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Method Development for Laser Diffraction

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Generating reliable, accurate particle size data is dependent upon the quality of the method. This presentation shows how HORIBA develops methods for laser diffraction particle size analyzers. This information will be useful for any laser diffraction analyzer and specifically the LA-950 Particle Size Analyzer. Ian Treviranus, from HORIBA Scientific, covers the following topics: Overview of sampling & dispersions Effect of ultrasound & air pressure Case studies Making life easy with the Method Expert ISO recommendations
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© 2013 HORIBA, Ltd. All rights reserved. Method Development Ian Treviranus [email protected] www.horiba.com/us/particle
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Page 1: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Method Development

Ian [email protected]/us/particle

Page 2: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

What we’ll talk about

Accuracy, precision, resolution

Setting goals, ISO/USP input

Wet method development

Dry method development

Q&A

Page 3: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Starting point

Instrument is fully functionalSuitable sample for technology

Counters are classic example

Stay current with free webinarsParticle size essentials,

method development, sampling & dispersion advice, DLS and zeta potential technology reviews

Page 4: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

General concerns

Data correlation (larger topic, def. doable!)

Reliable results (accuracy? precision?)Generating real resultsValidating methodsEffect of ultrasound/air

pressure on resultsDispersing powders

(webinar TR005, TR016)

Validating data (webinar TR004)

Page 5: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Featured technologies

LA-950Laser Diffraction

SZ-100Dynamic Light Scattering & Zeta Potential

CAMSIZER & CAMSIZER XTDynamic Image Analysis

PSA300Static Image Analysis

SA-9600Flowing Gas BET Surface Area

Page 6: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

LA-950: Laser Diffraction

Particle size performance leaderNinth generationUltra durableLowest total cost of ownershipSuspension, emulsion, powder,

paste, gel10 nanometer – 3 mm

Page 7: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Dynamic Range 0.01 – 3000 µmWidest wet measurement rangeOnly system to measure 30 nm!

30 nm silica 40 nm latex

Page 8: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Goal: Reproducible method that tracks product performance Choose measurement approach (dry vs. suspension) Lock down RI Vary measurement settings that can influence result

Dry: measurement duration, concentration, air pressureWet: sampler selection, dispersion, duration, concentration, energy

(mixing + ultrasound)

Test method (reproducibility)Meet ISO, USP or internal guidelinesCheck COV at d10, d50, d90

Section Overview

Page 9: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Reproducible method that tracks product performance You might have other goals

Accuracy: tricky subject, is it the “real” particle size?Repeatability: liquid suspension re-circulating in samplerReproducibility: prepare, measure, empty, repeatResolution: optimize to find second populationsMatch historic data (sieves), but quicker, easier technique

Use structured approach for any decision/choice that may influence result

Have data to support selections made Document process so colleagues understand your choices

Goals for any Method

Page 10: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

(A) Low accuracy, low precision measurements form a diffuse, off-center cluster; (B) Low accuracy, high precision measurements form a tight off-center cluster; (C) High accuracy, low precision measurements form a cluster that is evenly distributed but distant from the center of the target; (D) High Accuracy, high precision measurements are clustered in the center of the target.

LOW ACCURACYLOW PRECISION LOW ACCURACY

HIGH PRECISION HIGH ACCURACYLOW PRECISION HIGH ACCURACY

HIGH PRECISION

Accuracy vs. Precision

Page 11: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Is it the “real particle size”?Comparison to referee techniqueMicroscope (image analysis) is referee

technique for particle characterizationTwo kinds of image analysis:

Dynamic image analysis; particles flowingStatic image analysis; particles sit on slide

on automated stage

Accuracy

Page 12: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Dynamic:particles flow past camera

Static:particles fixed on slide,stage moves slide

Image Analysis to Verify

Page 13: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Scheme for outlining particle evaluation for preclinical studies.

Decision tree outlining particle evaluation for Phase I clinical studies

Proposed Guidelines

Page 14: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Scheme for outlining particle evaluation for Phase III clinical studies

Proposed Guidelines

Page 15: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

RepeatabilityPrepare sample, add to wet sampler, re-

circulate, measure same multiple times (suspensions only)

Provides limited information

ReproducibilityPrepare sample, measure, drain, repeat

(suspensions + dry)Distinguishes great methods

Types of Precision

Page 16: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

24 Samplings of Polystyrene Latex

-5

0

5

10

15

20

25

30

0.11

40.

15

0.19

70.

258

0.33

90.

445

0.58

30.

765

1.00

41.

318

1.72

92.

268

2.97

63.

904

5.12

26.

719

8.81

5

Size (microns)

Frequency

%

Repeatability

Page 17: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Reproducibility: prepare, measure, empty, repeat What would be good reproducibility?

Look at accepted standardsMeasure 3 times, calculated COV at d10, d50, d90

– COV (RSD) = st dev/mean * 100

ISO13320

– COV < 3% at median d50

– COV < 5% at d10 & d 90

USP<429>

– COV < 10% at median d 50

– COV < 15% at d10 & d 90

Note: double all limitsWhen d10, d50, or d90 < 10 m

Reproducibility

Page 18: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Ability to measure small differences in particle size

Small differences between successive samples (different production lots) are most important

Detection limit of small amount of material outside of main size distribution

Best defined by user’s real-world requirements

Resolution

Page 19: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Resolve size difference between two materials of similar size

552nm and 600nm PSL Measured separately:

high resolution Measure together: low

resolution, would blend peaks

Laser diffraction is a “resolution limited” technique

Is this High or Low Resolution?

Page 20: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Resolution of multiple modes in a single sample

Next peak 2x of previous size

83nm, 204nm, 503nm PSL

Resolution: Multi-modal

Page 21: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Next peak 2x of previous size

Resolution is independent of where you are on size scale

100µm,

200µm,

400µm glass beads

Resolution: Multi-modal

Page 22: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

0.1 micron silica material

2% by weight of ~1 micron quartz standard added

Original slide showed .25%

Resolution: Outlier Populations

Page 23: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Median Size : 0.031 μm

Median Size : 1.65 μm

Median (Peak 1) : 0.031 μmMedian (Peak 2) : 1.75 μm

Top left: LUDOXTM-50 PSD,Lower left: 0.1wt% Geltech 1.5 PSDTop right: 0.05wt% Geltech 1.5 in LUDOX Result shows both oversize particle detection & very good accuracy for both components.

*See AN179 CMP SLURRY MEASUREMENT USING LASER DIFFRACTION

0.05wt%

Resolution: Outlier Example

Page 24: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Wet Method Development

Page 25: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

First determine RI Choose solvent (water, surfactants, hexane, etc.) Sampler selection: sample volume Pump & stirrer settings Concentration Measurement duration Does the sample need ultrasound?

Document size-time plotDisperse sample, but don’t break particlesCheck for reproducibility

Wet Method Workflow

Page 26: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Real component via literature or web search, Becke line, etc. Measure sample, vary imaginary component to see if/how

results change Recalculate using different imaginary components, choose

value that minimizes R parameter error calculation

Determine Refractive Index

Page 27: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

LA-950 Method Expert

Page 28: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Larger, broad distributions require larger sample volume

Lower volume samplers for precious materials or solvents

LA-950 Sample Handlers

Dispersing Volume (mL)

Aqua/SolvoFlow 180 - 330

MiniFlow 35 - 50

Fraction Cell 15

Small Volume Fraction Cell

10

Median (D50): 35 nm

Sample Amount: 132 mg

Median (D50): 114 µm

Sample Amount: 1.29 mg

Median (D50): 9.33 µm

Sample Amount: 0.165 mg

Note: FractionCell has only magnetic stir bar, not for large or heavy particles

Bio polymer Colloidal silica Magnesium stearate

Sampler Selection

Page 29: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Must be high enough to suspend & circulate heavy particles

Not so high that bubbles are introduced

Adding energy – can disperse loose agglomerates

Measure at several settings & select optimum

Can be automated in software (see right)

Exp # Agitation Circulation Dmean (nm) D10 (nm) D90 (nm)

1 1 1 187.03 137.5 245.7

2 1 3 184.23 135.9 242.1

3 3 1 187.28 137.8 245.8

4 3 3 184.61 136.1 242.5

5 1 1 185.32 136.3 243.7

6 1 3 184.04 135.8 241.8

7 3 1 184.13 135.8 241.9

8 3 3 184.98 136.4 242.9

Parameters Selected: Agitation: 2 Circulation: 2

Pump & Stirrer

Page 30: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

High enough for good S/N ratio Low enough to avoid multiple

scattering Typically 95 – 80 %T Measure at different T%, look at

Chi Square calculation

d50

Chi2

Concentration

Page 31: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Long enough for reproducibility

Typically 5 sec, up to several minutes

Longer time for large, broad distributions

Can be automated in software

Could be used for robustness testing during method validation

Measurement Duration

Page 32: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Adding energy to break up agglomerates – disperse to primary particles, without breaking particles

Similar to changing air pressure on dry powder feeder Typically set to 100% energy, vary time (sec) on Investigate tails of distribution

High end to see if agglomerates removedSmall end to see if new, smaller particles appear (breakage)

Test reproducibility, consider robustness Note:

Do not use on emulsionsCan cause thermal mixing trouble w/solvents - waitUse external probe if t> 2-5 minutes

Ultrasonic Dispersion

Page 33: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Level (power)Time onIterationsDelayGenerate result

graphs

LA-950 Method Expert

Page 34: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Wet Method Development

Case Study

Microcrystalline Cellulose

Page 35: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Effect of Ultrasound: MCC

Page 36: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

0

20

40

60

80

100

120

140

160

180

1 2 3 4 5 6 7 8 9 10 11 12 13

0 sec

5 sec

10 sec15 sec

20 sec40 sec

60 sec

Siz

e (

m)

Ultrasound (sec)

D90D50D10

Effect of Ultrasound: MCC

Page 37: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

ISO13320

– COV < 3% at median d50

– COV < 5% at d10 & d 90

USP<429>

– COV < 10% at median d 50

– COV < 15% at d10 & d 90

Reproducibility Test at 15 sec

Page 38: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

From LA-950 Software

Precision Test Automation

Page 39: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

58 methods Image analysis for

morphology Laser diffraction for PSD If RSD for d50 < 20%,

then acceptable for QC environment

Note: RSD increases with decreasing size

*Barber, Keuter, and Kravig, A Logical Stepwise Approach to Laser Diffraction Particle Size Distribution Analysis Methods Development and Validation Pharmaceutical Development and Technology, 3(2), 153-161 (1998)

Acceptable

Not acceptable per USP<429>

Reproducibility

Page 40: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

*Barber, Keuter, and Kravig, A Logical Stepwise Approach to Laser Diffraction Particle Size Distribution Analysis Methods Development and Validation Pharmaceutical Development and Technology, 3(2), 153-161 (1998)

Acceptable

Not acceptable

Remove points from not acceptable region using Fraction Cell

Sampler Selection

Page 41: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Dry Method Development

Page 42: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

First get sampling right & determine RI Measure at 3 different pressures (low, medium, high) Determine optimum pressure based on good

dispersion while not breaking particles Can also compare dry vs. wet measurements Adjust other settings to optimize sample

concentration & duration Ideally measure all of powder placed into the sampler

Segregation can occur on vibrating trayConstant mass flow rate important for stable concentration

during measurement

Once settings chosen, test reproducibility

Dry Method Workflow

Page 43: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Siz

e

Increasing energy

Stability

Theoretical Actual

Siz

e

Increasing energy

Higher air pressure or longer ultrasound duration

Dispersion vs. Breakage

Page 44: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Dispersion and milling can be parallel rather than sequential processes

Theoretical

Actual

Dispersion vs. Breakage

Page 45: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

1 bar

2 bar

3 bar

Pressure Titration

Page 46: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Dry Method Development

Case Studies

Magnesium Stearate

Microcrystalline Cellulose

Page 47: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

High = 3 barMid = 2 barLow = 1 bar

Effect of Air Pressure: Mg Stearate

Page 48: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

0

2

4

6

8

10

12

14

16

18

D90

D50

D10

D90 15.258 14.394 12.822

D50 8.626 8.149 7.502

D10 4.862 4.564 4.234

1 2 3

Effect of Air Pressure: Mg Stearate

Page 49: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Reproducibility Test at 3 Bar

Page 50: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Reproducibility Test at 2 Bar

Page 51: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Reproducibility Test at 1 Bar

Page 52: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Effect of Air Pressure: MCC

Page 53: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

0

50

100

150

200

D90

D50

D10

D90 161.158 160.713 144.259

D50 65.938 64.599 58.578

D10 25.76 24.308 22.655

1 2 3

Effect of Air Pressure: MCC

Page 54: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Reproducibility Test at 3 Bar

Page 55: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Wet and Dry Comparison

Page 56: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Must have representative samplePowders: select air pressureSuspensions: wet, disperseCheck accuracy w/microscopeInvestigate system settings:

concentration, agitation, ultrasoundDesign for maximum precisionFollow guidelines in standards

Summary

Page 57: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

Danke Merci

Gracias

Большое спасибо

Grazie/اُشْك2 ر

Σας ευχαριστούμε

감사합니다 Obrigado

Tacka dig

谢谢 ขอบคุ�ณคุรั�บ

Thank youありがとうございました

धन्यवा�दநன்ற

Page 58: Method Development for Laser Diffraction

© 2013 HORIBA, Ltd. All rights reserved.

www.horiba.com/particle

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