Lecture 5. Labs this week:

Size: px
Start display at page:

Download "Lecture 5. Labs this week:"

Transcription

1 Labs this week: Lab 10: Bleed-off Circuit Lecture 5 Lab 11/12: Asynchronous/Synchronous and Parallel/Tandem Operations Systems Review Homework (due 10/11) Participation is research lab Hydraulic Hybrid Vehicles Next week: Guest lecturer Mike Olson, Eaton Hydraulics 141 Review: Sequencing and Circuit analysis Fluid Bulk modulus Fluid Inertance Component modeling Pressure reducing valve Pressure compensated flow control valve 1

2 Lab Works: Prelabs TA explanation Matlab/Simulink Useful for learning Not works: Not enough connectors TA needs to smile Too many reports Clearer lab handouts Better labels Emphasize main points Requirements for lab reports What Work / What Don t 142 Lecture Works: Explanations of labs before hand In-class examples Slides / handouts available Theory useful Participation Not works: Answers to questions not available Behind with labs sometimes No-break Disconnect from lab More animations More examples 2

3 143 Sequencing Circuits Sequence valve cracking pressure settings to enable proper sequencing Too high never cracks Too low simultaneous motion instead of sequence P1 F Crack at P_R Hint: Sketch the time course of pressure P1. What determines the P1 when it cylinder 1 is moving and when it bottoms out 3

4 Example: 3MW Wind Turbine, 35MPa 144 4

5 Friction Factor Moody Diagram 145 5

6 146 Example L clearance = 0.1mm Cylindrical Spool P 90 deg elbow diameter = 0.5cm Sleeve Q = 30 LPM?1: Assuming small leakage, determine pressure P.?2: How long does L have to be for leakage to be less than 0.01% of the flow? 6

7 Fluid Compressibility: Bulk Modulus 147 Hydraulic fluid is slightly compressible: fluid volume decreases from V by dv on application of pressure dp - dv V 1 = dp is the bulk modulus - varies a lot with temperature and amount of aeration For = 200kPsi, 5000psi pressure compresses fluid by 2.5% Increases with pressure Decreased significantly by entrained air content 7

8 148 Bulk modulus: cont d For precise application, can be important, especially for long stroke, narrow, cylinders dl = pressure*l/ = force*l/(area* ) D=0.5in bore, 6 in stroke 0.15in/1000 lb-f D=1 in bore, L=1.5in stroke (same volume) 0.01in/1000 lb-f 16 times smaller Note that compressibility equation looks like equation for a spring 8

9 Energy in Compressed Fluid (Li and Wang, 2011) 149 9

10 Accounting for Bulk Modulus 150 Compressibility increases spring like action Possibility of having resonance M V = Q/A Spring, K M Q A Questions: How to pick K? Compressible cylinder Ideal cylinder (velocity generator) + Spring 10

11 Modeling compressibility in cylinders 151 Consider when the cylinder ports are blocked Suppose the load F is applied on the piston, how much does the piston move? Note: the chamber should include all the volumes between the piston and the valve (i.e. include hoses) Case 1: Double ended actuator Case 2: Single ended actuator F Does the spring constant change with position of the piston? 11

12 Equivalent Spring Constant 152 Data F Differentiating: K eq Finite if dead volumes (hoses) included Worst case x 12

13 Fluid Inertance (inertia) 153 F = m * a for the accelerating fluid (transients) Normally, the pressure needed to accelerate the fluid is neglected. When is this important? Momentum calculation for a hose: Length = L, Area = A P1 P2 A P = d dt d dt LAv = LQ P = L A dq dt inertance Important for long, narrow pipes water hammer effect! 13

14 How to make a big mass out of little mass? 154 v v Total weight of device = M Kinetic energy = (100 M) v 2 /2 What is in the pink box? 14

15 155 Power Computations A hydraulic device is generally an n-port system each port interacts with its environment - hydraulic, mechanical, (electric) Hydraulic power: energy flux through each port Power_in = F*vel_in = P*A*vel_in = P * Q hoses load P 1, Q 1 P 2, Q 2 E-power For a hose filled with incompressible fluid, Q_2 = -Q_1 Net hydraulic power in = (P 1 - P 2 )*Q How about a single ended or a double ended actuator, or a hydraulic motor? 15

16 156 Power Computation - cont d Hydraulic actuator / motor has 2 hydraulic port and 1 mechanical (load) port Net hydraulic power input = Net mechanical power input = Mechanical power variables: Force and velocity Torque and angular velocity For passive components, net power input not greater than 0. Calculate hydraulic power for hydraulic motor Relationship between hydraulic power and mechanical power? 16

17 157 Computer circuit analysis 0 Pump flow 0 Pressure Flow rate Flow Flow1 Pressure Pump turns Constant Slider Gain Needle2 0 Pressure Pressure 0 Flow Flow 2 turns Needle1 Slider Gain2 Constant1 17

18 Component Modeling - Pressure Reducing Valve 158 How do we write equations for this valve? Spool Force balance / Newton s law Spring Preload / Compression Orifice 18

19 Modeling 159 Function: Regulate pressure at B Operation: If P_B is too large (small), spool moves up (down) to reduce (increase) orifice size P B A B - ( F spring (x)- F seat ) - P D A D = M x A D F spr i n g A(x) B Preload x Possible Spring and area functions x 19

Lecture 5. Labs this week: Please review ME3281 Systems materials! Viscosity and pressure drop analysis Fluid Bulk modulus Fluid Inertance

Lecture 5. Labs this week: Please review ME3281 Systems materials! Viscosity and pressure drop analysis Fluid Bulk modulus Fluid Inertance Labs this week: Lab 10: Sequencing circuit Lecture 5 Lab 11/12: Asynchronous/Synchronous and Parallel/Tandem Operations Please review ME3281 Systems materials! 132 Viscosity and pressure drop analysis

More information

Lecture 4. Lab this week: Cartridge valves Flow divider Properties of Hydraulic Fluids. Lab 8 Sequencing circuit Lab 9 Flow divider

Lecture 4. Lab this week: Cartridge valves Flow divider Properties of Hydraulic Fluids. Lab 8 Sequencing circuit Lab 9 Flow divider 91 Lecture 4 Lab this week: Lab 8 Sequencing circuit Lab 9 Flow divider Cartridge valves Flow divider Properties of Hydraulic Fluids Viscosity friction and leakage Bulk modulus Inertance Cartridge Valves

More information

Hydraulic (Fluid) Systems

Hydraulic (Fluid) Systems Hydraulic (Fluid) Systems Basic Modeling Elements Resistance apacitance Inertance Pressure and Flow Sources Interconnection Relationships ompatibility Law ontinuity Law Derive Input/Output Models ME375

More information

ME 4232: FLUID POWER CONTROLS LAB. Class #5 Valve Modeling

ME 4232: FLUID POWER CONTROLS LAB. Class #5 Valve Modeling ME 4232: FLUID POWER CONTROLS LAB Class #5 Valve Modeling Notes No Office Hours Today Upcoming Labs: Lab 9: Flow Divider Lab 10: Sequencing Circuits 2 Agenda Wrap-up: Leakage Calculations Fluid Compressibility

More information

LECTURE 8. Hydraulic machines and systems II 2002 MIT PSDAM LAB

LECTURE 8. Hydraulic machines and systems II 2002 MIT PSDAM LAB LECTURE 8 Hydraulic machines and systems II Basic hydraulic machines & components Graphical Nomenclature Arrows show direction of flow Control Volume Pipe or hose with fluid flow Pipe or hose without fluid

More information

Chapter Four fluid flow mass, energy, Bernoulli and momentum

Chapter Four fluid flow mass, energy, Bernoulli and momentum 4-1Conservation of Mass Principle Consider a control volume of arbitrary shape, as shown in Fig (4-1). Figure (4-1): the differential control volume and differential control volume (Total mass entering

More information

HYDRAULIC CONTROL SYSTEMS

HYDRAULIC CONTROL SYSTEMS HYDRAULIC CONTROL SYSTEMS Noah D. Manring Mechanical and Aerospace Engineering Department University of Missouri-Columbia WILEY John Wiley & Sons, Inc. vii Preface Introduction xiii XV FUNDAMENTALS 1 Fluid

More information

Lecture Note 8-1 Hydraulic Systems. System Analysis Spring

Lecture Note 8-1 Hydraulic Systems. System Analysis Spring Lecture Note 8-1 Hydraulic Systems 1 Vehicle Model - Brake Model Brake Model Font Wheel Brake Pedal Vacuum Booster Master Cylinder Proportionnig Valve Vacuum Booster Rear Wheel Master Cylinder Proportioning

More information

SCHOOL OF COMPUTING, ENGINEERING AND MATHEMATICS SEMESTER 1 EXAMINATIONS 2012/2013 XE121. ENGINEERING CONCEPTS (Test)

SCHOOL OF COMPUTING, ENGINEERING AND MATHEMATICS SEMESTER 1 EXAMINATIONS 2012/2013 XE121. ENGINEERING CONCEPTS (Test) s SCHOOL OF COMPUTING, ENGINEERING AND MATHEMATICS SEMESTER EXAMINATIONS 202/203 XE2 ENGINEERING CONCEPTS (Test) Time allowed: TWO hours Answer: Attempt FOUR questions only, a maximum of TWO questions

More information

CHAPTER 3 QUARTER AIRCRAFT MODELING

CHAPTER 3 QUARTER AIRCRAFT MODELING 30 CHAPTER 3 QUARTER AIRCRAFT MODELING 3.1 GENERAL In this chapter, the quarter aircraft model is developed and the dynamic equations are derived. The quarter aircraft model is two degrees of freedom model

More information

Lecture Fluid system elements

Lecture Fluid system elements Lecture 8.1 Fluid system elements volumetric flowrate pressure drop Detailed distributed models of fluids, such as the Navier-Stokes equations, are necessary for understanding many aspects of fluid systems

More information

Lab 1: Dynamic Simulation Using Simulink and Matlab

Lab 1: Dynamic Simulation Using Simulink and Matlab Lab 1: Dynamic Simulation Using Simulink and Matlab Objectives In this lab you will learn how to use a program called Simulink to simulate dynamic systems. Simulink runs under Matlab and uses block diagrams

More information

Model-Based Design, Analysis, & Control: Valve-Controlled Hydraulic System K. Craig 1

Model-Based Design, Analysis, & Control: Valve-Controlled Hydraulic System K. Craig 1 Model-Based Design, Analysis, & Control: K. Craig 1 K. Craig K. Craig 3 K. Craig 4 K. Craig 5 Mission: It s All About Process Dynamic System Investigation K. Craig 6 K. Craig 7 K. Craig 8 K. Craig 9 K.

More information

LECTURE 6- ENERGY LOSSES IN HYDRAULIC SYSTEMS SELF EVALUATION QUESTIONS AND ANSWERS

LECTURE 6- ENERGY LOSSES IN HYDRAULIC SYSTEMS SELF EVALUATION QUESTIONS AND ANSWERS LECTURE 6- ENERGY LOSSES IN HYDRAULIC SYSTEMS SELF EVALUATION QUESTIONS AND ANSWERS 1. What is the head loss ( in units of bars) across a 30mm wide open gate valve when oil ( SG=0.9) flow through at a

More information

Lesson 6 Review of fundamentals: Fluid flow

Lesson 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 information

Dynamic Modeling of Fluid Power Transmissions for Wind Turbines

Dynamic Modeling of Fluid Power Transmissions for Wind Turbines Dynamic Modeling of Fluid Power Transmissions for Wind Turbines EWEA OFFSHORE 211 N.F.B. Diepeveen, A. Jarquin Laguna n.f.b.diepeveen@tudelft.nl, a.jarquinlaguna@tudelft.nl Offshore Wind Group, TU Delft,

More information

ENGI9496 Modeling and Simulation of Dynamic Systems Bond Graphs

ENGI9496 Modeling and Simulation of Dynamic Systems Bond Graphs ENGI9496 Modeling and Simulation of Dynamic Systems Bond Graphs Topics covered so far: Analogies between mechanical (translation and rotation), fluid, and electrical systems o Review of domain-specific

More information

Thermodynamics ENGR360-MEP112 LECTURE 7

Thermodynamics ENGR360-MEP112 LECTURE 7 Thermodynamics ENGR360-MEP11 LECTURE 7 Thermodynamics ENGR360/MEP11 Objectives: 1. Conservation of mass principle.. Conservation of energy principle applied to control volumes (first law of thermodynamics).

More information

FINAL EXAM. ME 200 Thermodynamics I, Spring 2013 CIRCLE YOUR LECTURE BELOW:

FINAL EXAM. ME 200 Thermodynamics I, Spring 2013 CIRCLE YOUR LECTURE BELOW: ME 200 Thermodynamics I, Spring 2013 CIRCLE YOUR LECTURE BELOW: Div. 5 7:30 am Div. 2 10:30 am Div. 4 12:30 am Prof. Naik Prof. Braun Prof. Bae Div. 3 2:30 pm Div. 1 4:30 pm Div. 6 4:30 pm Prof. Chen Prof.

More information

Therefore, the control volume in this case can be treated as a solid body, with a net force or thrust of. bm # V

Therefore, the control volume in this case can be treated as a solid body, with a net force or thrust of. bm # V When the mass m of the control volume remains nearly constant, the first term of the Eq. 6 8 simply becomes mass times acceleration since 39 CHAPTER 6 d(mv ) CV m dv CV CV (ma ) CV Therefore, the control

More information

ME-B41 Lab 1: Hydrostatics. Experimental Procedures

ME-B41 Lab 1: Hydrostatics. Experimental Procedures ME-B41 Lab 1: Hydrostatics In this lab you will do four brief experiments related to the following topics: manometry, buoyancy, forces on submerged planes, and hydraulics (a hydraulic jack). Each experiment

More information

Modeling of Dynamic Systems: Notes on Bond Graphs Version 1.0 Copyright Diane L. Peters, Ph.D., P.E.

Modeling of Dynamic Systems: Notes on Bond Graphs Version 1.0 Copyright Diane L. Peters, Ph.D., P.E. Modeling of Dynamic Systems: Notes on Bond Graphs Version 1.0 Copyright 2015 Diane L. Peters, Ph.D., P.E. Spring 2015 2 Contents 1 Overview of Dynamic Modeling 5 2 Bond Graph Basics 7 2.1 Causality.............................

More information

Load Prediction-based Energy-efficient Hydraulic Actuation. of a Robotic Arm. 1 Introduction

Load Prediction-based Energy-efficient Hydraulic Actuation. of a Robotic Arm. 1 Introduction oad rediction-based Energy-efficient Hydraulic ctuation of a Robotic rm Miss Can Du, rof ndrew lummer and Dr Nigel Johnston fixed displacement pump. This can reduce the weight of plant compared with the

More information

Chapter 6. Hydraulic cylinders/rams (linear motors), and Lines/fittings. - Transforms the flow of a pressurized fluid into a push or pull of a rod.

Chapter 6. Hydraulic cylinders/rams (linear motors), and Lines/fittings. - Transforms the flow of a pressurized fluid into a push or pull of a rod. Chapter 6. Hydraulic cylinders/rams (linear motors), and Lines/fittings - Transforms the flow of a pressurized fluid into a push or pull of a rod. 6. Single cting Rams Gravity, spring, etc. can force piston

More information

CLASS Fourth Units (Second part)

CLASS Fourth Units (Second part) CLASS Fourth Units (Second part) Energy analysis of closed systems Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display. MOVING BOUNDARY WORK Moving boundary work (P

More information

Check-Q-meter. Table of contents. Features. Functions. RE 27551/ /10 Replaces: Type FD

Check-Q-meter. Table of contents. Features. Functions. RE 27551/ /10 Replaces: Type FD Check-Q-meter RE /0.0 /0 Replaces: 09.9 Type FD Nominal size... Series ax. Operating pressure 0 bar ax. Flow 0 l/min K9/ Table of contents Contents Page Features Functions Ordering details Symbols Functional

More information

Index. Index. More information. in this web service Cambridge University Press

Index. Index. More information.  in this web service Cambridge University Press A-type elements, 4 7, 18, 31, 168, 198, 202, 219, 220, 222, 225 A-type variables. See Across variable ac current, 172, 251 ac induction motor, 251 Acceleration rotational, 30 translational, 16 Accumulator,

More information

Modelling the Dynamics of Flight Control Surfaces Under Actuation Compliances and Losses

Modelling the Dynamics of Flight Control Surfaces Under Actuation Compliances and Losses Modelling the Dynamics of Flight Control Surfaces Under Actuation Compliances and Losses Ashok Joshi Department of Aerospace Engineering Indian Institute of Technology, Bombay Powai, Mumbai, 4 76, India

More information

Research Article Modeling and Performance Improvement of the Constant Power Regulator Systems in Variable Displacement Axial Piston Pump

Research Article Modeling and Performance Improvement of the Constant Power Regulator Systems in Variable Displacement Axial Piston Pump The Scientific World Journal Volume 13, Article ID 7382, 11 pages http://dx.doi.org/1.1155/13/7382 Research Article Modeling and Performance Improvement of the Constant Power Regulator Systems in Variable

More information

Introduction to Turbomachinery

Introduction to Turbomachinery 1. Coordinate System Introduction to Turbomachinery Since there are stationary and rotating blades in turbomachines, they tend to form a cylindrical form, represented in three directions; 1. Axial 2. Radial

More information

Lecture 13 HYDRAULIC ACTUATORS[CONTINUED]

Lecture 13 HYDRAULIC ACTUATORS[CONTINUED] Lecture 1 HYDRAULIC ACTUATORS[CONTINUED] 1.5Acceleration and Deceleration of Cylinder Loads Cylinders are subjected to acceleration and deceleration during their oeration. Cylinders are decelerated to

More information

Dynamics of the synchronous machine

Dynamics of the synchronous machine ELEC0047 - Power system dynamics, control and stability Dynamics of the synchronous machine Thierry Van Cutsem t.vancutsem@ulg.ac.be www.montefiore.ulg.ac.be/~vct October 2018 1 / 38 Time constants and

More information

Lecture 9 - Rotational Dynamics

Lecture 9 - Rotational Dynamics Lecture 9 - Rotational Dynamics A Puzzle... Angular momentum is a 3D vector, and changing its direction produces a torque τ = dl. An important application in our daily lives is that bicycles don t fall

More information

Design and Modeling of Fluid Power Systems ME 597/ABE Lecture 7

Design and Modeling of Fluid Power Systems ME 597/ABE Lecture 7 Systems ME 597/ABE 591 - Lecture 7 Dr. Monika Ivantysynova MAHA Professor Fluid Power Systems MAHA Fluid Power Research Center Purdue University Content of 6th lecture The lubricating gap as a basic design

More information

Received 21 April 2008; accepted 6 January 2009

Received 21 April 2008; accepted 6 January 2009 Indian Journal of Engineering & Materials Sciences Vol. 16, February 2009, pp. 7-13 Inestigation on the characteristics of a new high frequency three-way proportional pressure reducing ale in ariable ale

More information

Chapter 5. Mass and Energy Analysis of Control Volumes. by Asst. Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn

Chapter 5. Mass and Energy Analysis of Control Volumes. by Asst. Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn Chapter 5 Mass and Energy Analysis of Control Volumes by Asst. Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn Reference: Cengel, Yunus A. and Michael A. Boles, Thermodynamics:

More information

Performance Modeling of a Piezohydraulic Actuator with Active Valves

Performance Modeling of a Piezohydraulic Actuator with Active Valves Performance Modeling of a Piezohydraulic Actuator with Active Valves H. Tan, W. Hurst, and D. J. Leo Center for Intelligent Material Systems and Structures Mechanical Engineering Department Virginia Tech

More information

HARDWARE-IN-THE-LOOP SIMULATION EXPERIMENTS WITH A HYDRAULIC MANIPULATOR MODEL

HARDWARE-IN-THE-LOOP SIMULATION EXPERIMENTS WITH A HYDRAULIC MANIPULATOR MODEL HARDWARE-IN-THE-LOOP SIMULATION EXPERIMENTS WITH A HYDRAULIC MANIPULATOR MODEL Jorge A. Ferreira, André F. Quintã, Carlos M. Cabral Departament of Mechanical Engineering University of Aveiro, Portugal

More information

Available online at ScienceDirect. Procedia Engineering 106 (2015 ) Dynamics and Vibroacoustics of Machines (DVM2014)

Available online at  ScienceDirect. Procedia Engineering 106 (2015 ) Dynamics and Vibroacoustics of Machines (DVM2014) Available online at www.sciencedirect.com ScienceDirect Procedia Engineering (5 ) 49 57 Dynamics and Vibroacoustics of Machines (DVM4) Process simulation of energy behaviour of pneumatic drives Elvira

More information

Simulation Study on Pressure Control using Nonlinear Input/Output Linearization Method and Classical PID Approach

Simulation Study on Pressure Control using Nonlinear Input/Output Linearization Method and Classical PID Approach Simulation Study on Pressure Control using Nonlinear Input/Output Linearization Method and Classical PID Approach Ufuk Bakirdogen*, Matthias Liermann** *Institute for Fluid Power Drives and Controls (IFAS),

More information

Modeling and Simulation Revision III D R. T A R E K A. T U T U N J I P H I L A D E L P H I A U N I V E R S I T Y, J O R D A N

Modeling and Simulation Revision III D R. T A R E K A. T U T U N J I P H I L A D E L P H I A U N I V E R S I T Y, J O R D A N Modeling and Simulation Revision III D R. T A R E K A. T U T U N J I P H I L A D E L P H I A U N I V E R S I T Y, J O R D A N 0 1 4 Block Diagrams Block diagram models consist of two fundamental objects:

More information

Stevens High School AP Physics II Work for Not-school

Stevens High School AP Physics II Work for Not-school 1. (AP SAMPLE QUESTION) An ideal fluid is flowing with a speed of 12 cm/s through a pipe of diameter 5 cm. The pipe splits into three smaller pipes, each with a diameter of 2 cm. What is the speed of the

More information

HYDRAULIC LINEAR ACTUATOR VELOCITY CONTROL USING A FEEDFORWARD-PLUS-PID CONTROL

HYDRAULIC LINEAR ACTUATOR VELOCITY CONTROL USING A FEEDFORWARD-PLUS-PID CONTROL HYDRAULIC LINEAR ACTUATOR VELOCITY CONTROL UING A FEEDFORWARD-PLU-PID CONTROL Qin Zhang Department of Agricultural Engineering University of Illinois at Urbana-Champaign, Urbana, IL 68 ABTRACT: A practical

More information

Chapter 7. Entropy. by Asst.Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn

Chapter 7. Entropy. by Asst.Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn Chapter 7 Entropy by Asst.Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn Reference: Cengel, Yunus A. and Michael A. Boles, Thermodynamics: An Engineering Approach, 5th ed.,

More information

COURSE 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 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 information

M O D U L E - 3A Model A10V0 Piston Pump Manual A10V0 PUMP. Features

M O D U L E - 3A Model A10V0 Piston Pump Manual A10V0 PUMP. Features T E C H N I C A L I N F O R M A T I O N M A N U A L F O R T H E A 1 0 V 0 V A R I A B L E D I S P L A C E M E N T P U M P S A10V0 PUMP Features High Efficiency through load sensing (= fuel savings) Maximum

More information

Answers to questions in each section should be tied together and handed in separately.

Answers to questions in each section should be tied together and handed in separately. EGT0 ENGINEERING TRIPOS PART IA Wednesday 4 June 014 9 to 1 Paper 1 MECHANICAL ENGINEERING Answer all questions. The approximate number of marks allocated to each part of a question is indicated in the

More information

The Bernoulli Equation

The Bernoulli Equation The Bernoulli Equation The most used and the most abused equation in fluid mechanics. Newton s Second Law: F = ma In general, most real flows are 3-D, unsteady (x, y, z, t; r,θ, z, t; etc) Let consider

More information

MODELLING AND CONTROL OF A SAUER DANFOSS PVG-32 VALVE

MODELLING AND CONTROL OF A SAUER DANFOSS PVG-32 VALVE MODELLING AND CONTROL OF A SAUER DANFOSS PVG-32 VALVE 5 semester project Group MCE5-522 Department of Energy Technology Aalborg university Autumn/winter 29 Title: Semester: Semester theme: Modelling and

More information

4 Mechanics of Fluids (I)

4 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 information

where = rate of change of total energy of the system, = rate of heat added to the system, = rate of work done by the system

where = rate of change of total energy of the system, = rate of heat added to the system, = rate of work done by the system The Energy Equation for Control Volumes Recall, the First Law of Thermodynamics: where = rate of change of total energy of the system, = rate of heat added to the system, = rate of work done by the system

More information

Objectives. Conservation of mass principle: Mass Equation The Bernoulli equation Conservation of energy principle: Energy equation

Objectives. Conservation of mass principle: Mass Equation The Bernoulli equation Conservation of energy principle: Energy equation Objectives Conservation of mass principle: Mass Equation The Bernoulli equation Conservation of energy principle: Energy equation Conservation of Mass Conservation of Mass Mass, like energy, is a conserved

More information

Newton's Laws You should be able to state these laws using both words and equations.

Newton's Laws You should be able to state these laws using both words and equations. Review before first test Physical Mechanics Fall 000 Newton's Laws You should be able to state these laws using both words and equations. The nd law most important for meteorology. Second law: net force

More information

Modeling, Control and Experimental Validation of a Device for Seismic Events Simulation

Modeling, Control and Experimental Validation of a Device for Seismic Events Simulation Modeling, Control and Experimental Validation of a Device for Seismic Events Simulation Paolo Righettini, Roberto Strada, Vittorio Lorenzi, Alberto Oldani, Mattia Rossetti Abstract Single and multi-axis

More information

Mathematical Modeling of a Two Spool Flow Control Servovalve Using a Pressure Control Pilot 1

Mathematical Modeling of a Two Spool Flow Control Servovalve Using a Pressure Control Pilot 1 Randall T. Anderson 2 e-mail: randalltanderson@eaton.com Perry Y. Li e-mail: pli@me.umn.edu Department of Mechanical Engineering, University of Minnesota, 111 Church St. SE, Minneapolis, MN 55455 Mathematical

More information

DEVELOPMENT OF MEASUREMENT STANDARD FOR DYNAMIC PRESSURE AT MIKES

DEVELOPMENT OF MEASUREMENT STANDARD FOR DYNAMIC PRESSURE AT MIKES DEVELOPMENT OF MEASUREMENT STANDARD FOR DYNAMIC PRESSURE AT MIKES Sari Saxholm, Antti Lakka, Martti Heinonen, Kari Riski MIKES, Centre for Metrology and Accreditation Tekniikantie 1, Espoo Finland telephone:

More information

MOMENTUM PRINCIPLE. Review: Last time, we derived the Reynolds Transport Theorem: Chapter 6. where B is any extensive property (proportional to mass),

MOMENTUM PRINCIPLE. Review: Last time, we derived the Reynolds Transport Theorem: Chapter 6. where B is any extensive property (proportional to mass), Chapter 6 MOMENTUM PRINCIPLE Review: Last time, we derived the Reynolds Transport Theorem: where B is any extensive property (proportional to mass), and b is the corresponding intensive property (B / m

More information

Translational Motion Rotational Motion Equations Sheet

Translational Motion Rotational Motion Equations Sheet PHYSICS 01 Translational Motion Rotational Motion Equations Sheet LINEAR ANGULAR Time t t Displacement x; (x = rθ) θ Velocity v = Δx/Δt; (v = rω) ω = Δθ/Δt Acceleration a = Δv/Δt; (a = rα) α = Δω/Δt (

More information

Applied Fluid Mechanics

Applied 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 information

Mechatronics Exercise: Modeling, Analysis, & Control of an Electrohydraulic Valve-Controlled Servomechanism

Mechatronics Exercise: Modeling, Analysis, & Control of an Electrohydraulic Valve-Controlled Servomechanism Mechatronics Exercise: Modeling, Analysis, & Control of an Electrohydraulic Valve-Controlled Servomechanism 11 Introduction Although a wide variety of detailed hydraulic control schemes are in use, a useful

More information

CHAPTER 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES

CHAPTER 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES Thermodynamics: An Engineering Approach 8th Edition in SI Units Yunus A. Çengel, Michael A. Boles McGraw-Hill, 2015 CHAPTER 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES Lecture slides by Dr. Fawzi Elfghi

More information

PHYA5/2C. (JUN15PHYA52C01) WMP/Jun15/PHYA5/2C/E5. General Certificate of Education Advanced Level Examination June Section B PMT TOTAL

PHYA5/2C. (JUN15PHYA52C01) WMP/Jun15/PHYA5/2C/E5. General Certificate of Education Advanced Level Examination June Section B PMT TOTAL Centre Number Candidate Number For Examiner s Use Surname Other Names Candidate Signature Examiner s Initials General Certificate of Education Advanced Level Examination June 2015 Question 1 2 Mark Physics

More information

Project TOUCAN. A Study of a Two-Can System. Prof. R.G. Longoria Update Fall ME 144L Prof. R.G. Longoria Dynamic Systems and Controls Laboratory

Project TOUCAN. A Study of a Two-Can System. Prof. R.G. Longoria Update Fall ME 144L Prof. R.G. Longoria Dynamic Systems and Controls Laboratory Project TOUCAN A Study of a Two-Can System Prof. R.G. Longoria Update Fall 2009 Laboratory Goals Gain familiarity with building models that reflect reality. Show how a model can be used to guide physical

More information

9. Pumps (compressors & turbines) Partly based on Chapter 10 of the De Nevers textbook.

9. 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 information

PROBLEM SET 6. SOLUTIONS April 1, 2004

PROBLEM SET 6. SOLUTIONS April 1, 2004 Harvard-MIT Division of Health Sciences and Technology HST.54J: Quantitative Physiology: Organ Transport Systems Instructors: Roger Mark and Jose Venegas MASSACHUSETTS INSTITUTE OF TECHNOLOGY Departments

More information

Contents. Dynamics and control of mechanical systems. Focus on

Contents. Dynamics and control of mechanical systems. Focus on Dynamics and control of mechanical systems Date Day 1 (01/08) Day 2 (03/08) Day 3 (05/08) Day 4 (07/08) Day 5 (09/08) Day 6 (11/08) Content Review of the basics of mechanics. Kinematics of rigid bodies

More information

Exam 3 Practice Solutions

Exam 3 Practice Solutions Exam 3 Practice Solutions Multiple Choice 1. A thin hoop, a solid disk, and a solid sphere, each with the same mass and radius, are at rest at the top of an inclined plane. If all three are released at

More information

DSCC PASSIVE CONTROL OF A HYDRAULIC HUMAN POWER AMPLIFIER USING A HYDRAULIC TRANSFORMER

DSCC PASSIVE CONTROL OF A HYDRAULIC HUMAN POWER AMPLIFIER USING A HYDRAULIC TRANSFORMER Proceedings of the ASME 25 Dynamic Systems and Control Conference DSCC25 October 28-3, 25, Columbus, Ohio, USA DSCC25-9734 PASSIVE CONTROL OF A HYDRAULIC HUMAN POWER AMPLIFIER USING A HYDRAULIC TRANSFORMER

More information

Physics Nov Cooling by Expansion

Physics Nov Cooling by Expansion Physics 301 19-Nov-2004 25-1 Cooling by Expansion Now we re going to change the subject and consider the techniques used to get really cold temperatures. Of course, the best way to learn about these techniques

More information

EQUILIBRIUM and ELASTICITY

EQUILIBRIUM and ELASTICITY PH 221-1D Spring 2013 EQUILIBRIUM and ELASTICITY Lectures 30-32 Chapter 12 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition) 1 Chapter 12 Equilibrium and Elasticity In this chapter we will

More information

Modeling and Simulation for Automatic Control

Modeling and Simulation for Automatic Control Modeling and Simulation for Automatic Control Olav Egeland and Jan Tommy Gravdahl Norwegian University of Science and Technology Trondheim, Norway MARINE CYBERNETICS Г~Т.! " " http://www.mannecybemetics.com

More information

Lecture PowerPoints. Chapter 4 Physics: Principles with Applications, 7 th edition Giancoli

Lecture PowerPoints. Chapter 4 Physics: Principles with Applications, 7 th edition Giancoli Lecture PowerPoints Chapter 4 Physics: Principles with Applications, 7 th edition Giancoli This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching

More information

Investigation of a nonlinear dynamic hydraulic system model through the energy analysis approach

Investigation of a nonlinear dynamic hydraulic system model through the energy analysis approach Journal of Mechanical Science and Technology 3 (009) 973~979 Journal of Mechanical Science and Technology www.springerlink.com/content/1738-9x DOI.07/s6-009-081- Investigation of a nonlinear dynamic hydraulic

More information

Titre. AMESim and Common Rail type Injection Systems. Technical Bulletin n 110

Titre. AMESim and Common Rail type Injection Systems. Technical Bulletin n 110 Titre AMESim and Common Rail type Injection Systems Technical Bulletin n 110 How to contact IMAGINE: North America Europe Asia imagine-us@amesim.com imagine@amesim.com imagine-japan@amesim.com Visit www.amesim.com

More information

Today. What concepts did you find most difficult, or what would you like to be sure we discuss in lecture? EXAM 1. Friction (two types)

Today. What concepts did you find most difficult, or what would you like to be sure we discuss in lecture? EXAM 1. Friction (two types) Physics 101: Lecture 07 Frictional forces and circular motion What concepts did you find most difficult, or what would you like to be sure we discuss in lecture? i get confused as to which way the friction

More information

On Fluid Compressibility in Switch-Mode Hydraulic Circuits - Part II: Experimental Results

On Fluid Compressibility in Switch-Mode Hydraulic Circuits - Part II: Experimental Results On Fluid Compressibility in Switch-Mode Hydraulic Circuits - Part II: Experimental Results James D. Van de Ven Department of Mechanical Engineering Worcester Polytechnic Institute 100 Institute Rd. Worcester,

More information

Fluid Dynamics Exercises and questions for the course

Fluid Dynamics Exercises and questions for the course Fluid Dynamics Exercises and questions for the course January 15, 2014 A two dimensional flow field characterised by the following velocity components in polar coordinates is called a free vortex: u r

More information

Experiment (4): Flow measurement

Experiment (4): Flow measurement Experiment (4): Flow measurement Introduction: The flow measuring apparatus is used to familiarize the students with typical methods of flow measurement of an incompressible fluid and, at the same time

More information

Integrated analysis of hydraulic PTOs in WECs

Integrated analysis of hydraulic PTOs in WECs Integrated analysis of hydraulic PTOs in WECs Conference on CeSOS Highlights and AMOS Visions Limin Yang 29 th May, 2013, Trondheim Content Introduction Model description of wave energy converter (WEC)

More information

Modeling and Simulation Revision IV D R. T A R E K A. T U T U N J I P H I L A D E L P H I A U N I V E R S I T Y, J O R D A N

Modeling and Simulation Revision IV D R. T A R E K A. T U T U N J I P H I L A D E L P H I A U N I V E R S I T Y, J O R D A N Modeling and Simulation Revision IV D R. T A R E K A. T U T U N J I P H I L A D E L P H I A U N I V E R S I T Y, J O R D A N 2 0 1 7 Modeling Modeling is the process of representing the behavior of a real

More information

REE 307 Fluid Mechanics II. Lecture 1. Sep 27, Dr./ Ahmed Mohamed Nagib Elmekawy. Zewail City for Science and Technology

REE 307 Fluid Mechanics II. Lecture 1. Sep 27, Dr./ Ahmed Mohamed Nagib Elmekawy. Zewail City for Science and Technology REE 307 Fluid Mechanics II Lecture 1 Sep 27, 2017 Dr./ Ahmed Mohamed Nagib Elmekawy Zewail City for Science and Technology Course Materials drahmednagib.com 2 COURSE OUTLINE Fundamental of Flow in pipes

More information

Turbines and speed governors

Turbines and speed governors ELEC0047 - Power system dynamics, control and stability Turbines and speed governors Thierry Van Cutsem t.vancutsem@ulg.ac.be www.montefiore.ulg.ac.be/~vct November 2017 1 / 31 2 / 31 Steam turbines Turbines

More information

Control Engineering BDA30703

Control Engineering BDA30703 Control Engineering BDA30703 Lecture 4: Transducers Prepared by: Ramhuzaini bin Abd. Rahman Expected Outcomes At the end of this lecture, students should be able to; 1) Explain a basic measurement system.

More information

You know for EE 303 that electrical speed for a generator equals the mechanical speed times the number of poles, per eq. (1).

You know for EE 303 that electrical speed for a generator equals the mechanical speed times the number of poles, per eq. (1). Stability 1 1. Introduction We now begin Chapter 14.1 in your text. Our previous work in this course has focused on analysis of currents during faulted conditions in order to design protective systems

More information

AP Physics C Mechanics Objectives

AP Physics C Mechanics Objectives AP Physics C Mechanics Objectives I. KINEMATICS A. Motion in One Dimension 1. The relationships among position, velocity and acceleration a. Given a graph of position vs. time, identify or sketch a graph

More information

Chapter 12. Static Equilibrium and Elasticity

Chapter 12. Static Equilibrium and Elasticity Chapter 12 Static Equilibrium and Elasticity Static Equilibrium Equilibrium implies that the object moves with both constant velocity and constant angular velocity relative to an observer in an inertial

More information

LECTURE 9. Hydraulic machines III and EM machines 2002 MIT PSDAM LAB

LECTURE 9. Hydraulic machines III and EM machines 2002 MIT PSDAM LAB LECTURE 9 Hydraulic machines III and EM machines .000 DC Permanent magnet electric motors Topics of today s lecture: Project I schedule revisions Test Bernoulli s equation Electric motors Review I x B

More information

Cross Product Angular Momentum

Cross Product Angular Momentum Lecture 21 Chapter 12 Physics I Cross Product Angular Momentum Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsi IN THIS CHAPTER, you will continue discussing rotational dynamics

More information

THERMODYNAMICS, FLUID AND PLANT PROCESSES. The tutorials are drawn from other subjects so the solutions are identified by the appropriate tutorial.

THERMODYNAMICS, FLUID AND PLANT PROCESSES. The tutorials are drawn from other subjects so the solutions are identified by the appropriate tutorial. THERMODYNAMICS, FLUID AND PLANT PROCESSES The tutorials are drawn from other subjects so the solutions are identified by the appropriate tutorial. THERMODYNAMICS TUTORIAL 2 THERMODYNAMIC PRINCIPLES SAE

More information

COMPARISON OF TWO METHODS TO SOLVE PRESSURES IN SMALL VOLUMES IN REAL-TIME SIMULATION OF A MOBILE DIRECTIONAL CONTROL VALVE

COMPARISON OF TWO METHODS TO SOLVE PRESSURES IN SMALL VOLUMES IN REAL-TIME SIMULATION OF A MOBILE DIRECTIONAL CONTROL VALVE COMPARISON OF TWO METHODS TO SOLVE PRESSURES IN SMALL VOLUMES IN REAL-TIME SIMULATION OF A MOBILE DIRECTIONAL CONTROL VALVE Rafael ÅMAN*, Heikki HANDROOS*, Pasi KORKEALAAKSO** and Asko ROUVINEN** * Laboratory

More information

Texas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos

Texas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos Texas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos Lecture 6: Modeling of Electromechanical Systems Principles of Motor Operation

More information

Cartridge Valves Technical Information. Quick reference

Cartridge Valves Technical Information. Quick reference Quick reference Contents CPF0... 8. CP600-5... 8. CP60-5... 8. 066 handle kit... 8.5 MP06... 8.6 MP... 8.6 X05-FD0 Traction manifold... 8.9 X05-FD6 Traction manifold... 8.0 X05-FD0 Traction manifold...

More information

Chapter Two. Basic Thermodynamics, Fluid Mechanics: Definitions of Efficiency. Laith Batarseh

Chapter Two. Basic Thermodynamics, Fluid Mechanics: Definitions of Efficiency. Laith Batarseh Chapter Two Basic Thermodynamics, Fluid Mechanics: Definitions of Efficiency Laith Batarseh The equation of continuity Most analyses in this book are limited to one-dimensional steady flows where the velocity

More information

Physics Holiday Program

Physics Holiday Program Physics Holiday Program What we will cover here 1. Brief intro about Base quantities 2. Conversion of units with different prefixes 3. Technique to answer the 10m questions. Discussion Question 1: 1. Convert

More information

ME3560 Tentative Schedule Spring 2019

ME3560 Tentative Schedule Spring 2019 ME3560 Tentative Schedule Spring 2019 Week Number Date Lecture Topics Covered Prior to Lecture Read Section Assignment Prep Problems for Prep Probs. Must be Solved by 1 Monday 1/7/2019 1 Introduction to

More information

EXPERIMENT No.1 FLOW MEASUREMENT BY ORIFICEMETER

EXPERIMENT 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 information

Preparing for Six Flags Physics Concepts

Preparing for Six Flags Physics Concepts Preparing for Six Flags Physics Concepts uniform means constant, unchanging At a uniform speed, the distance traveled is given by Distance = speed x time At uniform velocity, the displacement is given

More information

Thermodynamics. Thermo : heat dynamics : motion Thermodynamics is the study of motion of heat. Time and Causality Engines Properties of matter

Thermodynamics. Thermo : heat dynamics : motion Thermodynamics is the study of motion of heat. Time and Causality Engines Properties of matter Thermodynamics Thermo : heat dynamics : motion Thermodynamics is the study of motion of heat. Time and Causality Engines Properties of matter Graeme Ackland Lecture 1: Systems and state variables September

More information

STABILITY OF PNEUMATIC and HYDRAULIC VALVES

STABILITY OF PNEUMATIC and HYDRAULIC VALVES STABILITY OF PNEUMATIC and HYDRAULIC VALVES These three tutorials will not be found in any examination syllabus. They have been added to the web site for engineers seeking knowledge on why valve elements

More information

Chapter 13 Lecture. Essential University Physics Richard Wolfson 2 nd Edition. Oscillatory Motion Pearson Education, Inc.

Chapter 13 Lecture. Essential University Physics Richard Wolfson 2 nd Edition. Oscillatory Motion Pearson Education, Inc. Chapter 13 Lecture Essential University Physics Richard Wolfson nd Edition Oscillatory Motion Slide 13-1 In this lecture you ll learn To describe the conditions under which oscillatory motion occurs To

More information