Heat transfer in Rotating Fluidized Beds in a Static Geometry: A CFD study



Similar documents
Chapter 5 Using Newton s Laws: Friction, Circular Motion, Drag Forces. Copyright 2009 Pearson Education, Inc.

VALIDATION, MODELING, AND SCALE-UP OF CHEMICAL LOOPING COMBUSTION WITH OXYGEN UNCOUPLING

Process Integration of Chemical Looping Combustion with Oxygen Uncoupling in a Coal-Fired Power Plant

Battery Thermal Management System Design Modeling

XI / PHYSICS FLUIDS IN MOTION 11/PA

Turbulence, Heat and Mass Transfer (THMT 09) Poiseuille flow of liquid methane in nanoscopic graphite channels by molecular dynamics simulation

HW Set VI page 1 of 9 PHYSICS 1401 (1) homework solutions

PHYSICS 111 HOMEWORK SOLUTION #10. April 8, 2013

Forces on the Rocket. Rocket Dynamics. Equation of Motion: F = Ma

Computational Fluid Dynamics (CFD) and Multiphase Flow Modelling. Associate Professor Britt M. Halvorsen (Dr. Ing) Amaranath S.

Turbine Design for Thermoacoustic

CFD SIMULATION OF SDHW STORAGE TANK WITH AND WITHOUT HEATER

1. Fluids Mechanics and Fluid Properties. 1.1 Objectives of this section. 1.2 Fluids

Lecture 6 - Boundary Conditions. Applied Computational Fluid Dynamics

AS COMPETITION PAPER 2008

Physics 2A, Sec B00: Mechanics -- Winter 2011 Instructor: B. Grinstein Final Exam

Computational Fluid Dynamic Modeling Applications

Use of OpenFoam in a CFD analysis of a finger type slug catcher. Dynaflow Conference 2011 January , Rotterdam, the Netherlands

Basic Principles in Microfluidics

Fluid Mechanics Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

The CFD simulation and an experimental study of hydrodynamic behaviour of liquid-solid flow

Wind Turbine Power Calculations

HW Set II page 1 of 9 PHYSICS 1401 (1) homework solutions

Lecture 14 - Multiphase Flows. Applied Computational Fluid Dynamics

C B A T 3 T 2 T What is the magnitude of the force T 1? A) 37.5 N B) 75.0 N C) 113 N D) 157 N E) 192 N

Overall pressure balance and system stability in a liquid solid circulating fluidized bed

AP Physics Circular Motion Practice Test B,B,B,A,D,D,C,B,D,B,E,E,E, m/s, 0.4 N, 1.5 m, 6.3m/s, m/s, 22.9 m/s

Journal bearings/sliding bearings

HEAT TRANSFER ANALYSIS IN A 3D SQUARE CHANNEL LAMINAR FLOW WITH USING BAFFLES 1 Vikram Bishnoi

AN EFFECT OF GRID QUALITY ON THE RESULTS OF NUMERICAL SIMULATIONS OF THE FLUID FLOW FIELD IN AN AGITATED VESSEL

Natural Convection. Buoyancy force

International Journal of TechnoChem Research. Eldho Abraham

Physics 1A Lecture 10C

Fluid Mechanics: Static s Kinematics Dynamics Fluid

Principles of Ion Implant

Lecture 24 - Surface tension, viscous flow, thermodynamics

Fluids and Solids: Fundamentals

THERMAL STRATIFICATION IN A HOT WATER TANK ESTABLISHED BY HEAT LOSS FROM THE TANK

CO MPa (abs) 20 C

TWO-DIMENSIONAL FINITE ELEMENT ANALYSIS OF FORCED CONVECTION FLOW AND HEAT TRANSFER IN A LAMINAR CHANNEL FLOW

Mixing in the process industry: Chemicals Food Pharmaceuticals Paper Polymers Minerals Environmental. Chemical Industry:

Turbulence Modeling in CFD Simulation of Intake Manifold for a 4 Cylinder Engine

du u U 0 U dy y b 0 b

Long term prediction of marble erosion for the conservation of the statue of David of Michelangelo

Relevance of Modern Optimization Methods in Turbo Machinery Applications

What is the most obvious difference between pipe flow and open channel flow????????????? (in terms of flow conditions and energy situation)

Chemical Looping with Oxygen Uncoupling with Coal

DEVELOPMENT OF HIGH SPEED RESPONSE LAMINAR FLOW METER FOR AIR CONDITIONING

F N A) 330 N 0.31 B) 310 N 0.33 C) 250 N 0.27 D) 290 N 0.30 E) 370 N 0.26

SHORT ANSWER. Write the word or phrase that best completes each statement or answers the question.

Modeling and Simulation of Complex Multiphase Flows in the Pharmaceutical Industry

GT ANALYSIS OF A MICROGASTURBINE FED BY NATURAL GAS AND SYNTHESIS GAS: MGT TEST BENCH AND COMBUSTOR CFD ANALYSIS

Numerical analysis of size reduction of municipal solid waste particles on the traveling grate of a waste-to-energy combustion chamber

PHYS 211 FINAL FALL 2004 Form A

CFD Grows Up! Martin W. Liddament Ventilation, Energy and Environmental Technology (VEETECH Ltd) What is Computational Fluid Dynamics?

Babcock & Wilcox's IR-CFB Boiler Technology. S. P. Ganeshan. Papertech -2010, Hyderabad. Divisional Manager, Thermax Limited, Boilers & Heaters Group

CE 204 FLUID MECHANICS

Introduction to Computational Fluid Dynamics (CFD) for Combustion. (801)

Center of Gravity. We touched on this briefly in chapter 7! x 2

Using Computational Fluid Dynamics (CFD) Simulation to Model Fluid Motion in Process Vessels on Fixed and Floating Platforms

INTERNATIONAL JOURNAL OF RESEARCH IN AERONAUTICAL AND MECHANICAL ENGINEERING

Exam 2 is at 7 pm tomorrow Conflict is at 5:15 pm in 151 Loomis

Differential Relations for Fluid Flow. Acceleration field of a fluid. The differential equation of mass conservation

Chapter 3.8 & 6 Solutions

Problem Statement In order to satisfy production and storage requirements, small and medium-scale industrial

Steady Flow: Laminar and Turbulent in an S-Bend

CFD Analysis of a butterfly valve in a compressible fluid

Chapter 9. particle is increased.

cmn_lecture.2 CAD OF DOUBLE PIPE HEAT EXCHANGERS

Practice Problems on Boundary Layers. Answer(s): D = 107 N D = 152 N. C. Wassgren, Purdue University Page 1 of 17 Last Updated: 2010 Nov 22

Flow Assurance & Operability


COMPUTATIONAL FLUID DYNAMICS (CFD) ANALYSIS OF INTERMEDIATE PRESSURE STEAM TURBINE

By K.K.Parthiban / Boiler specialist / Venus Energy Audit System

Flow characteristics of microchannel melts during injection molding of microstructure medical components

G U I D E T O A P P L I E D O R B I T A L M E C H A N I C S F O R K E R B A L S P A C E P R O G R A M

Joints Workshop Vibration and Turbomachinery

Dry Grinding of Technical Ceramics into the Submicron Range

A MTR FUEL ELEMENT FLOW DISTRIBUTION MEASUREMENT PRELIMINARY RESULTS

INVESTIGATION OF FALLING BALL VISCOMETRY AND ITS ACCURACY GROUP R1 Evelyn Chou, Julia Glaser, Bella Goyal, Sherri Wykosky

MODELING, SIMULATION AND DESIGN OF CONTROL CIRCUIT FOR FLEXIBLE ENERGY SYSTEM IN MATLAB&SIMULINK

Pushing the limits. Turbine simulation for next-generation turbochargers

Contents. Microfluidics - Jens Ducrée Physics: Fluid Dynamics 1

Steady Heat Conduction

Increase the efficiency of your rotating machines by optimizing your bearing lubrication

So if ω 0 increases 3-fold, the stopping angle increases 3 2 = 9-fold.

Laminar and Turbulent flow. Flow Sensors. Reynolds Number. Thermal flow Sensor. Flow and Flow rate. R = Mass Flow controllers

Supporting document to NORSOK Standard C-004, Edition 2, May 2013, Section 5.4 Hot air flow

NUMERICAL ANALYSIS OF THE EFFECTS OF WIND ON BUILDING STRUCTURES

If all three collisions below are totally inelastic, which one(s) will bring the car on the left to a complete halt?

A SILICON-BASED MICRO GAS TURBINE ENGINE FOR POWER GENERATION. Singapore Institute of Manufacturing Technology, Singapore

WJP, PHY381 (2015) Wabash Journal of Physics v4.3, p.1. Cloud Chamber. R.C. Dennis, Tuan Le, M.J. Madsen, and J. Brown

Model of a flow in intersecting microchannels. Denis Semyonov

Direct Conversion of Wind Energy into Heat Using Joule Machine

Sewage sludge treatment with oxygen enrichement and oxyfuel combustion in CFBC - new pilot plant results

Pumps: Convert mechanical energy (often developed from electrical source) into hydraulic energy (position, pressure and kinetic energy).

1. The Kinetic Theory of Matter states that all matter is composed of atoms and molecules that are in a constant state of constant random motion

Putting a chill on global warming

Transcription:

Heat transfer in Rotating Fluidized Beds in a Static Geometry: A CFD study Nicolas Staudt, Juray De Wilde* * Université catholique de Louvain MAPR / IMAP Réaumur, Place Sainte Barbe 2 1348 Louvain-la-Neuve Belgium juray.dewilde@uclouvain.be THE CONCEPT THEORETICAL INVESTIGATION COMPUTATIONAL FLUID DYNAMICS STUDY STEP RESPONSE TECHNIQUE CONVENTIONAL FLUIDIZED BED ROTATING FLUIDIZED BED IN A STATIC GEOMETRY CONCLUSIONS 1

THE CONCEPT FLUIDIZED BED PROCESS INTENSIFICATION IMPROVE EXTERNAL HEAT AND MASS TRANSFER (BETWEEN GAS & SOLIDS) IMPROVE INTERNAL MASS TRANSFER REDUCE GAS-SOLID CONTACT TIME INCREASE RATIO FREEBOARD SURFACE TO BED HEIGHT INCREASE MASS & HEAT TRANSFER COEFFICIENT FLUIDIZE SMALLER PARTICLES REDUCE BED HEIGHT & INCREASE GAS VELOCITY CYLINDRICAL GEOMETRY INCREASE GAS-SOLID SLIP VELOCITY FLUIDIZE IN A CENTRIFUGAL FIELD THE CONCEPT chimney outlet () solids outlet solids 2

THE CONCEPT 36-cm DIAMETER FLUIDIZATION CHAMBER 1G GELDART D HIGH GAS-SOLID SLIP VELOCITIES SHORT GAS-SOLID CONTACT TIMES 1G GELDART B 1G-GELDART D-TYPE: DENSE AND UNIFORM BED 1G-GELDART B-TYPE: SOMEWHAT LESS DENSE AND LESS UNIFORM BUBBLING BED BUBBLING SUPPRESSED AT HIGHER SOLIDS LOADINGS THE CONCEPT CRITERIA FOR STABLE AND UNIFORM OPERATION 2 1.8 Chimney: 1000 rpm, S = 3.56 10-2 kg/s 1.6 Solids loading [kg] 1.4 1.2 1 0.8 0.6 0.4 0.2 stable uniform rotating fluidized bed slugging channeling 0 600 650 700 750 800 850 1G Geldart D-type particles, 24-cm diameter fluidization chamber Gas flow rate [Nm3/h] (De Wilde & de Broqueville, 2007) 3

THE CONCEPT FLEXIBILITY IN THE FLUIDIZATION GAS FLOW RATE Force per cubic meter particle bed [N/m3] 80000 70000 60000 50000 40000 30000 20000 10000 1G-GELDART D-TYPE PARTICLES 24-cm DIAMETER FLUID. CHAMBER Average centrifugal force Average radial -solid drag force 0 650 700 750 800 850 900 Fluidization flow rate [Nm3/h] 6.5 7.0 7.5 8.0 8.5 Average radial (-solid slip) velocity [m/s] LIMITED RADIAL BED EXPANSION, EVEN RADIAL BED CONTRACTION 1600 GAS-SOLID HEAT TRANSFER COEFFICIENT THEORETICAL INVESTIGATION Gas-solid heat transfer coefficient [J/(m^2 s K)] 1400 1200 1000 800 600 400 200 hf: h gs radius at r = 0.12 m hf: h gs radius at r = 0.10 m hf: h gs radius at r = 0.07 m V = 0.01135 m 3 Solids loading = 11.35 kg h grav gs = 2 123 J /( m s K) 0 1500 2500 3500 4500 5500 6500 7500 8500 9500 Fluidization flow rate [m3/h] 4

GAS-SOLID HEAT TRANSFER ROTATING FLUIDIZED BED IN A STATIC GEOMETRY POTENTIAL: INCREASED SPECIFIC FLUIDIZATION GAS FLOW RATE (i.e. per unit volume particle bed), due to increased width / height -ratio INCREASED FLEXIBILITY IN THE FLUIDIZATION GAS FLOW RATE AND COOLING OR HEATING VIA THE FLUIDIZATION GAS, due to similar effect of the fluidization flow rate on centrifugal and -solid drag force INCREASED GAS-SOLID HEAT AND MASS TRANSFER COEFFICIENTS POSSIBLE, due to increased -solid slip velocity COMPUTATIONAL FLUID DYNAMICS STUDY RESPONSE OF PARTICLE BED TEMPERATURE TO STEP CHANGE IN THE FLUIDIZATION GAS TEMPERATURE FROM 300 K TO 400 K AT TIME t 0 Eulerian-Eulerian approach with Kinetic Theory of Granular Flow Particles: 700 µm, 2500 kg/m 3 Restitution coefficients : - Particle - particle: 0.95 - Particle - wall: 0.9 Specularity coefficient : 0.5 Solids loading : 33.75 kg/m length fluid. chamber COMPARISON CONVENTIONAL FLUIDIZED BED AND ROTATING FLUIDIZED BED IN A STATIC GEOMETRY 5

CONVENTIONAL FLUIDIZED BED SOLIDS VOLUME FRACTION 195 m 2 /h 540 m 2 /h 1080 m 2 /h FLUIDIZATION GAS FLOW RATE ROTATING FLUIDIZED BED IN A STATIC GEOMETRY SOLIDS VOLUME FRACTION 29800 m 2 /h 59600 m 2 /h FLUIDIZATION GAS FLOW RATE (HIGHER THAN WITH CONVENTIONAL FLUIDIZED BED) RADIAL BED EXPANSION LIMITED PARTICLE BED UNIFORMITY BETTER THAN WITH CONVENTIONAL FLUIDIZED BED 6

PARTICLE BED TEMPERATURE RESPONSE 400 390 Rotating fluidized bed in a static geometry Fluidization flow rate: Vitesse 59600 d'entrée m 3 / (h mdu length gaz fluid. : 39,4 chamber m/s) Vitesse 29800 d'entrée m 3 / (h mdu length gaz fluid. : 19,7 chamber m/s) Fluidization temperature Average particle bed temperature [K] 380 370 360 350 340 330 320 310 Conventional fluidized bed Fluidization flow rate: Vitesse 1080 msuperficielle 3 / (h m length du fluid. gaz chamber : 2 m/s ) Vitesse 540 m 3 superficielle / (h m length du fluid. gaz chamber : 1 ) m/s 300 0 1 2 3 4 5 6 7 8 9 10 11 Time [s] FASTER RESPONSE RFB-SG, DUE TO: INCREASED SPECIFIC FLUIDIZATION GAS FLOW RATE INCREASED GAS-SOLID HEAT TRANSFER COEFFICIENT PARTICLE BED TEMPERATURE UNIFORMITY t = 2 s t = 4 s t = 6 s t = 10 s Conventional fluidized bed Fluidization flow rate = 195 m 3 / (h m length fluid. chamber ) 7

PARTICLE BED TEMPERATURE UNIFORMITY t = 2 s t = 4 s t = 6 s t = 10 s Conventional fluidized bed Fluidization flow rate = 540 m 3 / (h m length fluid. chamber ) PARTICLE BED TEMPERATURE UNIFORMITY t = 2 s t = 4 s t = 6 s t = 10 s Conventional fluidized bed Fluidization flow rate = 1080 m 3 / (h m length fluid. chamber ) 8

PARTICLE BED TEMPERATURE UNIFORMITY t = 1 s t = 2 s t = 4 s t = 6 s Rotating fluidized bed in a static geometry Fluidization flow rate = 29800 m 3 / (h m length fluid. chamber ) PARTICLE BED TEMPERATURE UNIFORMITY t = 2 s t = 3 s Rotating fluidized bed in a static geometry Fluidization flow rate = 59600 m 3 / (h m length fluid. chamber ) IMPROVED PARTICLE BED TEMPERATURE UNIFORMITY, DUE TO TANGENTIAL FLUIDIZATION PARTICLE BED, i.e. THE PARTICLE BED ROTATIONAL MOTION 9

CONCLUSIONS CFD SIMULATIONS CONFIRM THAT ROTATING FLUIDIZED BEDS IN A STATIC GEOMETRY: Offer an increased specific fluidization flow rate Offer increased flexibility with respect to cooling or heating via the fluidization flow rate Offer the potential of -solid heat and mass transfer coefficients one to several orders of magnitude higher than in Conventional Fluidized Bed. Offer improved particle bed temperature uniformity due to excellent mixing resulting from the particle bed rotational motion PERSPECTIVES FOR USE OF ROTATING FLUIDIZED BEDS IN A STATIC GEOMETRY FOR FAST, HIGHLY ENDO- OR EXOTHERMIC REACTIONS OR FOR DRYING APPLICATIONS 10