M E 320 Professor John M. Cimbala Lecture 23

Similar documents
CHAPTER EIGHT P U M P I N G O F L I Q U I D S

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

(Refer Slide Time: 4:41)

COURSE CODE : 3072 COURSE CATEGORY : B PERIODS/ WEEK : 5 PERIODS/ SEMESTER : 75 CREDIT : 5 TIME SCHEDULE

SOE2156: Fluids Lecture 4

Chapter Four Hydraulic Machines

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

Chapter Four fluid flow mass, energy, Bernoulli and momentum

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

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

Applied Fluid Mechanics

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

M E 320 Professor John M. Cimbala Lecture 24

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

Chapter Four Hydraulic Machines

DESIGN AND CFD ANALYSIS OF A CENTRIFUGAL PUMP

Department of Civil and Environmental Engineering CVNG 1001: Mechanics of Fluids

Radial Compressors. Damian Vogt Course MJ2429. Nomenclature

(Refer Slide Time: 0:45)

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

4 Mechanics of Fluids (I)

CLASS Fourth Units (Second part)

Chapter 7 The Energy Equation

FLOW IN PIPES. Mark J McCready University of Notre Dame July 24, chemeprof.com

Lecture 22. Mechanical Energy Balance

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

Conservation of Angular Momentum

CHAPTER TWO CENTRIFUGAL PUMPS 2.1 Energy Transfer In Turbo Machines

Chapter 7. Introduction to Fluid Machinery

mywbut.com Hydraulic Turbines

University of Washington Department of Chemistry Chemistry 452 Summer Quarter 2014

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

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

M E 320 Professor John M. Cimbala Lecture 05

Thermodynamics ENGR360-MEP112 LECTURE 7

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

MASS, MOMENTUM, AND ENERGY EQUATIONS

Chapter 5. Mass and Energy Analysis of Control Volumes

Dr. S. Ramachandran Prof. R. Devaraj. Mr. YVS. Karthick AIR WALK PUBLICATIONS

Piping Systems and Flow Analysis (Chapter 3)

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

Pumping Stations Design For Infrastructure Master Program Engineering Faculty-IUG

CHAPTER 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES

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

SUMMER 14 EXAMINATION

Contents. 2 Basic Components Aerofoils Force Generation Performance Parameters xvii

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

CENTRIFUGAL PUMP SELECTION, SIZING, AND INTERPRETATION OF PERFORMANCE CURVES

ME 316: Thermofluids Laboratory

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

COMPUTER AIDED DESIGN OF RADIAL TIPPED CENTRIFUGAL BLOWERS AND FANS

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

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

ENGINEERING FLUID MECHANICS. CHAPTER 1 Properties of Fluids

Lesson 6 Review of fundamentals: Fluid flow

Detailed Outline, M E 320 Fluid Flow, Spring Semester 2015

Steven Burian Civil & Environmental Engineering September 25, 2013

Effect of Geometric Configuration on Performance of Uniflow Cyclone

Numerical Modelling of Twin-screw Pumps Based on Computational Fluid Dynamics

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

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

Pipe Flow. Lecture 17

3 Energy Exchange in Turbomachines

BASIC EQUATION. Rotational speed = = ABC 60

Chapter 4. Turbomachinery. 4.1 Introduction. 4.2 Pumps

Volume and Mass Flow Rate Measurement Author: John M. Cimbala, Penn State University Latest revision: 07 December 2007


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

BASIC EQUATION. Rotational speed. u = linear velocity in m/s r = radius in m ω = angular velocity in rad/s D = diameter in m N = rotation per minute

Centrifugal Machines Table of Contents

SUMMER-17 EXAMINATION Model Answer. Subject Title: Fluid Flow Operations subject code: page 1 of 27

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

by Dr. Shibayan Sarkar Department of Mechanical Engineering

ME332 FLUID MECHANICS LABORATORY (PART II)

ENT 254: Applied Thermodynamics

INTERNATIONAL JOURNAL OF ADVANCED RESEARCH IN ENGINEERING AND TECHNOLOGY (IJARET)

Analysis of flow characteristics of a cam rotor pump

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

Applied Thermodynamics for Marine Systems Prof. P. K. Das Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

COURSE NUMBER: ME 321 Fluid Mechanics I 3 credit hour. Basic Equations in fluid Dynamics

Compression and Expansion of Fluids

HVAC Clinic. Duct Design

B.E/B.Tech/M.E/M.Tech : Chemical Engineering Regulation: 2016 PG Specialisation : NA Sub. Code / Sub. Name : CH16304 FLUID MECHANICS Unit : I

COMPUTATIONAL FLOW ANALYSIS THROUGH A DOUBLE-SUCTION IMPELLER OF A CENTRIFUGAL PUMP

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

ON THE ONSET AND DEVELOPMENT OF ROTATING STALL WITHIN A VANED DIFFUSER OF A CENTRIFUGAL PUMP

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

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

CE 6403 APPLIED HYDRAULIC ENGINEERING UNIT - V PUMPS

1D AND 3D TOOLS TO DESIGN SUPERCRITICAL CO 2 RADIAL COMPRESSORS: A COMPARISON

Applied Fluid Mechanics

Flow analysis in centrifugal compressor vaneless diffusers

Applied Fluid Mechanics

Part A: 1 pts each, 10 pts total, no partial credit.

Introduction to Turbomachinery

Calculation of Power and Flow Capacity of Rotor / Stator Devices in VisiMix RSD Program.

RADIAL COMPRESSOR FAULT IDENTIFICATION USING DYNAMIC MEASUREMENT DATA. N. Aretakis, Research Assistant K.Mathioudakis, Assistant Professor

International Journal of Research in Advent Technology Available Online at:

Fluid Structural Analysis of Centrifugal FAN Using FEA

Transcription:

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. A diffuser is simply a gradual expansion in a pipe or duct. 1 2 d V 1 θ D V 2 A diffuser is a minor loss, and we can look up its minor loss coefficient K L in Table 8-4 and other places. [Note: Use the larger V (at smaller pipe section) to determine the minor loss.] Notice that K L decreases as d/d increases (D/d decreases) However, even after taking into account the minor loss (and its associated irreversible head loss or loss of pressure), it turns out that the pressure still rises (increases) through a diffuser!

The best conical diffuser (high pressure rise with minimal loss) has D/d 8 (area ratioof 8), included angle θ 4 o, and L/d 25. [White, F. M., 7 th ed., 2009, p. 408.] Drawn to scale, 1 2 d θ D L

Example: Diffuser Given: Water (ρ = 1000 kg/m 3, µ = 1.00 10-3 kg/m s) flows through a horizontal diffuser, as sketched. The flow is fully developed at both locations 1 and 2. The inner diameter changes from d to D through the diffuser. The outlet of the diffuser is open to atmospheric pressure. 2 1 10 o d V 1 10 o D V 2 Given information: d = 1.2 cm D = 2.0 cm θ = 2 10 o = 20 o (θ is the total included angle) V 1 = 6.0 m/s P 2 = P atm α 1 = 1.06 and α 2 = 1.06 (fully developed turbulent pipe flow) To do: Calculate the gage pressure at location 1 and discuss. Solution: To be done in class.

E. Turbomachinery (Chapter 14) 1. Introduction and terminology; types of pumps a. Positive displacement pumps b. Dynamic pumps Pump is a general term for any device that adds mechanical energy to a fluid. For liquids, we usually call them pumps. For gases, we usually call them fans, blowers, or compressors, depending on the relative pressure rise and volume flow rate. There are two basic types of pump: Positive displacement pumps (PDPs) fluid is sucked into a closed volume, and then the fluid is pushed out. Dynamic pumps no closed volume is involved; instead, rotating blades called impeller blades supply energy to the fluid. Positive Displacement Pumps: Your heart is a great example of a positive displacement pump (PDP). Blood is sucked into the right and left ventricles as they expand. The appropriate valves open and close as necessary. Blood is pushed out when the right and left ventricles contract. Again, the appropriate valves open and close to enable this. Engineers have designed artificial hearts that are also PDPs, and work in similar fashion:

In this design, compressed air is used to expand and contract a bladder to suck in and expel the blood in much the same way as a bellows. There are many other examples of positive displacement pump designs: Bicycle tire pump Oldfashioned water pump

Peristaltic pump Three-lobe Rotary pump Gear pump Double screw pump It is very simple to predict the volume flow rate of a PDP. Let s consider a simple twolobe rotary pump for illustration: Two-lobe rotary pump We define the volume of one lobe.

By analyzing the geometry as the two counter-rotating shafts turn, we see that for each have turn of the shafts (180 o ), this pump delivers two lobe volumes of fluid. For a given rotation rate n (rpm) of the pump shaft, we can easily calculate the volume flow rate, assuming no leakage through the small gaps. This is illustrated in the following example problem:

Dynamic Pumps: Dynamic pumps do not have closed volumes. Instead, spinning impeller blades or rotor blades transfer kinetic energy and impart momentum to the fluid. There are three main types of dynamic pumps: centrifugal flow, axial flow, and mixed flow: Centrifugal flow pump: Fluid enters axially and is discharged radially. Axial flow pump: Fluid enters axially and is discharged axially. Mixed flow pump: Fluid enters axially and is discharged at some angle between radial and axial.

Of these, centrifugal pumps are the most common, and are recognized by their scrolled (snail-like) casing. Some typical centrifugal air blowers with characteristic snail-shaped scrolls: Front and side views of a typical centrifugal pump with backward-inclined blades: It is more difficult to predict the volume flow rate induced by a dynamic pump since there are not closed volumes that are easily calculated. Instead, we must use the equations of conservation of mass and angular momentum to analyze the flow and the performance of the pump.