some Characteristics of Lifting Surfaces, and Pitch-Moments The lifting surfaces of a vehicle generally include the wings, the horizontal and vertical tail, and other surfaces such
More informationPart A: 1 pts each, 10 pts total, no partial credit.
Part A: 1 pts each, 10 pts total, no partial credit. 1) (Correct: 1 pt/ Wrong: -3 pts). The sum of static, dynamic, and hydrostatic pressures is constant when flow is steady, irrotational, incompressible,
More informationNon Newtonian Fluid Dynamics
PDHonline Course M417 (3 PDH) Non Newtonian Fluid Dynamics Instructor: Paul G. Conley, PE 2012 PDH Online PDH Center 5272 Meadow Estates Drive Fairfax, VA 22030-6658 Phone & Fax: 703-988-0088 www.pdhonline.org
More informationexcept assume the parachute has diameter of 3.5 meters and calculate how long it takes to stop. (Must solve differential equation)
Homework 5 Due date: Thursday, Mar. 3 hapter 7 Problems 1. 7.88. 7.9 except assume the parachute has diameter of 3.5 meters and calculate how long it takes to stop. (Must solve differential equation) 3.
More informationν δ - 1 -
ν δ - 1 - δ ν ν δ ν ν - 2 - ρ δ ρ θ θ θ δ τ ρ θ δ δ θ δ δ δ δ τ μ δ μ δ ν δ δ δ - 3 - τ ρ δ ρ δ ρ δ δ δ δ δ δ δ δ δ δ δ - 4 - ρ μ ρ μ ρ ρ μ μ ρ - 5 - ρ τ μ τ μ ρ δ δ δ - 6 - τ ρ μ τ ρ μ ρ δ θ θ δ θ - 7
More informationThe online of midterm-tests of Fluid Mechanics 1
The online of midterm-tests of Fluid Mechanics 1 1) The information on a can of pop indicates that the can contains 460 ml. The mass of a full can of pop is 3.75 lbm while an empty can weights 80.5 lbf.
More informationEquilibrium in Three Dimensions
C h a p t e r 7 Equilibrium in Three Dimensions In this chapter, you will learn the following to World Class standards: Forces in Three Different Axis Wind Load on the Antennae Pole Practice Problem -
More information2.4 Rates of Change and Tangent Lines Pages 87-93
2.4 Rates of Change and Tangent Lines Pages 87-93 Average rate of change the amount of change divided by the time it takes. EXAMPLE 1 Finding Average Rate of Change Page 87 Find the average rate of change
More informationDefinitions. Temperature: Property of the atmosphere (τ). Function of altitude. Pressure: Property of the atmosphere (p). Function of altitude.
Definitions Chapter 3 Standard atmosphere: A model of the atmosphere based on the aerostatic equation, the perfect gas law, an assumed temperature distribution, and standard sea level conditions. Temperature:
More information6-1 Slope. Objectives 1. find the slope of a line 2. use rate of change to solve problems
6-1 Slope Objectives 1. find the slope of a line 2. use rate of change to solve problems What is the meaning of this sign? 1. Icy Road Ahead 2. Steep Road Ahead 3. Curvy Road Ahead 4. Trucks Entering Highway
More informationM E 320 Professor John M. Cimbala Lecture 24
M E 30 Professor John M. Cimbala Lecture 4 Today, we will: Discuss pump performance curves Discuss how to match a pump and a piping system, and do some example problems. Pump Performance a. Pump performance
More informationOpen Channel Flow I - The Manning Equation and Uniform Flow COURSE CONTENT
Open Channel Flow I - The Manning Equation and Uniform Flow Harlan H. Bengtson, PhD, P.E. COURSE CONTENT 1. Introduction Flow of a liquid may take place either as open channel flow or pressure flow. Pressure
More informationOnly if handing in. Name: Student No.: Page 2 of 7
UNIVERSITY OF TORONTO FACULTY OF APPLIED SCIENCE AND ENGINEERING FINAL EXAMINATION, DECEMBER 10, 2014 2:00 PM 2.5 HOURS CHE 211F FLUID MECHANICS EXAMINER: PROFESSOR D.G. ALLEN ANSWER ALL SEVEN (7) QUESTIONS
More informationAerodynamics SYST 460/560. George Mason University Fall 2008 CENTER FOR AIR TRANSPORTATION SYSTEMS RESEARCH. Copyright Lance Sherry (2008)
Aerodynamics SYST 460/560 George Mason University Fall 2008 1 CENTER FOR AIR TRANSPORTATION SYSTEMS RESEARCH Copyright Lance Sherry (2008) Ambient & Static Pressure Ambient Pressure Static Pressure 2 Ambient
More informationUNIT I FLUID PROPERTIES AND STATICS
SIDDHARTH GROUP OF INSTITUTIONS :: PUTTUR Siddharth Nagar, Narayanavanam Road 517583 QUESTION BANK (DESCRIPTIVE) Subject with Code : Fluid Mechanics (16CE106) Year & Sem: II-B.Tech & I-Sem Course & Branch:
More informationCE 6303 MECHANICS OF FLUIDS L T P C QUESTION BANK 3 0 0 3 UNIT I FLUID PROPERTIES AND FLUID STATICS PART - A 1. Define fluid and fluid mechanics. 2. Define real and ideal fluids. 3. Define mass density
More informationEXPERIMENT No.1 FLOW MEASUREMENT BY ORIFICEMETER
EXPERIMENT No.1 FLOW MEASUREMENT BY ORIFICEMETER 1.1 AIM: To determine the co-efficient of discharge of the orifice meter 1.2 EQUIPMENTS REQUIRED: Orifice meter test rig, Stopwatch 1.3 PREPARATION 1.3.1
More informationPhysics - Fluids. Read Page 174 (Density) TQ1. A fluid is what type of matter? TQ2. What is fluid mechanics? TQ3. What is the equation for density?
Homework Procedure: Read pages specified in Honors Physics Essentials by Dan Fullerton. Questions labeled TQ will be questions about the text you read. These TQ s can be answered in one word, one phrase,
More informationThe E80 Wind Tunnel Experiment the experience will blow you away. by Professor Duron Spring 2012
The E80 Wind Tunnel Experiment the experience will blow you away by Professor Duron Spring 2012 Objectives To familiarize the student with the basic operation and instrumentation of the HMC wind tunnel
More informationCHAPTER 3 BASIC EQUATIONS IN FLUID MECHANICS NOOR ALIZA AHMAD
CHAPTER 3 BASIC EQUATIONS IN FLUID MECHANICS 1 INTRODUCTION Flow often referred as an ideal fluid. We presume that such a fluid has no viscosity. However, this is an idealized situation that does not exist.
More informationCPO Science Foundations of Physics. Unit 8, Chapter 27
CPO Science Foundations of Physics Unit 8, Chapter 27 Unit 8: Matter and Energy Chapter 27 The Physical Properties of Matter 27.1 Properties of Solids 27.2 Properties of Liquids and Fluids 27.3 Properties
More informationUniversität Duisburg-Essen Fakultät für Ingenieurwissenschaften WS 2012 Maschinenbau, IVG, Thermodynamik Dr. M. A. Siddiqi
1 Universität Duisburg-Essen 3. Semester Fakultät für Ingenieurwissenschaften WS 2012 Maschinenbau, IVG, Thermodynamik Dr. M. A. Siddiqi THERMODYNAMICS LAB (ISE) Pressure Measurement 2 2 Pressure Measurement
More informationDepartment of Energy Fundamentals Handbook. THERMODYNAMICS, HEAT TRANSFER, AND FLUID FLOW, Module 3 Fluid Flow
Department of Energy Fundamentals Handbook THERMODYNAMICS, HEAT TRANSFER, AND FLUID FLOW, Module 3 REFERENCES REFERENCES Streeter, Victor L., Fluid Mechanics, 5th Edition, McGraw-Hill, New York, ISBN 07-062191-9.
More informationFlow Behavior Lab BSEN Major and Minor Losses. Samuel Dunbar
Flow Behavior Lab BSEN 3310 Major and Minor Losses Samuel Dunbar Abstract: The major losses, friction loss, and minor losses, head loss, in pipes were determined through the use of two different devices.
More informationACE Engineering College
ACE Engineering College Ankushapur (V), Ghatkesar (M), R.R.Dist 501 301. * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * MECHANICS OF FLUIDS & HYDRAULIC
More informationCHAPTER 4 OPTIMIZATION OF COEFFICIENT OF LIFT, DRAG AND POWER - AN ITERATIVE APPROACH
82 CHAPTER 4 OPTIMIZATION OF COEFFICIENT OF LIFT, DRAG AND POWER - AN ITERATIVE APPROACH The coefficient of lift, drag and power for wind turbine rotor is optimized using an iterative approach. The coefficient
More informationAerodynamics. Basic Aerodynamics. Continuity equation (mass conserved) Some thermodynamics. Energy equation (energy conserved)
Flow with no friction (inviscid) Aerodynamics Basic Aerodynamics Continuity equation (mass conserved) Flow with friction (viscous) Momentum equation (F = ma) 1. Euler s equation 2. Bernoulli s equation
More informationQuiz 6 Practice Problems
Quiz 6 Practice Problems Practice problems are similar, both in difficulty and in scope, to the type of problems you will see on the quiz. Problems marked with a are for your entertainment and are not
More informationApplied Fluid Mechanics
Applied Fluid Mechanics 1. The Nature of Fluid and the Study of Fluid Mechanics 2. Viscosity of Fluid 3. Pressure Measurement 4. Forces Due to Static Fluid 5. Buoyancy and Stability 6. Flow of Fluid and
More informationFor the intersections: cos x = 0 or sin x = 1 2
Chapter 6 Set-up examples The purpose of this document is to demonstrate the work that will be required if you are asked to set-up integrals on an exam and/or quiz.. Areas () Set up, do not evaluate, any
More informationSports Performance Visualisation in Teaching Activities
Sports Performance Visualisation in Teaching Kristina Marasović Kristina.Marasovic@pmfst.hr Mile Dželalija Mile.Dzelalija@pmfst.hr Faculty of Natural Sciences, Mathematics and Education University of Split
More informationApplications of Integration to Physics and Engineering
Applications of Integration to Physics and Engineering MATH 211, Calculus II J Robert Buchanan Department of Mathematics Spring 2018 Mass and Weight mass: quantity of matter (units: kg or g (metric) or
More informationFluids. Fluids in Motion or Fluid Dynamics
Fluids Fluids in Motion or Fluid Dynamics Resources: Serway - Chapter 9: 9.7-9.8 Physics B Lesson 3: Fluid Flow Continuity Physics B Lesson 4: Bernoulli's Equation MIT - 8: Hydrostatics, Archimedes' Principle,
More information4 Mechanics of Fluids (I)
1. The x and y components of velocity for a two-dimensional flow are u = 3.0 ft/s and v = 9.0x ft/s where x is in feet. Determine the equation for the streamlines and graph representative streamlines in
More informationAP Calculus AB Chapter 4 Packet Implicit Differentiation. 4.5: Implicit Functions
4.5: Implicit Functions We can employ implicit differentiation when an equation that defines a function is so complicated that we cannot use an explicit rule to find the derivative. EXAMPLE 1: Find dy
More informationFE Exam Fluids Review October 23, Important Concepts
FE Exam Fluids Review October 3, 013 mportant Concepts Density, specific volume, specific weight, specific gravity (Water 1000 kg/m^3, Air 1. kg/m^3) Meaning & Symbols? Stress, Pressure, Viscosity; Meaning
More informationLesson 6 Review of fundamentals: Fluid flow
Lesson 6 Review of fundamentals: Fluid flow The specific objective of this lesson is to conduct a brief review of the fundamentals of fluid flow and present: A general equation for conservation of mass
More informationFinal Exam Review Sheet Solutions
Final Exam Review Sheet Solutions. Find the derivatives of the following functions: a) f x x 3 tan x 3. f ' x x 3 tan x 3 x 3 sec x 3 3 x. Product rule and chain rule used. b) g x x 6 5 x ln x. g ' x 6
More information2 Internal Fluid Flow
Internal Fluid Flow.1 Definitions Fluid Dynamics The study of fluids in motion. Static Pressure The pressure at a given point exerted by the static head of the fluid present directly above that point.
More informationPhysics 220: Classical Mechanics
Lecture /33 Phys 0 Physics 0: Classical Mechanics Lecture: MWF 8:40 am 9:40 am (Phys 4) Michael Meier mdmeier@purdue.edu Office: Phys Room 38 Help Room: Phys Room schedule on course webpage Office Hours:
More information4.1 & 4.2 Student Notes Using the First and Second Derivatives. for all x in D, where D is the domain of f. The number f()
4.1 & 4. Student Notes Using the First and Second Derivatives Definition A function f has an absolute maximum (or global maximum) at c if f ( c) f ( x) for all x in D, where D is the domain of f. The number
More informationAnnubar Primary Element Flow Calculations
Rosemount 485 Annubar Annubar Primary Element Flow Calculations ANNUBAR PRIMARY ELEMENT FLOW EQUATIONS The Annubar primary element flow equations are all derived from the hydraulic equations which are
More informationIntroduction to Atmospheric Flight. Dr. Guven Aerospace Engineer (P.hD)
Introduction to Atmospheric Flight Dr. Guven Aerospace Engineer (P.hD) What is Atmospheric Flight? There are many different ways in which Aerospace engineering is associated with atmospheric flight concepts.
More informationAE 2020: Low Speed Aerodynamics. I. Introductory Remarks Read chapter 1 of Fundamentals of Aerodynamics by John D. Anderson
AE 2020: Low Speed Aerodynamics I. Introductory Remarks Read chapter 1 of Fundamentals of Aerodynamics by John D. Anderson Text Book Anderson, Fundamentals of Aerodynamics, 4th Edition, McGraw-Hill, Inc.
More informationLearning Objectives. Lesson 6: Mathematical Models of Fluid Flow Components. ET 438a Automatic Control Systems Technology 8/27/2015
Lesson 6: Mathematical Models of Fluid Flow Components ET 438a Automatic Control Systems Technology lesson6et438a.pptx 1 Learning Objectives After this presentation you will be able to: Define the characteristics
More informationFlow in Open Channel Flow Conditions
Civil Engineering Hydraulics Flow The graduate with a Science degree asks, "Why does it work?" The graduate with an Engineering degree asks, "How does it work?" The graduate with an Accounting degree asks,
More informationIntroduction to Mechanical Engineering
Introduction to Mechanical Engineering Chapter 1 The Mechanical Engineering Profession Chapter Problem-Solving and Communication Skills Chapter 3 Forces in Structures and Machines Chapter 4 Materials and
More informationPiping Systems and Flow Analysis (Chapter 3)
Piping Systems and Flow Analysis (Chapter 3) 2 Learning Outcomes (Chapter 3) Losses in Piping Systems Major losses Minor losses Pipe Networks Pipes in series Pipes in parallel Manifolds and Distribution
More informationHigh Speed Aerodynamics. Copyright 2009 Narayanan Komerath
Welcome to High Speed Aerodynamics 1 Lift, drag and pitching moment? Linearized Potential Flow Transformations Compressible Boundary Layer WHAT IS HIGH SPEED AERODYNAMICS? Airfoil section? Thin airfoil
More informationHydraulics 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. # 08 Pipe Flow Lecture No. # 05 Water Hammer and Surge Tank Energy cannot be consumed
More informationFlow Measurement in Pipes and Ducts COURSE CONTENT
Flow Measurement in Pipes and Ducts Dr. Harlan H. Bengtson, P.E. COURSE CONTENT 1. Introduction This course is about measurement of the flow rate of a fluid flowing under pressure in a closed conduit.
More informationMasters in Mechanical Engineering Aerodynamics 1 st Semester 2015/16
Masters in Mechanical Engineering Aerodynamics st Semester 05/6 Exam st season, 8 January 06 Name : Time : 8:30 Number: Duration : 3 hours st Part : No textbooks/notes allowed nd Part : Textbooks allowed
More informationBallistic Atmospheric Entry (Part II)
Ballistic Atmospheric Entry (Part II) News updates Straight-line (no gravity) ballistic entry based on altitude, rather than density Planetary entries (at least a start) 1 2010 David L. Akin - All rights
More informationExperiment- To determine the coefficient of impact for vanes. Experiment To determine the coefficient of discharge of an orifice meter.
SUBJECT: FLUID MECHANICS VIVA QUESTIONS (M.E 4 th SEM) Experiment- To determine the coefficient of impact for vanes. Q1. Explain impulse momentum principal. Ans1. Momentum equation is based on Newton s
More information6.1 According to Handbook of Chemistry and Physics the composition of air is
6. Compressible flow 6.1 According to Handbook of Chemistry and Physics the composition of air is From this, compute the gas constant R for air. 6. The figure shows a, Pitot-static tube used for velocity
More informationControl Your Product Quality by Controlling Your Product's Conveying Velocity
Bulletin No. 201-201 PH: 717-546-3165 FAX: 717-546-1888 e-mail: mktinfo@younginds.com http:www.younginds.com Multi-Phase Dense Phase Pneumatic tic Conveyor ors Control Your Product Quality by Controlling
More informationIntroduction to Aerospace Engineering
Introduction to Aerospace Engineering 5. Aircraft Performance 5.1 Equilibrium Flight In order to discuss performance, stability, and control, we must first establish the concept of equilibrium flight.
More information3 Applications of Derivatives Instantaneous Rates of Change Optimization Related Rates... 13
Contents Limits Derivatives 3. Difference Quotients......................................... 3. Average Rate of Change...................................... 4.3 Derivative Rules...........................................
More informationFluid Mechanics. The atmosphere is a fluid!
Fluid Mechanics The atmosphere is a fluid! Some definitions A fluid is any substance which can flow Liquids, gases, and plasmas Fluid statics studies fluids in equilibrium Density, pressure, buoyancy Fluid
More informationME332 FLUID MECHANICS LABORATORY (PART I)
ME332 FLUID MECHANICS LABORATORY (PART I) Mihir Sen Department of Aerospace and Mechanical Engineering University of Notre Dame Notre Dame, IN 46556 Version: January 14, 2002 Contents Unit 1: Hydrostatics
More informationLesson 37 Transmission Of Air In Air Conditioning Ducts
Lesson 37 Transmission Of Air In Air Conditioning Ducts Version 1 ME, IIT Kharagpur 1 The specific objectives of this chapter are to: 1. Describe an Air Handling Unit (AHU) and its functions (Section 37.1).
More informationIntroduction to Aerospace Engineering
4. Basic Fluid (Aero) Dynamics Introduction to Aerospace Engineering Here, we will try and look at a few basic ideas from the complicated field of fluid dynamics. The general area includes studies of incompressible,
More informationfor what specific application did Henri Pitot develop the Pitot tube? what was the name of NACA s (now NASA) first research laboratory?
1. 5% short answers for what specific application did Henri Pitot develop the Pitot tube? what was the name of NACA s (now NASA) first research laboratory? in what country (per Anderson) was the first
More informationFlight Vehicle Terminology
Flight Vehicle Terminology 1.0 Axes Systems There are 3 axes systems which can be used in Aeronautics, Aerodynamics & Flight Mechanics: Ground Axes G(x 0, y 0, z 0 ) Body Axes G(x, y, z) Aerodynamic Axes
More informationDepartment of Energy Sciences, LTH
Department of Energy Sciences, LTH MMV11 Fluid Mechanics LABORATION 1 Flow Around Bodies OBJECTIVES (1) To understand how body shape and surface finish influence the flow-related forces () To understand
More information6.5 Work and Fluid Forces
6.5 Work and Fluid Forces Work Work=Force Distance Work Work=Force Distance Units Force Distance Work Newton meter Joule (J) pound foot foot-pound (ft lb) Work Work=Force Distance Units Force Distance
More informationPipe Flow. Lecture 17
Pipe Flow Lecture 7 Pipe Flow and the Energy Equation For pipe flow, the Bernoulli equation alone is not sufficient. Friction loss along the pipe, and momentum loss through diameter changes and corners
More informationAppendix. Using Your Calculator. Squares, Square Roots, Reciprocals, and Logs. Addition, Subtraction, Multiplication, and Division
370770_app.qxd 1/9/03 7:2 PM Page A1 mac114 Mac 114:2nd shift:4_rst: Using Your Calculator In this section we will review how to use your calculator to perform common mathematical operations. This discussion
More information13) = 4 36 = ) = 5-8 = -3 =3 15) = = -58 = 58 16) = 81-9 = 72 = 72
Practice Practice Practice 3 ) (-3) + (-6) = -9 ) () + (-5) = -3 3) (-7) + (-) = -8 4) (-3) - (-6) = (-3) + 6 = + 3 5) (+) - (+5) = -3 6) (-7) - (-4) = (-7) + 4 = -3 7) (5)(-4) = - 8) (-3)(-6) = +8 9)
More informationNumerical Study on Performance of Curved Wind Turbine Blade for Loads Reduction
Numerical Study on Performance of Curved Wind Turbine Blade for Loads Reduction T. Maggio F. Grasso D.P. Coiro 13th International Conference Wind Engineering (ICWE13), 10-15 July 011, Amsterdam, the Netherlands.
More informationFluid Flow Analysis Penn State Chemical Engineering
Fluid Flow Analysis Penn State Chemical Engineering Revised Spring 2015 Table of Contents LEARNING OBJECTIVES... 1 EXPERIMENTAL OBJECTIVES AND OVERVIEW... 1 PRE-LAB STUDY... 2 EXPERIMENTS IN THE LAB...
More informationPhysics 107 HOMEWORK ASSIGNMENT #9
Physics 07 HOMEORK ASSIGNMENT #9 Cutnell & Johnson, 7 th edition Chapter : Problems 6, 8, 33, 40, 44 *6 A 58-kg skier is going down a slope oriented 35 above the horizontal. The area of each ski in contact
More informationMechanical Engineering for Renewable Energy Systems. Dr. Digby Symons. Wind Turbine Blade Design
ENGINEERING TRIPOS PART IB PAPER 8 ELECTIVE () Mechanical Engineering for Renewable Energy Systems Dr. Digby Symons Wind Turbine Blade Design Student Handout CONTENTS 1 Introduction... 3 Wind Turbine Blade
More informationActive Control of Separated Cascade Flow
Chapter 5 Active Control of Separated Cascade Flow In this chapter, the possibility of active control using a synthetic jet applied to an unconventional axial stator-rotor arrangement is investigated.
More informationPhysics 3 Summer 1990 Lab 7 - Hydrodynamics
Physics 3 Summer 1990 Lab 7 - Hydrodynamics Theory Consider an ideal liquid, one which is incompressible and which has no internal friction, flowing through pipe of varying cross section as shown in figure
More informationFundamentals of Algebra, Geometry, and Trigonometry. (Self-Study Course)
Fundamentals of Algebra, Geometry, and Trigonometry (Self-Study Course) This training is offered eclusively through the Pennsylvania Department of Transportation, Business Leadership Office, Technical
More informationLifting Airfoils in Incompressible Irrotational Flow. AA210b Lecture 3 January 13, AA210b - Fundamentals of Compressible Flow II 1
Lifting Airfoils in Incompressible Irrotational Flow AA21b Lecture 3 January 13, 28 AA21b - Fundamentals of Compressible Flow II 1 Governing Equations For an incompressible fluid, the continuity equation
More informationChapter 1 INTRODUCTION
Chapter 1 INTRODUCTION 1-1 The Fluid. 1-2 Dimensions. 1-3 Units. 1-4 Fluid Properties. 1 1-1 The Fluid: It is the substance that deforms continuously when subjected to a shear stress. Matter Solid Fluid
More informationEmpirical Co - Relations approach for solving problems of convection 10:06:43
Empirical Co - Relations approach for solving problems of convection 10:06:43 10:06:44 Empirical Corelations for Free Convection Use T f or T b for getting various properties like Re = VL c / ν β = thermal
More informationME 316: Thermofluids Laboratory
ME 316 Thermofluid Laboratory 6.1 KING FAHD UNIVERSITY OF PETROLEUM & MINERALS ME 316: Thermofluids Laboratory PELTON IMPULSE TURBINE 1) OBJECTIVES a) To introduce the operational principle of an impulse
More informationPipe Flow/Friction Factor Calculations using Excel Spreadsheets
Pipe Flow/Friction Factor Calculations using Excel Spreadsheets Harlan H. Bengtson, PE, PhD Emeritus Professor of Civil Engineering Southern Illinois University Edwardsville Table of Contents Introduction
More informationA SIMPLIFIED ANALYSIS OF NONLINEAR LONGITUDINAL DYNAMICS AND CONCEPTUAL CONTROL SYSTEM DESIGN
A SIMPLIFIED ANALYSIS OF NONLINEAR LONGITUDINAL DYNAMICS AND CONCEPTUAL CONTROL SYSTEM DESIGN ROBBIE BUNGE 1. Introduction The longitudinal dynamics of fixed-wing aircraft are a case in which classical
More information