Prof. Dr.-Ing. F.-K. Benra. ISE Bachelor Course

Size: px
Start display at page:

Download "Prof. Dr.-Ing. F.-K. Benra. ISE Bachelor Course"

Transcription

1 University Duisburg-Essen Campus Duisburg Faculty of Engineering Science Examination: Fluid Machines Examiner: Prof. Dr.-Ing. F.-K. Benra Date of examination: Handling time: 120 Minutes ISE Bachelor Course Designated scores: Exercise 1 Exercise 2 Exercise 3 Exercise 4 Exercise 5 ( 18 points) ( 20 points) ( 22 points) ( 24 points) ( 16 points) Σ 100 points Permitted utilities: Table of formulas (provided), pocket calculator

2 Exercise 1 (18 points) For an exhaust turbo-supercharger the impeller of a single stage centripetal turbine should be designed for following data: mass flow rate: m& = 0,95 kg/s pressure ratio: p 0 /p 2 = 1,82 inlet pressure: p 0 = 1,82 bar inlet temperature: T 0 = 710 K b 1 Fluid: combustion gas with D1 R = 288 J/(kg K) κ =1,35 = const. Di2 Dm2 Da2 The single stage is a repeating stage with swirlfree outflow and with adiabatic change in state. For the design following data are known: Static polytropic efficiency of the stage: η T = 0,82 Static polytropic efficiency of the stator: η T = 0,84 Kinematic degree of reaction: ρ h = 0,5 Flow coefficient: ϕ 1 = ϕ 2 = 0,72 Diameter ratio: D m2 /D 1 = 0,46 The change in state in stator and rotor is approximately polytropic. 1.1 Calculate the rotational speed of the machine for an optimum specific speed of σ ym = 0, Calculate the impeller diameter D 1. Use the enclosed Cordier-diagram. 1.3 Calculate the pressure and the temperature at impeller inlet (p 1, T 1 ) and at impeller outlet (p 2, T 2 ). 1.4 Calculate the width b 1 of the impeller, as well as the inner diameter D i2 and the outer diameter D a2 of the impeller.

3

4 Exercise 2 (20 points) A multi-stage, radial turbo compressor compresses oxygen to a higher pressure level. The change in state from inlet to outlet of the machine is approximately polytropic and adiabatic. For the mentioned pressure and temperature range, the oxygen can be described as an ideal gas with constant specific heat. Following data are known: Specific heat of O 2 : c p = 917 J/kgK Specific gas constant of O 2 : R = 259,8 J/kgK Polytropic efficiency η = 0,8 Inlet temperature T E = 295 K Inlet pressure: p Ε = 1 bar Velocities in absolute frame of reference: c r E = c r A Pressure ratio: p A /p E = 6,5 2.1 Calculate the mean polytropic exponent for the change in state from inlet to outlet of the machine. 2.2 Calculate the temperature and the pressure at outlet of the machine. 2.3 Calculate the specific work a EA, the specific change in enthalpy Δh EA, the specific flow work y EA and the specific dissipation j EA of the machine. 2.4 Draw the polytropic change in state of the machine from inlet to outlet in a T,sdiagram. Mark the flow work y EA, the change in enthalpy Δh EA and the dissipation j EA. 2.5 Calculate the temperature T A,S at machine outlet for the case of an isentropic change in state. Calculate the isentropic efficiency. η S

5 Exercise 3 ( 22 points) A radial blower for the delivery of carbon dioxide is equipped with an impeller with radial ending blades (ß 2 = 90 o ). The flow in front of the impeller is swirl free. The blower stage satisfies the repetition condition. In addition the following data are known: Measured volume flow: V & = 10 m /s Density of the gas: ρ = 1,98 kg/m 3 Outer impeller diameter: D 2 = 1 m Inner impeller diameter: D 1 = 0,6 m Meridional velocity: c m1 = c m2 = c m3 = 30 m/s Mechanical efficiency: η mech = 0,98 Rotational speed: n = 1470 min -1 For the change in state inside the machine the gas can be assumed as incompressible. The machine can be assumed as adiabatic. 3.1 Draw a sketch of a meridional section of the machine. Indicate the flow planes 1, 2, Draw a sketch of the impeller in a cutting plane normal to the axis of rotation. Show the blades in this plane as a circular flat cascade. Show qualitatively the right shape of the blades and indicate the direction of rotation of the impeller. 3.3 Draw the non-dimensional velocity triangles of this blower stage. (scale u 2 /u 2 = 1 =ˆ 10 cm) 3.4 Calculate the kinematic degree of reaction ρ h and the enthalpy coefficient ψ h of the stage.

6 Exercise 4 ( 24 points) For an axial turbine stage the following data at midspan are known: Adiabatic change in state: q = 0 Constant flow coefficient: ϕ 0 = ϕ 1 = ϕ 2 = 0,417 Inflow velocity: c 0 = 125 m/s Swirl free impeller outflow: α 2 = 90 deg Kinematic degree of reaction: ρ h = 0 Diameter of the mean streamline: D m0 = D m1 = D m2 = 0,662 m Rotational speed: n = 144 s -1 Flow conditions upstream and downstream of the stage are the same ( repeating stage) 4.1 Draw the non-dimensional velocity diagrams to scale and show the quantities of ϕ, ψ h and ρ h in the velocity diagrams (scale: u/u = 5 cm). 4.2 What is the name of this kind of turbine stage? 4.3 Show the thermodynamic process of the turbine stage in a qualitatively correct h,sdiagram and show the enthalpy differences Δh, Δh, Δh, Δh t, Δh s and Δh s. 4.4 Draw a qualitatively correct meridional section of the stage and the trend of the static pressure from the entrance to the outlet of the stage in a diagram. 4.5 Draw circumferential sections of the stator and of the rotor blade rows with a minimum of two blades for each row. 4.6 Determine the enthalpy coefficient ψ h and the specific work a of this turbine stage.

7 Exercise 5 ( 16 points) In the enclosed diagram, the non-dimensional head characteristic ψ yt = f (ϕ 2 ) of a turbomachine stage is given. The following additional data are known: Adiabatic change in state: q = 0 Swirl free impeller inflow: α 1 = 90 deg Constant flow coefficient: ϕ 1 = ϕ 2 = ϕ 3 = 0,4 Ratio of impeller diameters: d 1 /d 2 = 0,6 Circumferential speed at impeller exit: u 2 = 250 m/s Flow conditions upstream and downstream of the stage are the same ( repeating stage) 5.1 Is the machine a turbine or a compressor? 5.2 Draw into the given diagram the theoretical head characteristic ht = f (ϕ2) (after streamline theory) of the stage. For ϕ 2 = 1,5 the amount of ψht is zero. 5.3 What kind of blades has the impeller (forward swept, radial ending, backward swept)? 5.4 Calculate the total polytropic efficiency η pol,t,a for the design point A of the stage. Draw into the given diagram [η pol,t = f (ϕ 2 )] the efficiency curve of the stage in a qualitative manner, outgoing from the efficiency η pol,t,a at the design point. 5.5 Calculate the specific losses j for the design point of the stage. ψ 5.6 Draw the non-dimensional velocity triangles of the stage for the design point (scale: u 2 / u 2 = 10cm).

8 Exercise 5: Non-dimensional characteristic Name: Matr.-Nr:

Prof. Dr.-Ing. F.-K. Benra. ISE batchelor course

Prof. Dr.-Ing. F.-K. Benra. ISE batchelor course University Duisburg-Essen Campus Duisburg Faculty of engineering Science Department of Mechanical Engineering Examination: Fluid Machines Examiner: Prof. Dr.-Ing. F.-K. Benra Date of examination: 06.03.2006

More information

Prof. Dr.-Ing. F.-K. Benra. ISE Bachelor Course

Prof. Dr.-Ing. F.-K. Benra. ISE Bachelor Course University Duisburg-Essen Campus Duisburg Faculty of Engineering Science Department of Mechanical Engineering Name Matr.- Nr. Examination: Fluid Machines Examiner: Prof. Dr.-Ing. F.-K. Benra Date of examination:

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

Radial Compressors. Damian Vogt Course MJ2429. Nomenclature

Radial Compressors. Damian Vogt Course MJ2429. Nomenclature Turbomachinery Lecture Notes 1 007-10-04 Radial Compressors Damian Vogt Course MJ49 Nomenclature Subscripts Symbol Denotation Unit c Absolute velocity m/s h Enthalpy J/kg m& Mass flow rate kg/s r Radius

More information

Design of Multistage Turbine

Design of Multistage Turbine Turbomachinery Lecture Notes 7-9-4 Design of Multistage Turbine Damian Vogt Course MJ49 Nomenclature Subscripts Symbol Denotation Unit c Absolute velocity m/s c p Specific heat J/kgK h Enthalpy J/kg m&

More information

3 Energy Exchange in Turbomachines

3 Energy Exchange in Turbomachines 3 Energy Exchange in Turbomachines Problem 1 The solved and unsolved examples of this chapter are meant to illustrate the various forms of velocity triangles and the variety of the turbomachines. In addition,

More information

Contents. 1 Introduction to Gas-Turbine Engines Overview of Turbomachinery Nomenclature...9

Contents. 1 Introduction to Gas-Turbine Engines Overview of Turbomachinery Nomenclature...9 Preface page xv 1 Introduction to Gas-Turbine Engines...1 Definition 1 Advantages of Gas-Turbine Engines 1 Applications of Gas-Turbine Engines 3 The Gas Generator 3 Air Intake and Inlet Flow Passage 3

More information

In this lecture... Centrifugal compressors Thermodynamics of centrifugal compressors Components of a centrifugal compressor

In this lecture... Centrifugal compressors Thermodynamics of centrifugal compressors Components of a centrifugal compressor Lect- 3 In this lecture... Centrifugal compressors Thermodynamics of centrifugal compressors Components of a centrifugal compressor Centrifugal compressors Centrifugal compressors were used in the first

More information

Turbomachinery. Hasan Ozcan Assistant Professor. Mechanical Engineering Department Faculty of Engineering Karabuk University

Turbomachinery. Hasan Ozcan Assistant Professor. Mechanical Engineering Department Faculty of Engineering Karabuk University Turbomachinery Hasan Ozcan Assistant Professor Mechanical Engineering Department Faculty of Engineering Karabuk University Introduction Hasan Ozcan, Ph.D, (Assistant Professor) B.Sc :Erciyes University,

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

Journal of Mechatronics, Electrical Power, and Vehicular Technology

Journal of Mechatronics, Electrical Power, and Vehicular Technology J. Mechatron. Electr. Power Veh. Technol 06 (2015) 39 8 Journal of Mechatronics, Electrical Power, and Vehicular Technology e-issn:2088-6985 p-issn: 2087-3379 www.mevjournal.com GEOMETRY ANALYSIS AND EFFECT

More information

Design of Radial Turbines & Turbochargers

Design of Radial Turbines & Turbochargers RMD50 Design of Radial Turbines & Turbochargers Session delivered by: Prof. Q. H. Nagpurwala 4 @ M S Ramaiah School of Advanced Studies, Bengaluru Session Objective RMD50 To discuss the design of radial

More information

In this lecture... Radial flow turbines Types of radial flow turbines Thermodynamics and aerodynamics Losses in radial flow turbines

In this lecture... Radial flow turbines Types of radial flow turbines Thermodynamics and aerodynamics Losses in radial flow turbines Lect- 35 1 In this lecture... Radial flow turbines Types of radial flow turbines Thermodynamics and aerodynamics Losses in radial flow turbines Radial turbines Lect-35 Development of radial flow turbines

More information

Introduction to Fluid Machines and Compressible Flow Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

Introduction to Fluid Machines and Compressible Flow Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Introduction to Fluid Machines and Compressible Flow Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Lecture - 21 Centrifugal Compressor Part I Good morning

More information

Turbomachinery & Turbulence. Lecture 2: One dimensional thermodynamics.

Turbomachinery & Turbulence. Lecture 2: One dimensional thermodynamics. Turbomachinery & Turbulence. Lecture 2: One dimensional thermodynamics. F. Ravelet Laboratoire DynFluid, Arts et Metiers-ParisTech February 3, 2016 Control volume Global balance equations in open systems

More information

(Refer Slide Time: 4:41)

(Refer Slide Time: 4:41) Fluid Machines. Professor Sankar Kumar Som. Department Of Mechanical Engineering. Indian Institute Of Technology Kharagpur. Lecture-30. Basic Principle and Energy Transfer in Centrifugal Compressor Part

More information

PEMP RMD510. M.S. Ramaiah School of Advanced Studies, Bengaluru

PEMP RMD510. M.S. Ramaiah School of Advanced Studies, Bengaluru Design of Axial Flow Compressor- Session delivered by: Prof. Q. H. Nagpurwala Session Objectives To learn design procedure for axial compressor stages To calculate flow properties across the blade rows

More information

Please welcome for any correction or misprint in the entire manuscript and your valuable suggestions kindly mail us

Please welcome for any correction or misprint in the entire manuscript and your valuable suggestions kindly mail us Problems of Practices Of Fluid Mechanics Compressible Fluid Flow Prepared By Brij Bhooshan Asst. Professor B. S. A. College of Engg. And Technology Mathura, Uttar Pradesh, (India) Supported By: Purvi Bhooshan

More information

Lect 22. Radial Flow Turbines. Prof. Bhaskar Roy, Prof. A M Pradeep, Department of Aerospace, IIT Bombay

Lect 22. Radial Flow Turbines. Prof. Bhaskar Roy, Prof. A M Pradeep, Department of Aerospace, IIT Bombay Lecture Lect Radial Flow Turbines Lect Radial inflow turbines, which look similar to centrifugal compressor, are considered suitable for application in small aircraft engines. In many applications a radial

More information

MECA-H-402: Turbomachinery course Axial compressors

MECA-H-402: Turbomachinery course Axial compressors MECA-H-40: Turbomachinery course Axial compressors Pr. Patrick Hendrick Aero-Thermo-Mecanics Year 013-014 Contents List of figures iii 1 Axial compressors 1 1.1 Introduction...............................

More information

Contents. 2 Basic Components Aerofoils Force Generation Performance Parameters xvii

Contents. 2 Basic Components Aerofoils Force Generation Performance Parameters xvii Contents 1 Working Principles... 1 1.1 Definition of a Turbomachine... 1 1.2 Examples of Axial Turbomachines... 2 1.2.1 Axial Hydraulic Turbine... 2 1.2.2 Axial Pump... 4 1.3 Mean Line Analysis... 5 1.4

More information

Theory of turbo machine Effect of Blade Configuration on Characteristics of Centrifugal machines. Unit 2 (Potters & Wiggert Sec

Theory of turbo machine Effect of Blade Configuration on Characteristics of Centrifugal machines. Unit 2 (Potters & Wiggert Sec Theory of turbo machine Effect of Blade Configuration on Characteristics of Centrifugal machines Unit (Potters & Wiggert Sec. 1..1, &-607) Expression relating Q, H, P developed by Rotary machines Rotary

More information

Performance characteristics of turbo blower in a refuse collecting system according to operation conditions

Performance characteristics of turbo blower in a refuse collecting system according to operation conditions Journal of Mechanical Science and Technology 22 (2008) 1896~1901 Journal of Mechanical Science and Technology www.springerlink.com/content/1738-494x DOI 10.1007/s12206-008-0729-6 Performance characteristics

More information

Turbomachinery Aerodynamics Prof. Bhaskar Roy Prof. A M Pradeep Department of Aerospace Engineering Indian Institute of Technology, Bombay

Turbomachinery Aerodynamics Prof. Bhaskar Roy Prof. A M Pradeep Department of Aerospace Engineering Indian Institute of Technology, Bombay Turbomachinery Aerodynamics Prof. Bhaskar Roy Prof. A M Pradeep Department of Aerospace Engineering Indian Institute of Technology, Bombay Lecture No. # 26 Tutorial 4: 3D Flows in Axial Flow Turbines We

More information

Modeling and Validation of the SR-30 Turbojet Engine

Modeling and Validation of the SR-30 Turbojet Engine Modeling and Validation of the SR-30 Turbojet Engine Thermal Energy Technology 6. Semester Group TE6-604 Aalborg University Title: Modeling and Validation of the SR-30 Turbojet Engine Semester: 6. Semester

More information

ENERGY TRANSFER BETWEEN FLUID AND ROTOR. Dr. Ir. Harinaldi, M.Eng Mechanical Engineering Department Faculty of Engineering University of Indonesia

ENERGY TRANSFER BETWEEN FLUID AND ROTOR. Dr. Ir. Harinaldi, M.Eng Mechanical Engineering Department Faculty of Engineering University of Indonesia ENERGY TRANSFER BETWEEN FLUID AND ROTOR Dr. Ir. Harinaldi, M.Eng Mechanical Engineering Department Faculty of Engineering University of Indonesia Basic Laws and Equations Continuity Equation m m ρ mass

More information

EFFECT OF FORCED ROTATING VANELESS DIFFUSERS ON CENTRIFUGAL COMPRESSOR STAGE PERFORMANCE

EFFECT OF FORCED ROTATING VANELESS DIFFUSERS ON CENTRIFUGAL COMPRESSOR STAGE PERFORMANCE Journal of Engineering Science and Technology Vol. 6, No. 5 (2011) 558-574 School of Engineering, Taylor s University EFFECT OF FORCED ROTATING VANELESS DIFFUSERS ON CENTRIFUGAL COMPRESSOR STAGE PERFORMANCE

More information

One-Dimensional Isentropic Flow

One-Dimensional Isentropic Flow Cairo University Second Year Faculty of Engineering Gas Dynamics AER 201B Aerospace Department Sheet (1) 2011-2012 One-Dimensional Isentropic Flow 1. Assuming the flow of a perfect gas in an adiabatic,

More information

Lect-36. In this lecture... Tutorial on radial flow turbines. Prof. Bhaskar Roy, Prof. A M Pradeep, Department of Aerospace, IIT Bombay

Lect-36. In this lecture... Tutorial on radial flow turbines. Prof. Bhaskar Roy, Prof. A M Pradeep, Department of Aerospace, IIT Bombay Lect- 36 1 In this lecture... Lect-36 Tutorial on radial flow turbines 2 Problem # 1 Lect-36 The rotor of an IFR turbine, which is designed to operate at the nominal condition, is 23.76 cm in diameter

More information

Specific Static rotor work ( P P )

Specific Static rotor work ( P P ) The specific Static Rotor ork p 1 ρ Specific Static rotor work ( P P ) here P, P static pressures at points, (P P ) static pressure difference of the rotor ρ density, in case of a compressible medium average

More information

MAHALAKSHMI ENGINEERING COLLEGE

MAHALAKSHMI ENGINEERING COLLEGE MAHALAKSHMI ENGINEERING COLLEGE TIRUCHIRAPALLI-621213. Department: Mechanical Subject Code: ME2202 U N IT - 1 Semester: III Subject Name: ENGG. THERMODYNAMICS 1. 1 kg of gas at 1.1 bar, 27 o C is compressed

More information

Simple, stable and reliable modeling of gas properties of organic working fluids in aerodynamic designs of turbomachinery for ORC and VCC

Simple, stable and reliable modeling of gas properties of organic working fluids in aerodynamic designs of turbomachinery for ORC and VCC IOP Conference Series: Materials Science and Engineering PAPER OPEN ACCESS Simple, stable and reliable modeling of gas properties of organic working fluids in aerodynamic designs of turbomachinery for

More information

Laboratory Notes Heat and Power Division Royal Institute of Technology Stockholm, Sweden

Laboratory Notes Heat and Power Division Royal Institute of Technology Stockholm, Sweden Laboratory Notes Determination of Losses in a Linear Cascade (approx. hours laboratory exercise) Blades Stepper motor for moving the probes By Navarathna N. and Wei N. Division of Heat and Power Technology

More information

Axial Flow and Radial Flow Gas Turbines

Axial Flow and Radial Flow Gas Turbines 7 Axial Flow and Radial Flow Gas Turbines 7.1 INTRODUCTION TO AXIAL FLOW TURBINES The axial flow gas turbine is used in almost all applications of gas turbine power plant. Development of the axial flow

More information

Introduction to Fluid Machines and Compressible Flow Prof. S.K Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

Introduction to Fluid Machines and Compressible Flow Prof. S.K Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Introduction to Fluid Machines and Compressible Flow Prof. S.K Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Lecture No. # 24 Axial Flow Compressor Part I Good morning

More information

Two mark questions and answers UNIT I BASIC CONCEPT AND FIRST LAW SVCET

Two mark questions and answers UNIT I BASIC CONCEPT AND FIRST LAW SVCET Two mark questions and answers UNIT I BASIC CONCEPT AND FIRST LAW 1. What do you understand by pure substance? A pure substance is defined as one that is homogeneous and invariable in chemical composition

More information

Introduction to Fluid Machines and Compressible Flow Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

Introduction to Fluid Machines and Compressible Flow Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Introduction to Fluid Machines and Compressible Flow Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Lecture - 1 Introduction to Fluid Machines Well, good

More information

COMPUTER AIDED DESIGN OF RADIAL TIPPED CENTRIFUGAL BLOWERS AND FANS

COMPUTER AIDED DESIGN OF RADIAL TIPPED CENTRIFUGAL BLOWERS AND FANS 4 th International Conference on Mechanical Engineering, December 26-28, 21, Dhaka, Bangladesh/pp. IV 55-6 COMPUTER AIDED DESIGN OF RADIAL TIPPED CENTRIFUGAL BLOWERS AND FANS Nitin N. Vibhakar* and S.

More information

Study of the Losses in Fluid Machinery with the Help of Entropy

Study of the Losses in Fluid Machinery with the Help of Entropy Study of the Losses in Fluid Machinery with the Help of Entropy Martin Böhle 1, Annika Fleder 1, Matthias Mohr 1 * SYMPOSIA ON ROTATING MACHINERY ISROMAC 16 International Symposium on Transport Phenomena

More information

Chapter three. Two-dimensional Cascades. Laith Batarseh

Chapter three. Two-dimensional Cascades. Laith Batarseh Chapter three Two-dimensional Cascades Laith Batarseh Turbo cascades The linear cascade of blades comprises a number of identical blades, equally spaced and parallel to one another cascade tunnel low-speed,

More information

Lecture-10 Tutorial -2 Solved Problems and Tutorial Problems On Three Dimensional flow in Axial Flow Compressor

Lecture-10 Tutorial -2 Solved Problems and Tutorial Problems On Three Dimensional flow in Axial Flow Compressor 1 Lecture-10 Tutorial -2 Solved Problems and Tutorial Problems On Three Dimensional flow in Axial Flow Compressor 2 Recap of simple 3-D flow theories (These are mainly used for design) Lect-10 1)Free Vortex

More information

10 minutes reading time is allowed for this paper.

10 minutes reading time is allowed for this paper. EGT1 ENGINEERING TRIPOS PART IB Tuesday 31 May 2016 2 to 4 Paper 4 THERMOFLUID MECHANICS Answer not more than four questions. Answer not more than two questions from each section. All questions carry the

More information

mywbut.com Hydraulic Turbines

mywbut.com Hydraulic Turbines Hydraulic Turbines Hydro-electric power accounts for up to 0% of the world s electrical generation. Hydraulic turbines come in a variety of shapes determined by the available head and a number of sizes

More information

BME-A PREVIOUS YEAR QUESTIONS

BME-A PREVIOUS YEAR QUESTIONS BME-A PREVIOUS YEAR QUESTIONS CREDITS CHANGE ACCHA HAI TEAM UNIT-1 Introduction: Introduction to Thermodynamics, Concepts of systems, control volume, state, properties, equilibrium, quasi-static process,

More information

Unified Propulsion Quiz May 7, 2004

Unified Propulsion Quiz May 7, 2004 Unified Propulsion Quiz May 7, 2004 Closed Book no notes other than the equation sheet provided with the exam Calculators allowed. Put your name on each page of the exam. Read all questions carefully.

More information

AEROSPACE ENGINEERING DEPARTMENT. Second Year - Second Term ( ) Fluid Mechanics & Gas Dynamics

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 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

Principles of Turbomachinery

Principles of Turbomachinery Principles of Turbomachinery To J. M. T. Principles of Turbomachinery R. K. Turton Lecturer in Mechanical Engineering Loughborough University of Technology London New York E. & F. N. Spon ISBN 978-94-010-9691-1

More information

SOE2156: Fluids Lecture 4

SOE2156: Fluids Lecture 4 Turbo SOE2156: s Lecture 4 machine { a device exchanging energy (work) between a uid and a mechanical system. In particular : a turbomachine is a device using a rotating mechanical system. The ow of energy

More information

Where F1 is the force and dl1 is the infinitesimal displacement, but F1 = p1a1

Where F1 is the force and dl1 is the infinitesimal displacement, but F1 = p1a1 In order to force the fluid to flow across the boundary of the system against a pressure p1, work is done on the boundary of the system. The amount of work done is dw = - F1.dl1, Where F1 is the force

More information

A Numerical study of effect of Return Channel Vanes Shroud Wall Divergence Angle on the Cross-over System Performance in Centrifugal Compressors

A Numerical study of effect of Return Channel Vanes Shroud Wall Divergence Angle on the Cross-over System Performance in Centrifugal Compressors RESEARCH ARTICLE OPEN ACCESS A Numerical study of effect of Return Channel Vanes Shroud Wall Divergence Angle on the Cross-over System Performance in Centrifugal Compressors * K.Srinivasa Reddy *, M Sai

More information

Impact of Blade Quality on Maximum Efficiency of Low Head Hydraulic Turbine

Impact of Blade Quality on Maximum Efficiency of Low Head Hydraulic Turbine Mechanics and Mechanical Engineering Vol. 17, No. 3 2013) 269 284 c Lodz University of Technology Impact of Blade Quality on Maximum Efficiency of Low Head Hydraulic Turbine Romuald Puzyrewski Gdansk University

More information

Theory of turbo machinery / Turbomaskinernas teori. Dixon, chapter 7. Centrifugal Pumps, Fans and Compressors

Theory of turbo machinery / Turbomaskinernas teori. Dixon, chapter 7. Centrifugal Pumps, Fans and Compressors Theory of turbo machinery / Turbomaskinernas teori Dixon, chapter 7 Centrifugal Pumps, Fans and Compressors And to thy speed add wings. (MILTON, Paradise Lost.) What do radial machines look like? Swept

More information

Heat and Mass Transfer Prof. S.P. Sukhatme Department of Mechanical Engineering Indian Institute of Technology, Bombay

Heat and Mass Transfer Prof. S.P. Sukhatme Department of Mechanical Engineering Indian Institute of Technology, Bombay Heat and Mass Transfer Prof. S.P. Sukhatme Department of Mechanical Engineering Indian Institute of Technology, Bombay Lecture No. 18 Forced Convection-1 Welcome. We now begin our study of forced convection

More information

Turbine Blade Design of a Micro Gas Turbine

Turbine Blade Design of a Micro Gas Turbine Turbine Blade Design of a Micro Gas Turbine Bhagawat Yedla Vellore Institute of Technlogy, Vellore 632014, India Sanchit Nawal Vellore Institute of Technlogy, Vellore 632014, India Shreehari Murali Vellore

More information

Akshay Khadse, Lauren Blanchette, Mahmood Mohagheghi, Jayanta Kapat

Akshay Khadse, Lauren Blanchette, Mahmood Mohagheghi, Jayanta Kapat Impact of S-CO2 Properties on Centrifugal Compressor Impeller: Comparison of Two Loss Models for Mean Line Analyses The Supercritical CO2 Power Cycles Symposium 2016 Akshay Khadse, Lauren Blanchette, Mahmood

More information

UNIFIED DESIGN AND COMPARATIVE PERFORMANCE EVALUATION OF FORWARD AND BACKWARD CURVED RADIAL TIPPED CENTRIFUGAL FAN

UNIFIED DESIGN AND COMPARATIVE PERFORMANCE EVALUATION OF FORWARD AND BACKWARD CURVED RADIAL TIPPED CENTRIFUGAL FAN Proceedings of the International Conference on Mechanical Engineering 3 (ICME3) 6-8 December 3, Dhaka, Bangladesh ICME3-FL- UNIFIED DESIGN AND COMPARATIVE PERFORMANCE EVALUATION OF FORWARD AND BACKWARD

More information

M E 320 Professor John M. Cimbala Lecture 23

M E 320 Professor John M. Cimbala Lecture 23 M E 320 Professor John M. Cimbala Lecture 23 Today, we will: Discuss diffusers and do an example problem Begin discussing pumps, and how they are analyzed in pipe flow systems D. Diffusers 1. Introduction.

More information

ASSESSMENT OF DESIGN METHODOLOGY AND THREE DIMENSIONAL NUMERICAL (CFD) ANALYSIS OF CENTRIFUGAL BLOWER

ASSESSMENT OF DESIGN METHODOLOGY AND THREE DIMENSIONAL NUMERICAL (CFD) ANALYSIS OF CENTRIFUGAL BLOWER ASSESSMENT OF DESIGN METHODOLOGY AND THREE DIMENSIONAL NUMERICAL (CFD) ANALYSIS OF CENTRIFUGAL BLOWER D. R. Chaudhari 1, H. N. Patel 2 1,2 Mechanical Department, Government Engineering College Dahod, (India)

More information

ME Thermodynamics I

ME Thermodynamics I Homework - Week 01 HW-01 (25 points) Given: 5 Schematic of the solar cell/solar panel Find: 5 Identify the system and the heat/work interactions associated with it. Show the direction of the interactions.

More information

Stator Blade Motor Motor Housing

Stator Blade Motor Motor Housing The internal workings of a Ducted Fan The rotor velocity vectors and blade angles After looking at EDFs from a pure axial change of momentum position we must now address the question how the fan is shaped

More information

Introduction to Fluid Machines, and Compressible Flow Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

Introduction to Fluid Machines, and Compressible Flow Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Introduction to Fluid Machines, and Compressible Flow Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Lecture - 09 Introduction to Reaction Type of Hydraulic

More information

Signature: (Note that unsigned exams will be given a score of zero.)

Signature: (Note that unsigned exams will be given a score of zero.) Neatly print your name: Signature: (Note that unsigned exams will be given a score of zero.) Circle your lecture section (-1 point if not circled, or circled incorrectly): Prof. Dabiri Prof. Wassgren Prof.

More information

I. (20%) Answer the following True (T) or False (F). If false, explain why for full credit.

I. (20%) Answer the following True (T) or False (F). If false, explain why for full credit. I. (20%) Answer the following True (T) or False (F). If false, explain why for full credit. Both the Kelvin and Fahrenheit scales are absolute temperature scales. Specific volume, v, is an intensive property,

More information

Application of Computational Fluid Dynamics to Practical Design and Performance Analysis of Turbomachinery

Application of Computational Fluid Dynamics to Practical Design and Performance Analysis of Turbomachinery 10 Application of Computational Fluid Dynamics to Practical Design and Performance Analysis of Turbomachinery Hyoung Woo OH Chungju National University Korea 1. Introduction Over the past several decades,

More information

SECOND ENGINEER REG. III/2 APPLIED HEAT

SECOND ENGINEER REG. III/2 APPLIED HEAT SECOND ENGINEER REG. III/2 APPLIED HEAT LIST OF TOPICS A B C D E F G H I J K Pressure, Temperature, Energy Heat Transfer Internal Energy, Thermodynamic systems. First Law of Thermodynamics Gas Laws, Displacement

More information

(Refer Slide Time: 0:57)

(Refer Slide Time: 0:57) Fluid Dynamics And Turbo Machines. Professor Dr Dhiman Chatterjee. Department Of Mechanical Engineering. Indian Institute Of Technology Madras. Part B. Module-2. Lecture-4. Representation of Turbo Machines

More information

P 1 P * 1 T P * 1 T 1 T * 1. s 1 P 1

P 1 P * 1 T P * 1 T 1 T * 1. s 1 P 1 ME 131B Fluid Mechanics Solutions to Week Three Problem Session: Isentropic Flow II (1/26/98) 1. From an energy view point, (a) a nozzle is a device that converts static enthalpy into kinetic energy. (b)

More information

Preliminary design of a centrifugal turbine for ORC applications

Preliminary design of a centrifugal turbine for ORC applications ORC 2011 First International Seminar on ORC Power Systems TU Delft, The Netherlands, 22-23 September 2011 Preliminary design of a centrifugal turbine for ORC applications M. Pini 1, G. Persico 1, E. Casati

More information

Turbomachinery Flow Physics and Dynamic Performance

Turbomachinery Flow Physics and Dynamic Performance Turbomachinery Flow Physics and Dynamic Performance Bearbeitet von Meinhard T Schobeiri 1. Auflage 2004. Buch. XXI, 522 S. Hardcover ISBN 978 3 540 22368 9 Format (B x L): 15,5 x 23,5 cm Gewicht: 2070

More information

Effect of the Computational Domain Selection on the Calculation of Axial Fan Performance

Effect of the Computational Domain Selection on the Calculation of Axial Fan Performance Effect of the Computational Domain Selection on the Calculation of Axial Fan Performance Ayhan Nazmi İlikan 1 *, Erkan Ayder 2 ISROMAC 2016 International Symposium on Transport Phenomena and Dynamics of

More information

1. Basic state values of matter

1. Basic state values of matter 1. Basic state values of matter Example 1.1 The pressure inside a boiler is p p = 115.10 5 Pa and p v = 9.44.10 4 Pa inside a condenser. Calculate the absolute pressure inside the boiler and condenser

More information

Contents. Preface... xvii

Contents. Preface... xvii Contents Preface... xvii CHAPTER 1 Idealized Flow Machines...1 1.1 Conservation Equations... 1 1.1.1 Conservation of mass... 2 1.1.2 Conservation of momentum... 3 1.1.3 Conservation of energy... 3 1.2

More information

Numerical and Experimental Investigation of the Flow in a Centrifugal Pump Stage

Numerical and Experimental Investigation of the Flow in a Centrifugal Pump Stage Numerical and Experimental Investigation of the Flow in a Centrifugal Pump Stage FRIEDRICH-KARL BENRA, HANS JOSEF DOHMEN Faculty of Engineering Sciences Department of Mechanical Engineering, Turbomachinery

More information

Off-design flow analysis of low-pressure steam turbines

Off-design flow analysis of low-pressure steam turbines 215 Off-design flow analysis of low-pressure steam turbines M Petrovic 1 and WRiess 2 1 Department of Mechanical Engineering, University of Belgrade, Yugoslavia 2 Institute for Turbomachinery, University

More information

Application of Analytical and Numerical Methods for the Design of Transonic Axial Compressor Stages

Application of Analytical and Numerical Methods for the Design of Transonic Axial Compressor Stages Application of Analytical and Numerical Methods for the Design of Transonic Axial Compressor tages rof. Dr.-Ing. Martin Böhle Mechanical Engineering University of Wuppertal Gaußstraße 0, 4097 Wuppertal

More information

THERMAL ANALYSIS OF SECOND STAGE GAS TURBINE ROTOR BLADE

THERMAL ANALYSIS OF SECOND STAGE GAS TURBINE ROTOR BLADE Polymers Research Journal ISSN: 195-50 Volume 6, Number 01 Nova Science Publishers, Inc. THERMAL ANALYSIS OF SECOND STAGE GAS TURBINE ROTOR BLADE E. Poursaeidi, M. Mohammadi and S. S. Khamesi University

More information

ME 2322 Thermodynamics I PRE-LECTURE Lesson 23 Complete the items below Name:

ME 2322 Thermodynamics I PRE-LECTURE Lesson 23 Complete the items below Name: Lesson 23 1. (10 pt) Write the equation for the thermal efficiency of a Carnot heat engine below: 1 L H 2. (10 pt) Can the thermal efficiency of an actual engine ever exceed that of an equivalent Carnot

More information

vector H. If O is the point about which moments are desired, the angular moment about O is given:

vector H. If O is the point about which moments are desired, the angular moment about O is given: The angular momentum A control volume analysis can be applied to the angular momentum, by letting B equal to angularmomentum vector H. If O is the point about which moments are desired, the angular moment

More information

Jet Aircraft Propulsion Prof. Bhaskar Roy Prof A M Pradeep Department of Aerospace Engineering Indian Institute of Technology, Bombay

Jet Aircraft Propulsion Prof. Bhaskar Roy Prof A M Pradeep Department of Aerospace Engineering Indian Institute of Technology, Bombay Jet Aircraft Propulsion Prof. Bhaskar Roy Prof A M Pradeep Department of Aerospace Engineering Indian Institute of Technology, Bombay Module No. #01 Lecture No. # 07 Jet Engine Cycles For Aircraft propulsion

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

Lecture 22. Mechanical Energy Balance

Lecture 22. Mechanical Energy Balance Lecture 22 Mechanical Energy Balance Contents Exercise 1 Exercise 2 Exercise 3 Key Words: Fluid flow, Macroscopic Balance, Frictional Losses, Turbulent Flow Exercise 1 It is proposed to install a fan to

More information

Fan and Compressor Performance Scaling with Inlet Distortions

Fan and Compressor Performance Scaling with Inlet Distortions Fan and Compressor Performance Scaling with Inlet Distortions J. J. Defoe Turbomachinery and Unsteady Flows Research Group University of Windsor Windsor, ON, Canada UTIAS National Colloquium on Sustainable

More information

Theory of turbomachinery. Chapter 1

Theory of turbomachinery. Chapter 1 Theory of turbomachinery Chater Introduction: Basic Princiles Take your choice of those that can best aid your action. (Shakeseare, Coriolanus) Introduction Definition Turbomachinery describes machines

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

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

CALIFORNIA POLYTECHNIC STATE UNIVERSITY Mechanical Engineering Department ME 347, Fluid Mechanics II, Winter 2018

CALIFORNIA POLYTECHNIC STATE UNIVERSITY Mechanical Engineering Department ME 347, Fluid Mechanics II, Winter 2018 CALIFORNIA POLYTECHNIC STATE UNIVERSITY Mechanical Engineering Department ME 347, Fluid Mechanics II, Winter 2018 Date Day Subject Read HW Sept. 21 F Introduction 1, 2 24 M Finite control volume analysis

More information

Small Scale Axial Turbine Preliminary Design and Modelling

Small Scale Axial Turbine Preliminary Design and Modelling Small Scale Axial Turbine Preliminary Design and Modelling Shadreck M. Situmbeko University of Botswana, Gaborone, Botswana; University of KwaZulu-Natal, Durban, RSA; Freddie L. Inambao University of KwaZulu-Natal,

More information

Study on the Performance of a Sirocco Fan (Flow Around the Runner Blade)

Study on the Performance of a Sirocco Fan (Flow Around the Runner Blade) Rotating Machinery, 10(5): 415 424, 2004 Copyright c Taylor & Francis Inc. ISSN: 1023-621X print / 1542-3034 online DOI: 10.1080/10236210490474629 Study on the Performance of a Sirocco Fan (Flow Around

More information

CDF CALCULATION OF RADIAL FAN STAGE WITH VARIABLE LENGTH OF SEMI BLADES SVOČ FST 2012

CDF CALCULATION OF RADIAL FAN STAGE WITH VARIABLE LENGTH OF SEMI BLADES SVOČ FST 2012 CDF CALCULATION OF RADIAL FAN STAGE WITH VARIABLE LENGTH OF SEMI BLADES SVOČ FST 2012 Ing. Roman Gášpár, Západočeská univerzita v Plzni, Univerzitní 8, 306 14 Plzeň Česká republika NOMENCLATURE A area

More information

Introduction to Chemical Engineering Thermodynamics. Chapter 7. KFUPM Housam Binous CHE 303

Introduction to Chemical Engineering Thermodynamics. Chapter 7. KFUPM Housam Binous CHE 303 Introduction to Chemical Engineering Thermodynamics Chapter 7 1 Thermodynamics of flow is based on mass, energy and entropy balances Fluid mechanics encompasses the above balances and conservation of momentum

More information

Two Dimensional Design of Axial Compressor An Enhanced Version of LUAX-C

Two Dimensional Design of Axial Compressor An Enhanced Version of LUAX-C Two Dimensional Design of Axial Compressor An Enhanced Version of LUAX-C Daniele Perrotti Thesis for the Degree of Master of Science Division of Thermal Power Engineering Department of Energy Sciences

More information

Axial Flow Compressors and Fans

Axial Flow Compressors and Fans 5 Axial Flow Compressors and Fans 5.1 INTRODUCTION As mentioned in Chapter 4, the maximum pressure ratio achieved in centrifugal compressors is about 4:1 for simple machines (unless multi-staging is used)

More information

Theory and Applica0on of Gas Turbine Systems

Theory and Applica0on of Gas Turbine Systems Theory and Applica0on of Gas Turbine Systems Part IV: Axial and Radial Flow Turbines Munich Summer School at University of Applied Sciences Prof. Kim A. Shollenberger Introduc0on to Turbines Two basic

More information

IX. COMPRESSIBLE FLOW. ρ = P

IX. COMPRESSIBLE FLOW. ρ = P IX. COMPRESSIBLE FLOW Compressible flow is the study of fluids flowing at speeds comparable to the local speed of sound. This occurs when fluid speeds are about 30% or more of the local acoustic velocity.

More information

Centrifugal Machines Table of Contents

Centrifugal Machines Table of Contents NLNG Course 017 Table of Contents 1 Introduction and Basic Principles... 1.1 Hydraulic Machines... 1.... 1.3 Pump Geometry... 1.4 Pump Blade Geometry...3 1.5 Diffusers...5 1.6 Pump Losses...6 1.7 Example

More information

Exercise 8 - Turbocompressors

Exercise 8 - Turbocompressors Exercise 8 - Turbocompressors A turbocompressor TC) or turbocharger is a mechanical device used in internal combustion engines to enhance their power output. The basic idea of a TC is to force additional

More information

EXPLORING THE DESIGN SPACE OF THE SCO2 POWER CYCLE COMPRESSOR

EXPLORING THE DESIGN SPACE OF THE SCO2 POWER CYCLE COMPRESSOR The 4th International Symposium - Supercritical CO2 Power Cycles September 9-10, 2014, Pittsburgh, Pennsylvania EXPLORING THE DESIGN SPACE OF THE SCO2 POWER CYCLE COMPRESSOR Benjamín Monge Postdoc researcher

More information

MODELLING OF SINGLE-PHASE FLOW IN THE STATOR CHANNELS OF SUBMERSIBLE AERATOR

MODELLING OF SINGLE-PHASE FLOW IN THE STATOR CHANNELS OF SUBMERSIBLE AERATOR Engineering MECHANICS, Vol. 21, 2014, No. 5, p. 289 298 289 MODELLING OF SINGLE-PHASE FLOW IN THE STATOR CHANNELS OF SUBMERSIBLE AERATOR Martin Bílek*, Jaroslav Štigler* The paper deals with the design

More information