magnetic particle tracking in spouting and bubbling fluidized beds jack halow separation design...

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Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented at the 2012 Fall National Meeting of the American Institute of Chemical Engineers October 16-21, 2011 Pittsburgh, Pennsylvania

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Page 1: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Magnetic Particle Tracking in Spoutingand Bubbling Fluidized Beds

Jack Halow

Separation Design Group

Stuart Daw

Oak Ridge National Laboratory

Presented at the 2012 Fall National Meeting of the American Institute of Chemical Engineers

October 16-21, 2011

Pittsburgh, Pennsylvania

Page 2: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Objectives

Develop and demonstrate a unique experimental magnetic particle tracking system (MPTS) for studying solids mixing and dynamics in fluidized beds

Apply MPTS to develop statistically significant measures that characterize fluidized solids behavior

Develop correlations to develop fast running models of fluidized bed processes

Acquire data sets that can be used for validation of first principles and two phases and process models.

Page 3: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

The magnetic particle tracking system

Tracer particles are constructed over a tiny neodymium magnet core

Magnet is Imbedded in a bead, foamed or coated

Tracer particles used are >1 mm diameter, 0.4-7 g/cc

•Single tracer particles are injected into bed

•Magnetic field signals recorded for analysis

•Special algorithms deconvolute signals to give 3D trajectory data

Page 4: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Four inch bed with current MPTS setup

Probes aligned North, South, East, West

Helmholtz coils modify earth’s magnetic field in bed

Non-metallic bed and supports

Page 5: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

MTPS Current Capabilities

Beds up to 10 cm in diameter

Sampling rates up to 200 hertz

Runs times to 10 minutes

Sensitivity <0.5 milligauss equivalent to ~20 cm

Temperatures to 200-300 Centigrade possible

Applications to fluid beds, granular flow or fluid flow system

Tracer sizes > ~ 1 mm and densities > 0.4 g/cc

Trade off sometimes required between parameters

Page 6: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Information we get from MPTS 3D trajectory data

– Visualize tracer motion Position versus time graphs (i.e. Z or R vs time) Short time 3D vector plots: particular types of events 2D projections

– Visualize average location “Dot cloud” plots of data

– 3D clouds or 2D slices

– Quantify spatial information Frequency distributions Fit to statistical models for use in process model

– Quantify temporal information Autocorrelation analysis to yield characteristic times FFT for highly periodic processes

Page 7: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Experiments I’ll discuss

• Test conditions- 5.5 cm diameter bed- Porous plate distributor- 175 to 250 micron glass beads- 2.5 Umf (~15 cm/sec)- Slumped bed L/D =1- 0.76 g/cc 4 mm tracer- Sampling rate was 100 Hertz- Run time was 5 minutes- 5 replicate tests performed

• Data representations and analysis

Page 8: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Vertical position vs time – 30 sec

Page 9: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

3D views of three tests “Dot clouds” give average temporal representations

But replicates not directly comparable

Top View

Side View

Page 10: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Statistical comparisons are better

Direct one to one comparisons not viable– Overall conditions same but detailed dynamics

depend on detailed local initial conditions which are never identical

Spatial statistical comparison– Compare frequency distributions - probability of

spatial location

Temporal statistical comparison– Compare autocorrelation curves at various time

lags - characteristic cycle times

Page 11: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Spatial comparison: frequency plots Divide vertical height into 40 bins

Place each measured z into a bin and count up each bin

Calculate normalized frequency for each bin

Page 12: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Length of test is important

• Compares full tests and segments of a test• Agreement deteriorates

with shorter times•Need adequate run times

to characterize bed

300 sec

25 sec50 sec

Page 13: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Temporal comparison Autocorrelation function

– Compares times series to itself as it’s shifted in time

– Periodicity shows up as peaks in the correlation coefficient

~0.8 sec cycle time

Page 14: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Radial position at various levels

• Dots in ring at higher bed levels• Concentrated in center lower in bed

Page 15: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Radial Frequency Distributions

• For each of the six levels:• Radial position sorted into 7 even radius bins• Points counted and normalized for each bin

Page 16: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Radial position autocorrelation

• Doesn’t show significant correlation• Radial motion essentially random• Bubble position radially random

Page 17: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Velocities show bubble events• 5 second segment• X & Y spikes indicate rapid lateral motion from bubbles•X & Y motion coupled with vertical motion

Page 18: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Total velocity frequency distribution

•Weibull distribution gives excellent fit (CC=0.98)

Page 19: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Summary Magnetic particle tracking can provide highly detailed

information about the motion of single particles (> 1mm) in fluidized beds.

Direct trajectory comparisons give qualitative information

Statistical comparisons are quantitative

Spatial frequency distributions give time averaged locations: Weibull distribution can represent vertical positions

Temporal analysis such as autocorrelation can reveal average circulation times and perhaps regime transitions

Model validations should use statistical data

Model calculations must run for minutes to be meaningful

Page 20: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Publications

E. Patterson, J. Halow, and S. Daw, “Innovative Method Using Magnetic Particle Tracking to Measure Solids Circulation in a Spouted Fluidized Bed,” Ind. Eng. Chem. Res. 2010, 49, 5037–5043.

J. Halow, K Holsopple, B. Crawshaw, S. Daw, “Observed Mixing Behavior of Single Particles in a Bubbling Fluidized Bed of Higher-Density Particles,” Ind. Eng. Chem. Res. on-line just accepted, October 10, 2012

Presentations J. Halow, E. Patterson, S. Daw, 2009 Annual AIChE Mtg. Nashville, TN

J. Halow, B Crawshaw, S Daw, C. Finney, 2011 Annual AIChE Mtg. Minneapolis, MN

E. Patterson, 237th ACS National Mtg, Salt Lake City, March, 2009.

Holsopple, 239th ACS National Mtg, San Francisco, March, 2010

Page 21: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Contact

Jack Halow– [email protected]

– Phone: 724-966-9589

Page 22: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Background Slides

Page 23: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

MPTS – What is it? Tracer

– Small Neodynium magnet imbedded in particle– Tracer aligns with earth magnetic field orienting is magnetic field– Tracer density can be adjusted by choice of tracer material– Tracers diameters are 1 mm or larger– Tracer densities of from 0.4 to 7 g/cc

Sensors– Magneto-resistive type or Hall-effect– Externally mounted around bed– Orientation important for data analysis

Analysis– Special algorithms used to extract trajectory from field data– Data presentation by graphic and statistical techniques

Page 24: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Background and Motivation: Many processes utilize fluidized bed contactors and reactors

Turbulent multi-phase flow

High heat and mass transfer

Mixing of particles with gas, other particles key to performance

Different size and density of particles can lead to segregation

Dynamics of non-normal particles not well understood

Easy, safe inexpensive particle tracking system likely to have applications in many flow systems.

Page 25: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Vertical Position Probability Correlated with Weibull Distribution

kzk

ezk

zf

/

1

)(

for Z ≥ 0

k>0 is a shape factorλ>0 is a scale factor

Page 26: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Weibull Parameters Vary with Velocity and Tracer Density

•Weibul distribution represents data analytically•Useful for process modeling

Page 27: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Vertical position vs time – full test

Shows vertical motion

But Replicate tests not comparible

Page 28: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Radial position of tracer

•All points shown•Slight off center •Not much at walls

Page 29: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Radial Position Versus HeightSide view

Page 30: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Test Procedure

Bed and probes are leveled

Probes aligned probe NSEW

Bed material added and fluidized

Probe level adjusted to fluidized bed height

Probes zeroed

Data acquisition started.

Tracer dropped into bed

Page 31: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Temporal comparison - velocities• Tests with 0.76 g/cc traced• Velocity varied from just bubbling to turbulent• Characteristic circulation times evident

Page 32: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Autocorrelation of 1.2 g/cc tracer

Page 33: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Weibull Distribution with 0.76 g/cc Tracer

Page 34: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Weibull Distribution with 0.89 Tracer

Page 35: Magnetic Particle Tracking in Spouting and Bubbling Fluidized Beds Jack Halow Separation Design Group Stuart Daw Oak Ridge National Laboratory Presented

Weibull Distribution with 1.20 Tracer