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Spray 2

The document provides an overview of various characterization methods for spray drying nozzles, highlighting their importance in determining the quality of the final product. It details several techniques such as Phase Doppler Interferometry, Fraunhofer Diffraction, and Laser Sheet Imaging, along with their measurement characteristics and limitations. Additionally, it presents sample results from experiments conducted at En’Urga Inc. to demonstrate the effectiveness of these methods in analyzing spray patterns and drop sizes.

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0% found this document useful (0 votes)
21 views35 pages

Spray 2

The document provides an overview of various characterization methods for spray drying nozzles, highlighting their importance in determining the quality of the final product. It details several techniques such as Phase Doppler Interferometry, Fraunhofer Diffraction, and Laser Sheet Imaging, along with their measurement characteristics and limitations. Additionally, it presents sample results from experiments conducted at En’Urga Inc. to demonstrate the effectiveness of these methods in analyzing spray patterns and drop sizes.

Uploaded by

nooredinqadiri
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF, TXT or read online on Scribd
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Characterization Methods for Spray Drying Nozzles

An Overview

En’Urga Inc.
1201 Cumberland Avenue, West Lafayette, IN 47906

http://www.enurga.com
Motivation

 Spray drying used for producing


powder from a liquid or slurry
 Food, pharmaceuticals, consumer
products
 Can convert APIs from crystalline
to amorphous form for improved
bio-availability
 All spray dryers use some type of
nozzles
 Quality of nozzle determines the
final product quality
Outline

 Spray Characterization Methods


 Sample Results
 Spray characterization work at En’Urga Inc.
Spray Characterization Methods
Spray Characterization Methods

 Phase Doppler interferometry


 Fraunhofer diffraction
 Laser sheet imaging
 Extinction tomography
 Imaging velocimetry
 Holographic imaging
 Laser induced Fluorescence
 X-Ray visualization
Phase Doppler Interferometry

 Fringe pattern from


2 laser beams
 Particle scatters light
and projects pattern
 Detector at one
angle provides
velocity
 Multiple detectors
provide size
 Multiple setting
required for wide
dynamic range
Measurement Characteristics

Aerosol limitations Spherical, transparent/opaque


Distance to sample < 3m
Probe volume small
Size 1-500m
Number limitation Coincident, extinction
Sampling type Flux dependent
Measured quantities Velocity, size
Dynamic range 50
Sampling mode Time averaged, time resolved
Sensitivity highest large drops
Fraunhofer Diffraction
 Scattered intensity
from laser beam
 Fourier transform lens
for discrimination
 Array detectors
measures intensity at
different angles
 Mie scattering theory
for particle size
 Beam wandering a
problem in
evaporating fluids
Measurement Characteristics

Aerosol limitations None on shape/better if opaque


Distance to sample < 0.5 m
Probe volume Line of sight
Size 0.3-500 m
Number limitation Extinction, multiple scattering
Sampling type Concentration
Measured quantities Size
Dynamic range 100
Sampling mode Time averaged, time resolved
Sensitivity highest Middle range of drop sizes
Laser Sheet Imaging

 Laser sheet to illuminate spray


 Image taken using a CCD camera
at an oblique angle
 Intensity proportional to drop
surface area per unit volume

Potential Errors
 Laser extinction
 Signal attenuation
 Secondary emission
Measurement Characteristics

Aerosol limitations Spherical particles


Distance to sample < 0.5 m
Probe volume Planar, volume
Size 3-unlimited
Number limitation Extinction, image overlap
Sampling type Concentration dependent
Measured quantities Light intensity
Dynamic range 20
Sampling mode Instantaneous
Sensitivity highest Largest drops
Extinction Tomography (SETscan)

Spray
Array
detector
Laser

Laser sheet
Principle of Operation

 Path integrated extinction of laser sheets


 Multiple view angles for non-axisymmetric
turbulent flows
 Multiple slices to obtain high spatial resolution
 Local extinction coefficients obtained by statistical
tomography (MLE method)
 For liquid sprays, the local extinction coefficients is
equal to the drop surface areas per unit volume
Measurement Characteristics

Aerosol limitations Unrestricted


Distance to sample Unrestricted
Probe volume Planar
Size Unrestricted
Number limitation Extinction
Sampling type Concentration
Measured quantities Surface area * no. of drops/m3
Dynamic range Instrument SNR
Sampling mode Instantaneous, time averaged,
time resolved
Sensitivity highest Uniform across range
Imaging Velocimetry

 Two types available


 Planar Particle Imaging
Velocimetry and Statistical
Pattern Imaging Velocimetry
 First type tracks individual
particles and determines
displacement
 Second type tracks flow patterns
and determines peak spatial
correlations over a fixed time
window
Advantages and Disadvantages of SPIV
Advantages
 Does not require distinct particles
 Works with various types of lighting such as
shadowgraphy and natural lighting
 Work equally well with dense sprays
 High powered lasers not required
Disadvantages
 Bimodal velocity difficult to resolve
 Longer computational time required
 Minimum 10 KHz camera
Holographic Imaging

M – Mirror
L – Lens
BS – Beam splitter
 Scattered or shadow images mixed with a
reference beam
 Interference pattern on holographic film
 Image reconstructed to obtain particle size/shape
Planar Laser Induced Fluorescence
 Fuel, sometimes mixed with Dopant
 Excited with laser sheet
 Fluorescence observed with CCD array
 Intensity proportional to volume fraction
Potential Errors
Spray
Beam
expander  Laser extinction
Nd: YAG
laser
 Signal attenuation
Beam stop  Shot-to-shot variation
Cylindrical
lens Laser sheet

CCD
Camera
X-Ray visualization

X-Ray
source
X-Ray detector
array
Injector

 Ideal for dense sprays (light cannot penetrate)


 Used to obtain planar mass concentration
 Works with particles, gases, and liquids
Comparison of Methods

Measurement Characteristics Light Scattering Fraunhofer Light Sheet Imaging Extinction


Interferometry Diffraction, Ensem Tomography
Basic Measurement Diameter/Velocity Diameter Pattern Surface area
Accuracy +/- 20% +/- 20% Not quantitative +/- 2%
Particle Shape Restriction Spherical Sphere,Irregular Spherical none
Particle Composition Transparent, Opaque Better if opaque None none
Index of Refraction Dependence Yes Partial/none None None/Imaginary
Working distance (Trans to Det) 3 m 0.5 m 0.5m Unlimited
Sample Volume Small, Point Line of site Plane/volume Plane/volume
Sample Volume Bias Yes, Correction None Yes, Correction None
Size Minimum, mm 0.3 0.3 3 Unlimited
Maximum size 1,000 500 unlimited Unlimited
Number Density Maximum Coincid/extinction Extinction/MultiScat Extinction/overlap Extinction
Number Density Minimum None Yes, Low SNR Blank Images Low SNR
Sampling Type Flux Dependent Concentration Concentration N/A
Sampling Mode Time ave/ Instantaneous/ Instantaneous Time Ave, Time
Time Resolved Time Reolved Resolved, Instant
Size Dynamic Range 50 50 20 N/A
Particle Velocity Yes No Possible Possible
Number Density Measurements Yes Yes, With extinction Yes Yes
Measurement Sensitivity Highest for largest Highest for middle Highest for largest Uniform across range
Why surface area density

 Total amount of fuel or liquid evaporated is


proportional to heat release rate in combustion
and solid mass fraction in spray drying.
 Correlation coefficient (R) of different
parameters with total fuel evaporated
 Mass flux R = 0.903 Velocity R = -0.239
 Diameter = 0.681 Surface area density = 0.961

For combustion and spray drying applications, surface


area density is optimal method of comparing different
nozzles or checking uniformity
Sample Results
Sample Results (PDA)
16

40psi, 40gpm
14 40psi, 150gpm
70psi, 40gpm
70psi, 150gpm

V
12
70psi, 400gpm
100psi, 150gpm

Y-Velocity (m/s)
10 100psi, 400gpm

y 8

0
-50 -40 -30 -20 -10 0 10 20 30 40 50

Radial Position (mm)


Diameter vs. Radial Position (90 sweep)
6
100
70psi, 40gpm
70psi, 150gpm 90
4 70psi, 400gpm
80

70
2
X-Velocity (m/s)

Diameter (microns)
60

0 50

40

-2
30

20 100psi, 4.75% D.C


-4
100psi, 23% D.C
10
100psi, 73% D.C
0
-6
-50 -40 -30 -20 -10 0 10 20 30 40 50
-50 -40 -30 -20 -10 0 10 20 30 40 50
Radial Position (mm)
Radial Position (mm)
Sample Results (Malvern)

40 PSI, Malvern Data Test 4 40 g/min, D32


300 40 g/min, D43
40 g/min, D90
250 40 g/min, D10
Characteristic diameters, m

40 g/min, D50
40 g/min, D30
200 150 g/min, D32
150 g/min, D43
150 150 g/min, D90
150 g/min, D10
150 g/min, D50
100 150 g/min, D30
333 g/min, D32
50 333 g/min, D43  Single line data
333 g/min, D90  Two data
333 g/min, D10
0
333 g/min, D50
points at each
-2.0 -1.0 0.0 1.0 333g/min, D30 condition
Distance, inches
Sample Measurement (effect of vapor)
0 .2 5
D r o p s iz e d is t r ib u t io n n e g le c t in g f ir s t 4 r in g s
D r o p s iz e d is t r ib u t io n n e g le c t in g f ir s t 9 r in g s
0 .2 0

S M D c a s e 1 = 2 9 . 0 5 m ic r o n s
S M D c a s e 2 = 1 2 . 7 3 m ic r o n s
% volume in bin

0 .1 5

0 .1 0

0 .0 5

0 .0 0
0 20 0 400 600 800 1000
D r o p s iz e ( m ic r o n s )

 Effect of fuel vapor (beam wandering) is to cause spurious


readings of large drops
 Recommendation is to neglect reading of first 9 rings or all drops
larger than 150 microns
 Injector manufactures report case 2
Sample Results Patternator

 Struts signature
seen in drop
surface area map
 Hollow cone seen
as hollow
 Drip from nozzle
seen at the center
Sample Result: Agricultural Nozzle

 Ensemble average of drop surface area density


 High/low surface area indicates streaks/voids
Sample results from X-Ray

 Deconvoluted
 Deconvoluted results
results of mass
of mass fraction
fraction of water
of water
 Lower
 With SPIV, flow rate has
provides masshigher local concentration
flux within 5%
 High flow
 With patternator rate had
provides larger
drop size footprint
within 20%
SPIV shadowgraphy (penetration velocity)
70
Cond1 Injector # 86
Cond2
60
Cond3
Cond4
50 Cond5
Cond6
Distance (mm)

40

30

20

10

0
0.0 0.5 1.0 1.5 2.0 2.5 3.0
Time (ms)
Sample Results SPIV

GDI Injector at 20 MPa


PDA vs Patternator
Patternators Extinction 1/mm
Calculated Absorption Contour Plot 1/mm
0.03
10 10
0.02
0.025
5
5
0.015 0.02

Y (mm)
0
Y (cm)

0
0.01 0.015
-5
-5 0.01
0.005 -10
-10 0.005
-15
-15 -10 -5 0 5 10 15 -15 -10 -5 0 5 10
X (cm) X (mm)

Patternators Extinction 1/mmx 10-3


Calculated Absorption Contour Plot 1/mmx 10-3
7
20 20
5 6
10 10
4 5

Y (mm)
Y (cm)

0 0
3 4
-10
-10 2 3

-20 2
-20 1
-40 -20 0 20 40
-40 -20 0 20 40 X (mm)
X (cm)
Velocimeter vs PDA
Spray characterization at En’Urga Inc.
Current Spray Instruments

Optical patternator Large area patternator

X-Ray mass flow meter Pattern Imaging Velocimeter


Instruments under development
Planar drop sizer
SMD P= 50 PSI
20

10

Distance (mm)
0

-10

-20

-20 -10 0 10 20
Distance (mm)

Fluorescence tomography
120
Fluorescence Tomography
100 PDA measurement

P = 100 psi, X= 30 mm
80
Drop Size (m)

60

40

20

0
-20 -15 -10 -5 0 5 10 15 20
Radial Distance (mm)

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