An Introduction to Air Pollution

Size: px
Start display at page:

Download "An Introduction to Air Pollution"

Transcription

1 An Introduction to Air Pollution Chapter 6. Fabric filters 薛人瑋 Ph.D 2 nd October 2012

2 Fabric Filters Fabric filtration Air or combustion gases pass through a fabric Dust is trapped on the fabric Cleaned air exits the system Baghouses Rows of bags Inlet Exit Cleaning mechanism

3 Baghouse application and operation Baghouses- Compartmented: Shaker Reverse flow Noncompartmented: Pulse Jet Operation: Dirty air enters at low velocity Multiple filters (bags)collect PM PM falls to bottom Cleaned air exits

4 Advantages and disadvantages Advantages High efficiency for small particles Modular design Low velocity Low pressure drop Expense Large area Frequent cleaning/maintenance Operating temp limitations

5 Types of Baghouses Compartmented: Shaker baghouse Bags cleaned by oscillating framework Reverse air Clean air blown through bag is opposite direction Non-compartmented: Pulse jet Compressed air blown down bags for cleaning

6 Dust loading Fabric: filter material Woven fibers micron diameter Interstitial holes microns PM layer forms between fibrils Increased filtration efficiency Increased pressure drop S= filter drag V= filtering velocity

7 Theory Δ P Total pressure drop Δ P f Pressure drop due to the fabric Δ P p Pressure drop due to the particulate layer Δ P s Pressure drop due to the bag house structure

8 Darcy s equation ΔP f Pressure drop N/m 2 ΔP p Pressure drop N/m 2 D f D p μ V Depth of filter in the direction of flow (m) Depth of particulate layer in the direction of flow (m) Gas viscosity kg/m-s superficial filtering velocity m/min K f, K p Permeability (filter & particulate layer m 2 ) 60 Conversion factor δ/min V = Q/A Q volumetric gas flow rate m 3 /min A cloth area m 2

9 Dust Layer L Dust loading kg/m 3 t time of operation min ρ L Bulk density of the particulate layer kg/m 3 ΔP = ΔP f + ΔPp Filter Drag S = ΔP/V Areal dust density W = LVt S= k 1 +k 2 W

10 Permeability, K Permeability of filter material, (K 1 )( K e ) Extrapolated from test data Permeability of particulate layer, (K 2 )( K s ) Slope of test plot Determined from test data Fabric, dust Contributes to filter drag (S) as a function of areal dust density (W)

11 Filter drag model Filter drag: dependent on areal dust density (W) and fabric and dust layer permeability (K) S= filter drag, Pa-min/m or inches of water- min/ft W= areal dust density, kg/m 2 of fabric or lb/ft 2 of fabric L= dust loading, kg/m 3 or lb/ft 3 T= time of operation, minutes

12 Filter drag model Using the filter drag model to predict pressure drop (ΔP) after 60 min of operation Dust loading (L) = 15 g/m 3, V= 0.8 m/min Ke = 500 Pa-min/m, Ks= 3 Pa-min-m/g

13 Filter drag model Using the filter drag model to predict pressure drop (ΔP) after 60 min of operation Dust loading (L) = 15 g/m 3, V= 0.8 m/min Ke = 500 Pa-min/m, Ks= 3 Pa-min-m/g

14 Filter drag model Using the filter drag model to predict pressure drop (ΔP) after 60 min of operation

15 Dust Layer

16 DESIGN OF FABRIC FILTERS The equation for fabric filters is based on Darcy s law for flow through porous media. Fabric filtration can be represented by the following equation: S = K e + K s w Where, S = filter drag, N-min/m 3 S = P/V K e = extrapolated clean filter drag, N-min/m 3 K s = slope constant. Varies with the dust, gas and fabric, N-min/kg-m W= Areal dust density = L V t L = dust loading (g/m3), V = velocity (m/s) Both K e and K s are determined empirically from pilot tests.

17 Obtain Pilot Data to Determine ΔP versus loading

18 Problem Estimate the values of K e and K s for the filter drag model: Time (min) Filter P (Pa) Limestone dust loading L = 1.00 g/m 3 Fabric Area A = 1.00 m 2 Air flow rate Q = 0.80 m 3 /min

19 Solution Step 1: Calculate the air velocity Air velocity = 0.80 (m 3 /min)/1.00 m 2 = 0.80 m/min Step 2: S = P/V W = LVt Step 3: Determine K e and K s graphically K e = 470 N-min/m 3 K s = N-min/g-m

20 Reverse Air Fabric Filter

21 Example Problem

22 Solution

23 Solution

24 Pulse Jet Fabric Filter

25 Pulse jet design considerations Different filtering velocities No compartments Compressed air for bag cleaning Compressor power Pressure drop

26 Compressor power Major operating expense of pulse jet systems Compressor power (ω), kw: η = compressor efficiency γ = 1.4 (ratio of heat capacities C p /C v ) P 1, P 2 = initial and final pressures (abs), kpa Q 1 = volumetric flow rate at compressor inlet, m 3 /s

27 Compressor power Example: Find compressor power (ω), kw Flow rate (Q) = 20,000 cfm (9.5 m 3 /s) T = 50 C (323 K) P 1 = 1 atm (101.3 kpa) Air pulse (P 2 ) 100 psig (790 kpa) abs. Compressed/filtered air ratio = 0.6% Compressor efficiency (η)= 50%

28 Compressor power Compressor power (ω), kw: Flow rate (Q) = 20,000 cfm (9.5 m 3 /s) T = 50 C (323 K) Compressed/filtered air ratio = 0.6%

29 Compressor power Compressor power (ω), kw: Compressor efficiency (η)= 50% P 1 = 1 atm (101.3 kpa) Air pulse (P 2 ) 100 psig (790 kpa)

30 Fan Horsepower Flow rate (Q) = 20,000 cfm Assume 60% efficiency (η) for motor For ΔP = 17 inches w.g. BHP = 90 hp For ΔP = 3.4 inches w.g. BHP = 18 hp

31 Problem Calculate the number of bags required for an 8-compartment pulse-jet baghouse with the following process information and bag dimensions. Q, process gas exhaust rate 100,000 ft 3 /min A/C, gross air-to-cloth ratio 4 (ft 3 /min)/ft 2 Bag dimensions: bag diameter 6 in. bag height 12 ft

32 Solution

33 Solution

34 Solution

35 Solution

36 Shaker Baghouse

37 Hopper

38 Filtration time, t f Shaker and reverse-air baghouses Several compartments One compartment off-line for cleaning t f = filtration time, min N= number of compartments t r = run time, min t c = cleaning time, min

39 N=5, N-1=4 Filtration time, t f t f

40 Number of bags Example: Net cloth area = 8,000 ft 2 Select 3 (N) compartments N-1 = 2 (1 off-line for cleaning) 2 compartments on line to meet NCA Each compartment = 4,000 ft 2 4,000 ft 2 x 3 compartments = 12,000 ft 2 Bag size: 6 inch diameter, 8 feet long Bag area: πdh= π(0.5)(8)= 12.6 ft 2 12,000/12.6 = 952 bags

41 Filtering Velocity All (N) compartments on-line for Q = 20,000 cfm flow rate (Q N )through one compartment: N-1 compartments on line during cleaning flow rate through on-line compartments:

42 Filtering Velocity All (N) compartments on-line Filtering velocity (V N ) in one compartment (C): N-1 compartments on line during cleaning Design Filtering velocity (V N-1 ) in on-line compartments:

43 Pressure drop Max pressure drop (ΔP m ) occurs before next compartment to be cleaned (j) end of cleaning time for last compartment (j-1) at time t j (the time compartment j is on-line) t j t f

44 Pressure drop Calculating Max pressure drop (ΔPm) t f = 60 min, t c = 4 min, t r =? t f

45 Pressure drop Calculating Max pressure drop (ΔPm) During t j, the cloth in compartment j has accumulated areal dust density (W j ) Given dust loading (L) of 10gr/ft 3

46 Pressure drop Calculating Max pressure drop (ΔP m ) Given K e = 1.00 in wg-min/ft, K s = in wg-min-ft/gr During t j, the filter drag (S j ) in compartment j is

47 Pressure drop Calculating Max pressure drop (ΔPm) During t j, the actual filtering velocity (V j ) in compartment j is calculated Ratio of V j to V N-1 Total Number of Compartments, N f N = V j /V N

48 Pressure drop Calculating Max pressure drop (ΔPm) Finally, the maximun pressure drop can be calculated

49 A Compartment of Bags

50 Use Pilot Data to Design a Multicompartment Baghouse

51 Use Pilot Data to Design a Multicompartment Baghouse

FE Exam Fluids Review October 23, Important Concepts

FE Exam Fluids Review October 23, Important Concepts FE Exam Fluids Review October 3, 013 mportant Concepts Density, specific volume, specific weight, specific gravity (Water 1000 kg/m^3, Air 1. kg/m^3) Meaning & Symbols? Stress, Pressure, Viscosity; Meaning

More information

Cyclones. Vane Axial Cyclone 10/30/2013. EVE 402 Air Pollution Generation and Control. Chapter #5 Lectures (Part 4) A mechanical gas cleaning device

Cyclones. Vane Axial Cyclone 10/30/2013. EVE 402 Air Pollution Generation and Control. Chapter #5 Lectures (Part 4) A mechanical gas cleaning device EVE 402 Air Pollution Generation and Control Chapter #5 Lectures (Part 4) Cyclones A mechanical gas cleaning device Gas is spun (centrifugal force) to separate particles Two types Vane axial A ring of

More information

Effect of Air Density on Cyclone Performance and System Design

Effect of Air Density on Cyclone Performance and System Design Paper Number: 024216 An ASAE Meeting Presentation Effect of Air Density on Cyclone Performance and System Design Lingjuan Wang, Graduate Research Assistant Department of Biological and Agricultural Engineering

More information

PART II. Fluid Mechanics Pressure. Fluid Mechanics Pressure. Fluid Mechanics Specific Gravity. Some applications of fluid mechanics

PART II. Fluid Mechanics Pressure. Fluid Mechanics Pressure. Fluid Mechanics Specific Gravity. Some applications of fluid mechanics ART II Some applications of fluid mechanics Fluid Mechanics ressure ressure = F/A Units: Newton's per square meter, Nm -, kgm - s - The same unit is also known as a ascal, a, i.e. a = Nm - ) English units:

More information

Figure 1 Enlargement of Powdered Activated Carbon by microscope.

Figure 1 Enlargement of Powdered Activated Carbon by microscope. Introduction The following is a description of how the Powdered Activated Carbon (PAC) dosing system operates. Firstly an overview of how the Semi Dry Reactor and the purpose of carbon injection is described.

More information

Separations II: Solid-Gas Systems

Separations II: Solid-Gas Systems Micro- and Nanoparticle Technology Separations II: Solid-Gas Systems Dr. K. Wegner - Lecture 18.04.2018 18. April 2018 1. Introduction Removal of particles from a gas stream either for recovery or for

More information

C H A P T E R 5 ENVIRONMENTAL PROTECTION AGENCY. APTI 413: Control of Particulate Matter Emissions. Student Manual Chapter 5.

C H A P T E R 5 ENVIRONMENTAL PROTECTION AGENCY. APTI 413: Control of Particulate Matter Emissions. Student Manual Chapter 5. Chapter 5 C H A P T E R 5 ENVIRONMENTAL PROTECTION AGENCY APTI 413: Control of Particulate Matter Emissions Student Manual Chapter 5 C H A P T E R 5 A P T I : 4 1 3 C O N T R O L O F P A R T I C U L A

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

Chapter 9 Summary of Other Air Cleaners to Remove Particles

Chapter 9 Summary of Other Air Cleaners to Remove Particles Chapter 9 Summary of Other Air Cleaners to Remove Particles 9.2.3 Sampling Issues U = U 0 c = c 0 U = U 0 c = c 0 Q (a) isokinetic and isoaxial Q U = U 0 c = c 0 U < U 0 c > c 0 (b) subisokinetic and isoaxial

More information

Increase Productivity Using CFD Analysis

Increase Productivity Using CFD Analysis Increase Productivity Using CFD Analysis CFD of Process Engineering Plants for Performance Estimation and Redesign Vinod Taneja Vidhitech Solutions Abhishek Jain abhishek@zeusnumerix.com +91 9819009836

More information

EFFECT OF AIR DENSITY ON CYCLONE PERFORMANCE AND SYSTEM DESIGN

EFFECT OF AIR DENSITY ON CYCLONE PERFORMANCE AND SYSTEM DESIGN EFFECT OF AIR DENSITY ON CYCLONE PERFORMANCE AND SYSTEM DESIGN L. Wang, M. D. Buser, C. B. Parnell, B. W. Shaw ABSTRACT. 1D3D and 2D2D cyclones were tested at Amarillo, Texas, to evaluate the effect of

More information

2.0 KEY EQUATIONS. Evaporator Net Refrigeration Effect. Compressor Work. Net Condenser Effect

2.0 KEY EQUATIONS. Evaporator Net Refrigeration Effect. Compressor Work. Net Condenser Effect 2.0 KEY EQUATIONS Evaporator Net Refrigeration Effect Q net refrigeration effect [] = (H 1 H 4 ) lb (Refrig Flow Rate) (60) min lb min hr H 1 = leaving evaporator enthalpy lb ; H 4 = entering evaporator

More information

Computational Fluid Dynamic (CFD) Analysis of Gas and Liquid Flow Through a Modular Sample System

Computational Fluid Dynamic (CFD) Analysis of Gas and Liquid Flow Through a Modular Sample System Computational Fluid Dynamic (CFD) Analysis of Gas and Liquid Flow Through a Modular Sample System Tony Y. Bougebrayel, PE, PhD John J. Wawrowski Swagelok Solon, Ohio IFPAC 2003 Scottsdale, Az January 21-24,

More information

NEBB Fundamental Formulas

NEBB Fundamental Formulas Approved NEBB - May 1, 17 Page 1 of 8 Version 1.3 A = Area (ft²) IP, (m²) SI M = Mass (lb) IP, (kg) SI ACH = Air Changes per Hour ma = Mixed Air Ak = Effective Area m = meter (metre) AV = Average m³/s

More information

Water Pollution Control: Physical Methods. AWPPCE RPI Fall 2013

Water Pollution Control: Physical Methods. AWPPCE RPI Fall 2013 Water Pollution Control: Physical Methods AWPPCE RPI Fall 2013 Water Pollution Control Processes Water and Waste Water Treatment are usually carried out in specially designed vessels (reactors) under controlled

More information

Orifice and Venturi Pipe Flow Meters

Orifice and Venturi Pipe Flow Meters Orifice and Venturi Pipe Flow Meters For Liquid and Gas Flow by Harlan H. Bengtson, PhD, P.E. 1. Introduction Orifice and Venturi Pipe Flow Meters The flow rate of a fluid flowing in a pipe under pressure

More information

Section 1: Theory of Heat Unit 2: Matter and Energy

Section 1: Theory of Heat Unit 2: Matter and Energy Section 1: Theory of Heat Unit 2: Matter and Energy Unit Objectives After studying this chapter, you should be able to: define matter. list the three states in which matter is commonly found. define density.

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

Orifice and Venturi Pipe Flow Meters

Orifice and Venturi Pipe Flow Meters Orifice and Venturi Pipe Flow Meters by Harlan H. Bengtson, PhD, P.E. 1. Introduction Your Course Title Here The flow rate of a fluid flowing in a pipe under pressure is measured for a variety of applications,

More information

GAS/SOLID SEPARATIONS Cyclones, Electrostatic precipitators, (Hot) Gas filtration

GAS/SOLID SEPARATIONS Cyclones, Electrostatic precipitators, (Hot) Gas filtration 8 Fluid and Particulate systems 424521 /2018 GAS/SOLID SEPARATIONS Cyclones, Electrostatic precipitators, (Hot) Gas filtration Ron Zevenhoven ÅA Thermal and Flow Engineering ron.zevenhoven@abo.fi 8.1 Selection

More information

Optimization of DPF Structures with a 3D-Unit Cell Model

Optimization of DPF Structures with a 3D-Unit Cell Model Optimization of DPF Structures with a 3D-Unit Cell Model Wieland Beckert, Marcel Dannowski, Lisabeth Wagner, Jörg Adler, Lars Mammitzsch Fraunhofer IKTS, Dresden, Germany *Corresponding author: FhG IKTS,

More information

Northern Lesson 2 Gear Pump Terminology. Gear Pump 101. Lesson 2: Gear Pump Terminology. When your reputation depends on it!

Northern Lesson 2 Gear Pump Terminology. Gear Pump 101. Lesson 2: Gear Pump Terminology. When your reputation depends on it! Gear Pump 101 Lesson 2: Gear Pump Terminology When your reputation depends on it! Symbol Term Metric Unit Abbreviation US Customary Unit Abbreviation Conversion factor a A Area square millimeter mm2 square

More information

ME 201 Thermodynamics

ME 201 Thermodynamics ME 0 Thermodynamics Solutions First Law Practice Problems. Consider a balloon that has been blown up inside a building and has been allowed to come to equilibrium with the inside temperature of 5 C and

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

Chapter 5. Mass and Energy Analysis of Control Volumes

Chapter 5. Mass and Energy Analysis of Control Volumes Chapter 5 Mass and Energy Analysis of Control Volumes Conservation Principles for Control volumes The conservation of mass and the conservation of energy principles for open systems (or control volumes)

More information

SHORTCUT CALCULATIONS AND GRAPHICAL COMPRESSOR SELECTION PROCEDURES

SHORTCUT CALCULATIONS AND GRAPHICAL COMPRESSOR SELECTION PROCEDURES APPENDIX B SHORTCUT CALCULATIONS AND GRAPHICAL COMPRESSOR SELECTION PROCEDURES B.1 SELECTION GUIDE FOR ELLIOTT MULTISTAGE CENTRIFUGAL COMPRESSORS* * Reprinted from a 1994 Elliott Company sales bulletin.

More information

Lesson 37 Transmission Of Air In Air Conditioning Ducts

Lesson 37 Transmission Of Air In Air Conditioning Ducts Lesson 37 Transmission Of Air In Air Conditioning Ducts Version 1 ME, IIT Kharagpur 1 The specific objectives of this chapter are to: 1. Describe an Air Handling Unit (AHU) and its functions (Section 37.1).

More 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

Study of "Baffle Type Pre-separator Plus Cyclone" Abatement Systems for Cotton Gins

Study of Baffle Type Pre-separator Plus Cyclone Abatement Systems for Cotton Gins An ASAE/CSAE Meeting Presentation Paper Number: 044017 Study of "Baffle Type Pre-separator Plus Cyclone" Abatement Systems for Cotton Gins Lingjuan Wang, Ph.D., Postdoctoral Research Associate John D.

More information

Control of Primary Particulates

Control of Primary Particulates Control of Primary Particulates 1 Most of the fine particles in the atmosphere are secondary particles. Nonetheless, the control of primary particles is a major part of the air pollution control engineering.

More information

Separation Processes: Filtration

Separation Processes: Filtration Separation Processes: Filtration ChE 4M3 Kevin Dunn, 2014 kevin.dunn@mcmaster.ca http://learnche.mcmaster.ca/4m3 Overall revision number: 305 (September 2014) 1 Copyright, sharing, and attribution notice

More information

CHAPTER 1 Basic Considerations

CHAPTER 1 Basic Considerations CHAPTER Basic Considerations FE-type Exam Review Problems: Problems. to. Chapter / Basic Considerations. (C) m = F/a or kg = N/m/s = N s /m. (B) [μ] = [τ/(/dy)] = (F/L )/(L/T)/L = F. T/L. (A) 8 9.6 0 Pa

More information

HEAT CONTENT DECREASES U D R HEAT CONTENT INCREASESO. Btu/lb

HEAT CONTENT DECREASES U D R HEAT CONTENT INCREASESO. Btu/lb Pressure (psia) LINES OF CONSTANT ENTHALPY PRESSURE P R E S S U R E R I S E S P R E S S HEAT CONTENT DECREASES U R E D R HEAT CONTENT INCREASESO P S Btu/lb Heat Content Pressure (psia) SATURATION CURVE

More information

WORKBOOK FOR CHEMICAL REACTOR RELIEF SYSTEM SIZING ANNEX 10 NOMENCLATURE A cross-sectional flow area of relief system (m 2 ) A actual actual cross-sectional area of safety valve nozzle (m 2 ) A approx

More information

Recap: Introduction 12/1/2015. EVE 402 Air Pollution Generation and Control. Adsorption

Recap: Introduction 12/1/2015. EVE 402 Air Pollution Generation and Control. Adsorption EVE 402 Air Pollution Generation and Control Chapter #6 Lectures Adsorption Recap: Solubility: the extent of absorption into the bulk liquid after the gas has diffused through the interface An internal

More information

Problem 1.6 Make a guess at the order of magnitude of the mass (e.g., 0.01, 0.1, 1.0, 10, 100, or 1000 lbm or kg) of standard air that is in a room 10

Problem 1.6 Make a guess at the order of magnitude of the mass (e.g., 0.01, 0.1, 1.0, 10, 100, or 1000 lbm or kg) of standard air that is in a room 10 Problem 1.6 Make a guess at the order of magnitude of the mass (e.g., 0.01, 0.1, 1.0, 10, 100, or 1000 lbm or kg) of standard air that is in a room 10 ft by 10 ft by 8 ft, and then compute this mass in

More information

MAE 11. Homework 8: Solutions 11/30/2018

MAE 11. Homework 8: Solutions 11/30/2018 MAE 11 Homework 8: Solutions 11/30/2018 MAE 11 Fall 2018 HW #8 Due: Friday, November 30 (beginning of class at 12:00p) Requirements:: Include T s diagram for all cycles. Also include p v diagrams for Ch

More information

Piping Systems and Flow Analysis (Chapter 3)

Piping Systems and Flow Analysis (Chapter 3) Piping Systems and Flow Analysis (Chapter 3) 2 Learning Outcomes (Chapter 3) Losses in Piping Systems Major losses Minor losses Pipe Networks Pipes in series Pipes in parallel Manifolds and Distribution

More information

Modeling Formation and Bonding of Wood Composites

Modeling Formation and Bonding of Wood Composites Modeling Formation and Bonding of Wood Composites Chunping Dai FPInnovations Forintek Division Vancouver, Canada October, 2007 Empirical Approach vs Modeling Trial-and-Error Approach Advantages: - Simple

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

52nd North Carolina Industrial Ventilation Conference

52nd North Carolina Industrial Ventilation Conference System Design II Objectives Module Understand use of the ACGIH Calc sheet for system design. Become familiar with new design topics: Use of blast gates vs. balancing by design Balancing at a junction Air

More information

Calculation types: drained, undrained and fully coupled material behavior. Dr Francesca Ceccato

Calculation types: drained, undrained and fully coupled material behavior. Dr Francesca Ceccato Calculation types: drained, undrained and fully coupled material behavior Dr Francesca Ceccato Summary Introduction Applications: Piezocone penetration (CPTU) Submerged slope Conclusions Introduction Porous

More information

Research Article Performance of Single and Double Shaft Disk Separators

Research Article Performance of Single and Double Shaft Disk Separators Hindawi Publishing Corporation Physical Separation in Science and Engineering Volume 8, Article ID 58617, 5 pages doi:1.1155/8/58617 Research Article Performance of Single and Double Shaft Disk Separators

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

Fuel and Air Flow in the Cylinder

Fuel and Air Flow in the Cylinder Chapter 6 Fuel and Air Flow in the Cylinder 6.1) A four cylinder four stroke 3.0 L port-injected spark ignition engine is running at 00 rpm on a stoichiometric mix of octane and standard air at 100 kpa

More information

Technical Data Sheet DPT & DPIT-4005 SERIES DIFFERENTIAL PRESSURE TRANSDUCERS. Features. Description

Technical Data Sheet DPT & DPIT-4005 SERIES DIFFERENTIAL PRESSURE TRANSDUCERS. Features. Description Technical Data Sheet DPT & DPIT-4005 SERIES DIFFERENTIAL PRESSURE TRANSDUCERS Description The 4005 series of differential pressure transducers include Models DPT-4005 and DPIT-4005-M. The 4005 series differential

More information

THE ENERGY 68,SAVING TDVI. exible Combine Modular 24, 26, 28, 30, 32, 34, 36, 38, 40, 42, 44 HP 60, 62, 64, 66 HP

THE ENERGY 68,SAVING TDVI. exible Combine Modular 24, 26, 28, 30, 32, 34, 36, 38, 40, 42, 44 HP 60, 62, 64, 66 HP I N V E RT E R ion Range exible Combine Modular TDV I TDV I TDV I INVERTER INVERTER INVERTER 14, 16, 18, 20, 22 HP TDV I 24, 26, 28, 30, 32, 34, 36, 38, 40, 42, 44 HP INVERTER INVERTER INVERTER TDV I INVERTER

More information

Thermodynamics is the Science of Energy and Entropy

Thermodynamics is the Science of Energy and Entropy Definition of Thermodynamics: Thermodynamics is the Science of Energy and Entropy - Some definitions. - The zeroth law. - Properties of pure substances. - Ideal gas law. - Entropy and the second law. Some

More information

Pipe Flow/Friction Factor Calculations using Excel Spreadsheets

Pipe Flow/Friction Factor Calculations using Excel Spreadsheets Pipe Flow/Friction Factor Calculations using Excel Spreadsheets Harlan H. Bengtson, PE, PhD Emeritus Professor of Civil Engineering Southern Illinois University Edwardsville Table of Contents Introduction

More information

Civil aeroengines for subsonic cruise have convergent nozzles (page 83):

Civil aeroengines for subsonic cruise have convergent nozzles (page 83): 120 Civil aeroengines for subsonic cruise have convergent nozzles (page 83): Choked convergent nozzle must be sonic at the exit A N. Consequently, the pressure (p 19 ) at the nozzle exit will be above

More information

Aspects of Single Wafer Cleans Processing and Tools

Aspects of Single Wafer Cleans Processing and Tools Aspects of Single Wafer Cleans Processing and Tools Steven Verhaverbeke, Santa Clara, CA Date: June 16th, 2011 Contents 2 Generalities on Particles Generalities on particles in a chamber environment gas

More information

PARTICULATES #1. Introduction

PARTICULATES #1. Introduction Introduction PARTICULATES #1 Ash-forming elements in fuels Particulate emission standards Options for particulate control emissions Gravity settlers Gas cyclones Electrostatic precipitators see: www.hut.fi/~rzevenho/gasbook

More information

The First Law of Thermodynamics. By: Yidnekachew Messele

The First Law of Thermodynamics. By: Yidnekachew Messele The First Law of Thermodynamics By: Yidnekachew Messele It is the law that relates the various forms of energies for system of different types. It is simply the expression of the conservation of energy

More information

Wet Collectors. Type 1: Spray Chamber Scrubber 10/30/2013. EVE 402 Air Pollution Generation and Control. Chapter #5 Lectures (Part 5)

Wet Collectors. Type 1: Spray Chamber Scrubber 10/30/2013. EVE 402 Air Pollution Generation and Control. Chapter #5 Lectures (Part 5) EVE 40 Air Pollution eneration and Control Chapter #5 Lectures (Part 5) Wet Collectors Water is used to either capture particulate or increase aerosol size Hygroscopic particles (those that attract and

More information

Numerical Simulation of Turbulent Flow inside the Electrostatic Precipitator of a Power Plant

Numerical Simulation of Turbulent Flow inside the Electrostatic Precipitator of a Power Plant Numerical Simulation of Turbulent Flow inside the Electrostatic Precipitator of a Power Plant S.M.E. Haque 1*, M.G. Rasul 2, A. Deev 1, M.M.K. Khan 2 and J. Zhou 3 1 Process Engineering & Light Metals

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

Lecture 3: DESIGN CONSIDERATION OF DRIERS

Lecture 3: DESIGN CONSIDERATION OF DRIERS Lecture 3: DESIGN CONSIDERATION OF DRIERS 8. DESIGN OF DRYER Design of a rotary dryer only on the basis of fundamental principle is very difficult. Few of correlations that are available for design may

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

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

Section 4.1: Introduction to Jet Propulsion. MAE Propulsion Systems II

Section 4.1: Introduction to Jet Propulsion. MAE Propulsion Systems II Section 4.1: Introduction to Jet Propulsion Jet Propulsion Basics Squeeze Bang Blow Suck Credit: USAF Test Pilot School 2 Basic Types of Jet Engines Ramjet High Speed, Supersonic Propulsion, Passive Compression/Expansion

More information

In the next lecture...

In the next lecture... 16 1 In the next lecture... Solve problems from Entropy Carnot cycle Exergy Second law efficiency 2 Problem 1 A heat engine receives reversibly 420 kj/cycle of heat from a source at 327 o C and rejects

More information

Chapter 2 Dimensions, Units, and Unit Conversion

Chapter 2 Dimensions, Units, and Unit Conversion AE 205 Materials and Energy Balances Asst. Prof. Dr. Tippabust Eksangsri Chapter 2 Dimensions, Units, and Unit Conversion Dimensions Dimensions are concepts of measurement in engineering works. The basic

More information

Characteristics of standing disperse medium on the filter substrate

Characteristics of standing disperse medium on the filter substrate EPJ Web of Conferences 82, 01050 (2015) DOI: 10.1051/epjconf/20158201050 C Owned by the authors, published by EDP Sciences, 2015 Characteristics of standing disperse medium on the filter substrate Michail

More information

8.1 Technically Feasible Design of a Heat Exchanger

8.1 Technically Feasible Design of a Heat Exchanger 328 Technically Feasible Design Case Studies T 2 q 2 ρ 2 C p2 T F q ρ C p T q ρ C p T 2F q 2 ρ 2 C p2 Figure 3.5. Countercurrent double-pipe exchanger. 8. Technically Feasible Design of a Heat Exchanger

More information

DESIGN OF CYCLONE AND STUDY OF ITS PERFORMANCE PARAMETERS

DESIGN OF CYCLONE AND STUDY OF ITS PERFORMANCE PARAMETERS Research Paper ISSN 2278 0149 www.ijmerr.com Vol. 3, No. 4, October, 2014 2014 IJMERR. All Rights Reserved DESIGN OF CYCLONE AND STUDY OF ITS PERFORMANCE PARAMETERS Mahesh R Jadhav 1 * *Corresponding Author:

More information

CONCEPTS AND DEFINITIONS. Prepared by Engr. John Paul Timola

CONCEPTS AND DEFINITIONS. Prepared by Engr. John Paul Timola CONCEPTS AND DEFINITIONS Prepared by Engr. John Paul Timola ENGINEERING THERMODYNAMICS Science that involves design and analysis of devices and systems for energy conversion Deals with heat and work and

More information

Chapter Seven. For ideal gases, the ideal gas law provides a precise relationship between density and pressure:

Chapter Seven. For ideal gases, the ideal gas law provides a precise relationship between density and pressure: Chapter Seven Horizontal, steady-state flow of an ideal gas This case is presented for compressible gases, and their properties, especially density, vary appreciably with pressure. The conditions of the

More information

Chapter (6) Energy Equation and Its Applications

Chapter (6) Energy Equation and Its Applications Chapter (6) Energy Equation and Its Applications Bernoulli Equation Bernoulli equation is one of the most useful equations in fluid mechanics and hydraulics. And it s a statement of the principle of conservation

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

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

Outlines. simple relations of fluid dynamics Boundary layer analysis. Important for basic understanding of convection heat transfer

Outlines. simple relations of fluid dynamics Boundary layer analysis. Important for basic understanding of convection heat transfer Forced Convection Outlines To examine the methods of calculating convection heat transfer (particularly, the ways of predicting the value of convection heat transfer coefficient, h) Convection heat transfer

More information

Cyclone Click to go to the page. Cyclone

Cyclone Click to go to the page. Cyclone Cyclone.0311.2 Click to go to the page Cyclone The Cyclone (1,000-8,000 CFM) Suitable for collection of virtually any type of dust Applications: Heavy Moulding Grinding Planing Cabinet Shops Dust Transfer

More information

Impact of Weather House Design on REMP Air Sampler Results. Heather Baxter, Senior Scientist, Duke Energy

Impact of Weather House Design on REMP Air Sampler Results. Heather Baxter, Senior Scientist, Duke Energy Impact of Weather House Design on REMP Air Sampler Results Heather Baxter, Senior Scientist, Duke Energy Air Sampling Stations Originally, Harris Nuclear Plant had 6 air particulate/air iodine monitoring

More information

1.4 Perform the following unit conversions: (b) (c) s. g s. lb min. (d) (e) in. ft s. m 55 h. (f) ft s. km h. (g)

1.4 Perform the following unit conversions: (b) (c) s. g s. lb min. (d) (e) in. ft s. m 55 h. (f) ft s. km h. (g) 1.4 Perform the following unit conversions: 0.05 ft 1 in. (a) 1L 61in. 1L 1ft (b) 1kJ 650 J 10 J 1Btu 1.0551kJ 0.616 Btu (c) 41 Btu/h 0.15 kw 1kW 1h 600 s 778.17 ft lbf 1Btu ft lbf 99.596 s (d) g 78 s

More information

Thermodynamics of an Ideal Gas

Thermodynamics of an Ideal Gas Thermodynamics of an Ideal Gas A State Function Does not depend on how the system arrived at its present state; only on the characteristics of the present state. Volume, Pressure, Temperature, ΔE, ΔH State

More information

ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER. 20 June 2005

ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER. 20 June 2005 ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER 20 June 2005 Midterm Examination R. Culham & M. Bahrami This is a 90 minute, closed-book examination. You are permitted to use one 8.5 in. 11 in. crib

More information

Chapter 3 Permeability

Chapter 3 Permeability 3.2 Darcy s Law In 1856, Darcy investigated the flow of water through sand filters for water purification. His experimental apparatus is shown in Figure 3.11. By empirical observation Figure 3.11 Schematic

More information

Fluidisational velocity, resistance of permeable material layer

Fluidisational velocity, resistance of permeable material layer Fluidisational velocity, resistance of permeable material layer Fluidisation is a process whereby a granular material is converted from a static solidlike state to a dynamic fluid-like state. This process

More information

Only if handing in. Name: Student No.: Page 2 of 7

Only if handing in. Name: Student No.: Page 2 of 7 UNIVERSITY OF TORONTO FACULTY OF APPLIED SCIENCE AND ENGINEERING FINAL EXAMINATION, DECEMBER 10, 2014 2:00 PM 2.5 HOURS CHE 211F FLUID MECHANICS EXAMINER: PROFESSOR D.G. ALLEN ANSWER ALL SEVEN (7) QUESTIONS

More information

Course: MECH-341 Thermodynamics II Semester: Fall 2006

Course: MECH-341 Thermodynamics II Semester: Fall 2006 FINAL EXAM Date: Thursday, December 21, 2006, 9 am 12 am Examiner: Prof. E. Timofeev Associate Examiner: Prof. D. Frost READ CAREFULLY BEFORE YOU PROCEED: Course: MECH-341 Thermodynamics II Semester: Fall

More information

To receive full credit all work must be clearly provided. Please use units in all answers.

To receive full credit all work must be clearly provided. Please use units in all answers. Exam is Open Textbook, Open Class Notes, Computers can be used (Computer limited to class notes, lectures, homework, book material, calculator, conversion utilities, etc. No searching for similar problems

More information

Chapter 5: The First Law of Thermodynamics: Closed Systems

Chapter 5: The First Law of Thermodynamics: Closed Systems Chapter 5: The First Law of Thermodynamics: Closed Systems The first law of thermodynamics can be simply stated as follows: during an interaction between a system and its surroundings, the amount of energy

More information

Multiple Series Cyclones for Fine Dust

Multiple Series Cyclones for Fine Dust An ASAE Meeting Presentation Paper Number: 054014 Multiple Series Cyclones for Fine Dust D.P. Whitelock, Agricultural Engineer USDA-ARS Southwestern Cotton Ginning Research Laboratory, dwhitelo@nmsu.edu

More information

PREDICTING DPF PERFORMANCE BASED ON 3D MICROSCOPIC STRUCTURE FROM CT- SCAN

PREDICTING DPF PERFORMANCE BASED ON 3D MICROSCOPIC STRUCTURE FROM CT- SCAN 2016 CLEERS PREDICTING DPF PERFORMANCE BASED ON 3D MICROSCOPIC STRUCTURE FROM CT- SCAN Yujun Wang 1, Paul Folino 2, Carl J. Kamp 2, Rakesh K. Singh 1, Amin Saeid 1, Bachir Kharraja 1, Victor W. Wong 2

More information

CHAPTER 4 RESULTS AND DISCUSSION

CHAPTER 4 RESULTS AND DISCUSSION Chapter 4: RESULTS AND DISCUSSION 61 CHAPTER 4 RESULTS AND DISCUSSION 4.1 Exploratory Cooks Exploratory cooks were done in order to determine the relationship between the H-factor and kappa number relationship

More information

Sliding Bearings. Fig.(1) (a) Full-journal bearing and (b) partial-journal bearing

Sliding Bearings. Fig.(1) (a) Full-journal bearing and (b) partial-journal bearing Sliding Bearings The goal of a bearing is to provide relative positioning and rotational freedom while transmitting a load between two parts, commonly a shaft and its housing. The object of lubrication

More information

Chapter 7: External Forced Convection. Dr Ali Jawarneh Department of Mechanical Engineering Hashemite University

Chapter 7: External Forced Convection. Dr Ali Jawarneh Department of Mechanical Engineering Hashemite University Chapter 7: External Forced Convection Dr Ali Jawarneh Department of Mechanical Engineering Hashemite University Objectives When you finish studying this chapter, you should be able to: Distinguish between

More information

Reservoir Flow Properties Fundamentals COPYRIGHT. Introduction

Reservoir Flow Properties Fundamentals COPYRIGHT. Introduction Reservoir Flow Properties Fundamentals Why This Module is Important Introduction Fundamental understanding of the flow through rocks is extremely important to understand the behavior of the reservoir Permeability

More information

First Law of Thermodynamics

First Law of Thermodynamics CH2303 Chemical Engineering Thermodynamics I Unit II First Law of Thermodynamics Dr. M. Subramanian 07-July-2011 Associate Professor Department of Chemical Engineering Sri Sivasubramaniya Nadar College

More information

A amplitude. k stiffness m mass δ phase angle x 0 initial displacement v 0 initial velocity T period f frequency. A amplitude. ω angular frequency

A amplitude. k stiffness m mass δ phase angle x 0 initial displacement v 0 initial velocity T period f frequency. A amplitude. ω angular frequency EF 152 Final Exam, Fall, 2011 Page 1 of 10 EF 152 Final Exam, Fall, 2011 Page 2 of 10 The equation sheets may be removed when the test begins Guidelines: Assume 3 significant figures for all given numbers

More information

MEGASONIC CLEANING OF WAFERS IN ELECTROLYTE SOLUTIONS: POSSIBLE ROLE OF ELECTRO-ACOUSTIC AND CAVITATION EFFECTS. The University of Arizona, Tucson

MEGASONIC CLEANING OF WAFERS IN ELECTROLYTE SOLUTIONS: POSSIBLE ROLE OF ELECTRO-ACOUSTIC AND CAVITATION EFFECTS. The University of Arizona, Tucson MEGASONIC CLEANING OF WAFERS IN ELECTROLYTE SOLUTIONS: POSSIBLE ROLE OF ELECTRO-ACOUSTIC AND CAVITATION EFFECTS Manish Keswani 1, Srini Raghavan 1, Pierre Deymier 1 and Steven Verhaverbeke 2 1 The University

More information

c Dr. Md. Zahurul Haq (BUET) Thermodynamic Processes & Efficiency ME 6101 (2017) 2 / 25 T145 = Q + W cv + i h 2 = h (V2 1 V 2 2)

c Dr. Md. Zahurul Haq (BUET) Thermodynamic Processes & Efficiency ME 6101 (2017) 2 / 25 T145 = Q + W cv + i h 2 = h (V2 1 V 2 2) Thermodynamic Processes & Isentropic Efficiency Dr. Md. Zahurul Haq Professor Department of Mechanical Engineering Bangladesh University of Engineering & Technology (BUET Dhaka-1000, Bangladesh zahurul@me.buet.ac.bd

More information

Simulation of Soot Filtration on the Nano-, Micro- and Meso-scale

Simulation of Soot Filtration on the Nano-, Micro- and Meso-scale Simulation of Soot Filtration on the Nano-, Micro- and Meso-scale L. Cheng 1, S. Rief 1, A. Wiegmann 1, J. Adler 2, L. Mammitzsch 2 and U. Petasch 2 1 Fraunhofer-Institut Techno- und Wirtschaftsmathematik,

More information

Fuel Cell System Model: Auxiliary Components

Fuel Cell System Model: Auxiliary Components 2 Fuel Cell System Model: Auxiliary Components Models developed specifically for control studies have certain characteristics. Important characteristics such as dynamic (transient) effects are included

More information

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

FLOW IN PIPES. Mark J McCready University of Notre Dame July 24, chemeprof.com FLOW IN PIPES Mark J McCready University of Notre Dame July 24, 2017 OVERVIEW This lecture will provide the simplest framework to explain The three forces at that are important to fluid flow in pipes The

More information

M98-P2 (formerly C98-P1) Non-Newtonian Fluid Flow through Fabrics Matthew W. Dunn Philadelphia University

M98-P2 (formerly C98-P1) Non-Newtonian Fluid Flow through Fabrics Matthew W. Dunn Philadelphia University 1 Non-Newtonian Fluid Flow through Fabrics Matthew W. Dunn Philadelphia University http://spike.philacol.edu/perm/ Goal Statement The overall objectives of this program are to Model fabric porosity based

More information

PUMP SYSTEM ANALYSIS AND SIZING. BY JACQUES CHAURETTE p. eng.

PUMP SYSTEM ANALYSIS AND SIZING. BY JACQUES CHAURETTE p. eng. PUMP SYSTEM ANALYSIS AND SIZING BY JACQUES CHAURETTE p. eng. 5 th Edition February 2003 Published by Fluide Design Inc. www.fluidedesign.com Copyright 1994 I TABLE OF CONTENTS Introduction Symbols Chapter

More information

MCE380: Measurements and Instrumentation Lab

MCE380: Measurements and Instrumentation Lab MCE380: Measurements and Instrumentation Lab Chapter 8: Flow Measurements Topics: Basic Flow Equations Flow Obstruction Meters Positive Displacement Flowmeters Other Methods Holman, Ch. 7 Cleveland State

More information

20 m neon m propane. g 20. Problems with solutions:

20 m neon m propane. g 20. Problems with solutions: Problems with solutions:. A -m tank is filled with a gas at room temperature 0 C and pressure 00 Kpa. How much mass is there if the gas is a) Air b) Neon, or c) Propane? Given: T7K; P00KPa; M air 9; M

More information

Atmospheric pressure. 9 ft. 6 ft

Atmospheric pressure. 9 ft. 6 ft Name CEE 4 Final Exam, Aut 00; Answer all questions; 145 points total. Some information that might be helpful is provided below. A Moody diagram is printed on the last page. For water at 0 o C (68 o F):

More information