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Interpreting Your Laser Diffraction
                        Particle Size Analysis Results
                                   Decoding the Acronyms and Finding Insights




                                                   Ian Treviranus
                                            ian.treviranus@horiba.com
                                            www.horiba.com/us/particle




© 2011 HORIBA, Ltd. All rights reserved.
Outline

         The Basics

         Define Parameters

         Choose Parameters

         Interpret Results

© 2011 HORIBA, Ltd. All rights reserved.
The Workflow


                                           +          +


                                    =

© 2011 HORIBA, Ltd. All rights reserved.
The Problem




                                                  =


© 2011 HORIBA, Ltd. All rights reserved.
The Basics
       Particle                            Distribution of Particles




© 2011 HORIBA, Ltd. All rights reserved.
The Basics
       Particle Size Particle Size Distribution




                        4 µm



© 2011 HORIBA, Ltd. All rights reserved.
The Basics

                Which is the most meaningful size?




                       different                    different
                       size definitions              results


© 2011 HORIBA, Ltd. All rights reserved.
The Basics

                              Which sizes can be measured?




© 2011 HORIBA, Ltd. All rights reserved.
The Basics

         Laser Diffraction
                  Equivalent Spherical Diameter


         Dynamic Light Scattering
                  Hydrodynamic Radius


         Image Analysis
                  Lengths, Widths, Equivalent Spherical


         Acoustic Spectroscopy
                  Equivalent Spherical Diameter


© 2011 HORIBA, Ltd. All rights reserved.
The Basics
         Laser Diffraction
         Assumes hard, spherical shape model




         q% = amount
         of each size
         by volume




© 2011 HORIBA, Ltd. All rights reserved.
The Basics
         Dynamic Light Scattering
         Assumes hard, spherical shape model




         Frequency %
         = amount
         of each size
         by volume




© 2011 HORIBA, Ltd. All rights reserved.
The Basics
         Image Analysis
         Measures particle projection  no shape assumption




                                                        Undersize
                                                        Passing
                                                        Q3




© 2011 HORIBA, Ltd. All rights reserved.
The Basics
         Acoustic Spectroscopy
         Assumes hard, spherical shape model




© 2011 HORIBA, Ltd. All rights reserved.
Poll!




© 2011 HORIBA, Ltd. All rights reserved.
Conclusions

          Understand the data
                   A little goes a long way!


          Know something about the particles
           in your sample

          Particles have multiple dimensions,
           know which dimension your analyzer
           measures!

© 2011 HORIBA, Ltd. All rights reserved.
Outline

         The Basics

         Define Parameters

         Choose Parameters

         Interpret Results

© 2011 HORIBA, Ltd. All rights reserved.
Defining Parameters




© 2011 HORIBA, Ltd. All rights reserved.
Terms, Terms, and more Terms

         Particle Size
         Monomodal:                        One Peak
         Bimodal:                          Two Peaks
         Multimodal:                       Multiple Peaks

         Monodisperse:                     All particles have same size
         Polydisperse:                     Particles have many sizes

         Volume diameter:                  Diameter of a sphere having the same
                                           volume as the particle
         Surface diameter:                 Diameter of a sphere having the same
                                           surface as the particle



© 2011 HORIBA, Ltd. All rights reserved.
Terms, Terms, and more Terms

         Particle Size
         Frequency% / q% /                 Amount of each size by volume
         p3 / Retained / Sph Vol%

         Volume-based diameter             Calculated from vol. distribution
                                           emphasizes coarse particles
                                           (larger volume)
         Number-based diameter             Calculated from number dist.
                                           (individual particles)
                                           emphasizes fine particles
         Cumulative% on diameter           % of distribution finer/coarser
                                           than specified size
         Diameter on cumulative%           Size at which a specified % of
                                           distribution is finer/coarser

© 2011 HORIBA, Ltd. All rights reserved.
Terms, Terms, and more Terms

         Particle Shape
         Acicular:                         Needle-shaped, rigid
         Angular:                          Edgy, hard angles
         Fibrous:                          Thread-like, non-rigid
         Granular/Blocky:                  Irregular-shaped, low aspect-ratio
         Spherical:                        Regular-shaped, unity aspect ratio

         Aspect ratio:                     Breadth / length OR Length / breadth
         Sphericity:                       How spherical is the particle?
         Roundness:                        How round is the particle?




© 2011 HORIBA, Ltd. All rights reserved.
Poll!




© 2011 HORIBA, Ltd. All rights reserved.
Size Terminology
                                             0.1µm 1.0µm     10µm 100µm


10-10             10-9                10-8     10-7   10-6   10-5   10-4       10-3     10-2   10-1    10-0
                                             100 nm

          nanometer                             micrometer                 millimeter                 meter
            nm                                  Micron or µm                   mm                        m

Angstrom
  (Å)

         The most common designation is micrometers or
         microns. When very small, in colloid region,
         measured in nanometers, typically by ultra
         microscopes or by dynamic light scattering.



 © 2011 HORIBA, Ltd. All rights reserved.
Relative Size


                                                   Human Hair




                                                   Visible Particles: Lint, Dust, width
                                                   of the ridges of fingertips.
                                                   Dust and free flowing powders
                                                   Suspensions and fine powders
                                                   Suspensions and fine powders
                                                   Emulsions and Colloids
                                                   Proteins, Viruses, and Macro-
                                                   Molecules



© 2011 HORIBA, Ltd. All rights reserved.
Poll!




© 2011 HORIBA, Ltd. All rights reserved.
Central Values


Mean
Weighted Average                                                   Mean
Center of Gravity                                                  Median
                                                                   and
                                                                   Mode
Median
50% Point

Mode
Peak of the distribution
Most common value

                                                            Size


© 2011 HORIBA, Ltd. All rights reserved.
What does “Mean” mean?
                          Three spheres of diameters 1,2,3 units


                                    1
                                           2
                                                             3


  What is the average size of these spheres?
                          Average size = (1+2+3) ÷ 3 =2.00
  This is called the D[1,0] - the number mean


© 2011 HORIBA, Ltd. All rights reserved.
Many possible Mean values
                                1 2  3
                X nl  D[1,0]            2.00
                                   3
                                 1 4  9                       None of the answers
                X ns  D[ 2,0]            2.16
                                    3                           are wrong they have just
                                                                been calculated using
                                         1  8  27             different techniques
                  X nv        D[ 3,0]    3         2.29
                                              3

                                   1  8  27
                  X sv  D[ 3,2]              2.57
                                    1 2  3

                                           1  16  81
                   X vm  D[ 4,3]                      2.72
                                           1  8  27

© 2011 HORIBA, Ltd. All rights reserved.
Volume-based Mean diameter
D[4,3] which is often referred to as the Volume Mean Diameter [ VMD ]


                                            D [4,3] =
                                                        D n 4
                                                             i    i

                                                        D n 3
                                                             i    i

                                 Monitoring the D[4,3] value in your specification
                                  will emphasize the detection of large particles




 © 2011 HORIBA, Ltd. All rights reserved.
Central Values revisited

                                                                    Mean
                                                                    Weighted Average
                                                  Mode
                                                                    Center of Gravity
                                                         Median

                                                           Mean     Median
                                                                    50% Point
                                                           D[4,3]

                                                                    Mode
                                                                    Peak of the distribution
                                                                    Most common value


                                           Size

  Remember: D[4,3] is sensitive to large particles

© 2011 HORIBA, Ltd. All rights reserved.
Most Common Statistics
half are smaller than this diameter half are larger than this diameter
                                                        D(v,0.5)
                                                        median

  10% of the particles are                                      90% of the particles are
smaller than this diameter                                      smaller than this diameter
                     D(v,0.1)                                   D(v,0.9)
                                                                        D(v,1.0)
                                                                               Never use
                                                                               the D100!
                                             Size µm
                                                   D(4,3) sensitive to large particles

  © 2011 HORIBA, Ltd. All rights reserved.
Standard Deviation

                                                                        Normal (Gaussian)
                                                                         Distribution Curve
               -1 STD DEV                                +1 STD DEV      = distribution mean
                                            68.27%
                                                                         = standard deviation
                                                                        Exp = base of natural
                                                                         logarithms


-2 STD DEV                                                    +2 STD DEV

                                  95.45%

                                                Mean

                                1                         - (x - )2
       Y=                      2               Exp [                     ]
                                                             22
 © 2011 HORIBA, Ltd. All rights reserved.
Distribution Width

                                                          Polydispersity Index
                                                           (PI, PDI)
                                                          Span
                                                          Geometric Std. Dev.
                                                          Variance
                                                          Etc…




© 2011 HORIBA, Ltd. All rights reserved.
Poll!




© 2011 HORIBA, Ltd. All rights reserved.
Conclusions

          Be familiar with the nomenclature

          Many parameters can describe
           distribution
                   D50, D10, D90 commonly used
                   See Technical Note 156 in Download Center for more info



          Which Mean do you mean?



© 2011 HORIBA, Ltd. All rights reserved.
Outline

         The Basics

         Define Parameters

         Choose Parameters

         Interpret Results

© 2011 HORIBA, Ltd. All rights reserved.
Choosing Parameters




© 2011 HORIBA, Ltd. All rights reserved.
Choosing good statistics

Statistics describing the distribution must…
Tell us about our process
Be relevant
Be controlled well
Be reproducible!


Poor precision is the result of either a poor
 method or poor statistical choices
                                                We can help!
                                            labinfo@horiba.com



 © 2011 HORIBA, Ltd. All rights reserved.
The Basis for Reliable Data
Reproducibility!
Prepare, measure, empty, repeat


What would be good reproducibility?
Look at the accepted standards

ISO 13320
   COV < 3% at Median (D50)                 COV = 100 * (StDev / Mean)
   COV < 5% at D10 and D90

USP <429>
  COV < 10% at Median (D50)
  COV < 15% at D10 and D90

Note: All limits double when D50 < 10 µm
Note: Must acquire at least 3 measurements from unique samplings
 © 2011 HORIBA, Ltd. All rights reserved.
Calculation Automation




                                     Unique, automatic feature in LA-950 software
                                     See Technical Note 169 in Download Center
                                         for instructions to use these features


© 2011 HORIBA, Ltd. All rights reserved.
Distribution Extremes

         At a distance of a few standard
          deviations, non-instrumental errors can
          dominate




© 2011 HORIBA, Ltd. All rights reserved.
2 and 3 Standard Deviations

 95% of the distribution is within 2 standard
  deviations from the Mean
 99.7% of the distribution is within 3
  standard
  deviations
  from the mean




© 2011 HORIBA, Ltd. All rights reserved.
Reproducibility at the Extremes

   If we want the same level of reproducibility at
    the D99 value as the D50, we need to
    analyze similar amounts of material in the
    D99 histogram band




© 2011 HORIBA, Ltd. All rights reserved.
Better Method to Monitor Extremes
         Instead of specifying the D95, D99,
          D99.99, D100, DMax

         Specify the % of material greater than a
          certain size




© 2011 HORIBA, Ltd. All rights reserved.
Poll!




© 2011 HORIBA, Ltd. All rights reserved.
Conclusions
          Parameters should reflect product
           performance
                   But don’t make your life more difficult than it needs to be!
                   See Webinar TR007 Setting Size Specifications and
                   Technical Note 161 for more information


          Look to appropriate standards
                   ISO 13320, USP <429> can provide guidance


          Avoid monitoring the extremes
           whenever possible
                   Better to use D(4,3) when you want spec. to be
                   sensitive to presence of large particles

© 2011 HORIBA, Ltd. All rights reserved.
Outline

         The Basics

         Define Parameters

         Choose Parameters

         Interpret Results

© 2011 HORIBA, Ltd. All rights reserved.
Advanced Result Interpretation




© 2011 HORIBA, Ltd. All rights reserved.
General
Multiple Modes
Multiple peaks can be better described individually

        D10                             D50   D90




 © 2011 HORIBA, Ltd. All rights reserved.
Laser Diffraction
Multiple Scattering
Watch for finer “particles” appearing with increasing concentration




 © 2011 HORIBA, Ltd. All rights reserved.
Multiple Scattering
                                                                                              Multiple Scattering Example

                                                             2.50E+00
                                                                                                                                                    1 Bottle
                                                             2.00E+00                                                                               2 Bottles
                                                                                                                                                    3 Bottles


                                           Light Intensity
                                                                                                                                                    4 Bottles
                                                             1.50E+00
                                                                                                                                                    5 Bottles
                                                                                                                                                    6 Bottles
                                                             1.00E+00
                                                                                                                                                    7 Bottles
                                                                                                                                                    8 Bottles
                                                             5.00E-01                                                                               9 Bottles
                                                                                                                                                    10 Bottles
                                                             0.00E+00
                                                                        45        50          55           60          65           70         75
                                                                             Detector Number (higher detector numbers for smaller particles)



                                                                                           Multiple Scattering Example Zoom

                                                             6.00E-01
                                                                                                                                                    1 Bottle
                                                             5.00E-01
                                                                                                                                                    2 Bottles
                                                                                                                                                    3 Bottles
                                                             4.00E-01
                                           Light Intensity




                                                                                                                                                    4 Bottles
                                                                                                                                                    5 Bottles
                                                             3.00E-01
                                                                                                                                                    6 Bottles
                                                                                                                                                    7 Bottles
                                                             2.00E-01
                                                                                                                                                    8 Bottles

                                                             1.00E-01                                                                               9 Bottles
                                                                                                                                                    10 Bottles
                                                             0.00E+00
                                                                        65                                 70                                  75
                                                                             Detector Number (higher detector numbers for smaller particles)




© 2011 HORIBA, Ltd. All rights reserved.
Laser Diffraction
Dispersing Agglomerates
Watch for no change in coarsest particles with changing energy




                                                           2 bar

                                                                   1 bar

                                                   3 bar



© 2011 HORIBA, Ltd. All rights reserved.
Laser Diffraction
Breaking Particles
Watch for finer particles being created with increasing energy




                                            High = 3 bar
                                            Mid = 2 bar
                                            Low = 1 bar




 © 2011 HORIBA, Ltd. All rights reserved.
Conclusions

         Look at the distribution graph
                   See the forest AND the trees



         Precision != Accuracy
                   Vary measurement and calculation parameters




© 2011 HORIBA, Ltd. All rights reserved.
For More Details

           Visit www.horiba.com/us/particle

           Contact us directly at labinfo@horiba.com

           Visit the Download Center to find this recorded
           presentation and many more on other topics




© 2011 HORIBA, Ltd. All rights reserved.

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Understanding Your Particle Size Analyzer Results

  • 1. Interpreting Your Laser Diffraction Particle Size Analysis Results Decoding the Acronyms and Finding Insights Ian Treviranus ian.treviranus@horiba.com www.horiba.com/us/particle © 2011 HORIBA, Ltd. All rights reserved.
  • 2. Outline The Basics Define Parameters Choose Parameters Interpret Results © 2011 HORIBA, Ltd. All rights reserved.
  • 3. The Workflow + + = © 2011 HORIBA, Ltd. All rights reserved.
  • 4. The Problem = © 2011 HORIBA, Ltd. All rights reserved.
  • 5. The Basics Particle Distribution of Particles © 2011 HORIBA, Ltd. All rights reserved.
  • 6. The Basics Particle Size Particle Size Distribution 4 µm © 2011 HORIBA, Ltd. All rights reserved.
  • 7. The Basics Which is the most meaningful size? different different size definitions results © 2011 HORIBA, Ltd. All rights reserved.
  • 8. The Basics Which sizes can be measured? © 2011 HORIBA, Ltd. All rights reserved.
  • 9. The Basics Laser Diffraction Equivalent Spherical Diameter Dynamic Light Scattering Hydrodynamic Radius Image Analysis Lengths, Widths, Equivalent Spherical Acoustic Spectroscopy Equivalent Spherical Diameter © 2011 HORIBA, Ltd. All rights reserved.
  • 10. The Basics Laser Diffraction Assumes hard, spherical shape model q% = amount of each size by volume © 2011 HORIBA, Ltd. All rights reserved.
  • 11. The Basics Dynamic Light Scattering Assumes hard, spherical shape model Frequency % = amount of each size by volume © 2011 HORIBA, Ltd. All rights reserved.
  • 12. The Basics Image Analysis Measures particle projection  no shape assumption Undersize Passing Q3 © 2011 HORIBA, Ltd. All rights reserved.
  • 13. The Basics Acoustic Spectroscopy Assumes hard, spherical shape model © 2011 HORIBA, Ltd. All rights reserved.
  • 14. Poll! © 2011 HORIBA, Ltd. All rights reserved.
  • 15. Conclusions  Understand the data A little goes a long way!  Know something about the particles in your sample  Particles have multiple dimensions, know which dimension your analyzer measures! © 2011 HORIBA, Ltd. All rights reserved.
  • 16. Outline The Basics Define Parameters Choose Parameters Interpret Results © 2011 HORIBA, Ltd. All rights reserved.
  • 17. Defining Parameters © 2011 HORIBA, Ltd. All rights reserved.
  • 18. Terms, Terms, and more Terms Particle Size Monomodal: One Peak Bimodal: Two Peaks Multimodal: Multiple Peaks Monodisperse: All particles have same size Polydisperse: Particles have many sizes Volume diameter: Diameter of a sphere having the same volume as the particle Surface diameter: Diameter of a sphere having the same surface as the particle © 2011 HORIBA, Ltd. All rights reserved.
  • 19. Terms, Terms, and more Terms Particle Size Frequency% / q% / Amount of each size by volume p3 / Retained / Sph Vol% Volume-based diameter Calculated from vol. distribution emphasizes coarse particles (larger volume) Number-based diameter Calculated from number dist. (individual particles) emphasizes fine particles Cumulative% on diameter % of distribution finer/coarser than specified size Diameter on cumulative% Size at which a specified % of distribution is finer/coarser © 2011 HORIBA, Ltd. All rights reserved.
  • 20. Terms, Terms, and more Terms Particle Shape Acicular: Needle-shaped, rigid Angular: Edgy, hard angles Fibrous: Thread-like, non-rigid Granular/Blocky: Irregular-shaped, low aspect-ratio Spherical: Regular-shaped, unity aspect ratio Aspect ratio: Breadth / length OR Length / breadth Sphericity: How spherical is the particle? Roundness: How round is the particle? © 2011 HORIBA, Ltd. All rights reserved.
  • 21. Poll! © 2011 HORIBA, Ltd. All rights reserved.
  • 22. Size Terminology 0.1µm 1.0µm 10µm 100µm 10-10 10-9 10-8 10-7 10-6 10-5 10-4 10-3 10-2 10-1 10-0 100 nm nanometer micrometer millimeter meter nm Micron or µm mm m Angstrom (Å) The most common designation is micrometers or microns. When very small, in colloid region, measured in nanometers, typically by ultra microscopes or by dynamic light scattering. © 2011 HORIBA, Ltd. All rights reserved.
  • 23. Relative Size Human Hair Visible Particles: Lint, Dust, width of the ridges of fingertips. Dust and free flowing powders Suspensions and fine powders Suspensions and fine powders Emulsions and Colloids Proteins, Viruses, and Macro- Molecules © 2011 HORIBA, Ltd. All rights reserved.
  • 24. Poll! © 2011 HORIBA, Ltd. All rights reserved.
  • 25. Central Values Mean Weighted Average Mean Center of Gravity Median and Mode Median 50% Point Mode Peak of the distribution Most common value Size © 2011 HORIBA, Ltd. All rights reserved.
  • 26. What does “Mean” mean? Three spheres of diameters 1,2,3 units 1 2 3 What is the average size of these spheres? Average size = (1+2+3) ÷ 3 =2.00 This is called the D[1,0] - the number mean © 2011 HORIBA, Ltd. All rights reserved.
  • 27. Many possible Mean values 1 2  3 X nl  D[1,0]   2.00 3 1 4  9 None of the answers X ns  D[ 2,0]   2.16 3 are wrong they have just been calculated using 1  8  27 different techniques X nv  D[ 3,0]  3  2.29 3 1  8  27 X sv  D[ 3,2]   2.57 1 2  3 1  16  81 X vm  D[ 4,3]   2.72 1  8  27 © 2011 HORIBA, Ltd. All rights reserved.
  • 28. Volume-based Mean diameter D[4,3] which is often referred to as the Volume Mean Diameter [ VMD ] D [4,3] = D n 4 i i D n 3 i i Monitoring the D[4,3] value in your specification will emphasize the detection of large particles © 2011 HORIBA, Ltd. All rights reserved.
  • 29. Central Values revisited Mean Weighted Average Mode Center of Gravity Median Mean Median 50% Point D[4,3] Mode Peak of the distribution Most common value Size Remember: D[4,3] is sensitive to large particles © 2011 HORIBA, Ltd. All rights reserved.
  • 30. Most Common Statistics half are smaller than this diameter half are larger than this diameter D(v,0.5) median 10% of the particles are 90% of the particles are smaller than this diameter smaller than this diameter D(v,0.1) D(v,0.9) D(v,1.0) Never use the D100! Size µm D(4,3) sensitive to large particles © 2011 HORIBA, Ltd. All rights reserved.
  • 31. Standard Deviation  Normal (Gaussian) Distribution Curve -1 STD DEV +1 STD DEV   = distribution mean 68.27%   = standard deviation  Exp = base of natural logarithms -2 STD DEV +2 STD DEV 95.45% Mean 1 - (x - )2 Y=  2 Exp [ ] 22 © 2011 HORIBA, Ltd. All rights reserved.
  • 32. Distribution Width  Polydispersity Index (PI, PDI)  Span  Geometric Std. Dev.  Variance  Etc… © 2011 HORIBA, Ltd. All rights reserved.
  • 33. Poll! © 2011 HORIBA, Ltd. All rights reserved.
  • 34. Conclusions  Be familiar with the nomenclature  Many parameters can describe distribution D50, D10, D90 commonly used See Technical Note 156 in Download Center for more info  Which Mean do you mean? © 2011 HORIBA, Ltd. All rights reserved.
  • 35. Outline The Basics Define Parameters Choose Parameters Interpret Results © 2011 HORIBA, Ltd. All rights reserved.
  • 36. Choosing Parameters © 2011 HORIBA, Ltd. All rights reserved.
  • 37. Choosing good statistics Statistics describing the distribution must… Tell us about our process Be relevant Be controlled well Be reproducible! Poor precision is the result of either a poor method or poor statistical choices We can help! labinfo@horiba.com © 2011 HORIBA, Ltd. All rights reserved.
  • 38. The Basis for Reliable Data Reproducibility! Prepare, measure, empty, repeat What would be good reproducibility? Look at the accepted standards ISO 13320 COV < 3% at Median (D50) COV = 100 * (StDev / Mean) COV < 5% at D10 and D90 USP <429> COV < 10% at Median (D50) COV < 15% at D10 and D90 Note: All limits double when D50 < 10 µm Note: Must acquire at least 3 measurements from unique samplings © 2011 HORIBA, Ltd. All rights reserved.
  • 39. Calculation Automation Unique, automatic feature in LA-950 software See Technical Note 169 in Download Center for instructions to use these features © 2011 HORIBA, Ltd. All rights reserved.
  • 40. Distribution Extremes At a distance of a few standard deviations, non-instrumental errors can dominate © 2011 HORIBA, Ltd. All rights reserved.
  • 41. 2 and 3 Standard Deviations 95% of the distribution is within 2 standard deviations from the Mean 99.7% of the distribution is within 3 standard deviations from the mean © 2011 HORIBA, Ltd. All rights reserved.
  • 42. Reproducibility at the Extremes If we want the same level of reproducibility at the D99 value as the D50, we need to analyze similar amounts of material in the D99 histogram band © 2011 HORIBA, Ltd. All rights reserved.
  • 43. Better Method to Monitor Extremes Instead of specifying the D95, D99, D99.99, D100, DMax Specify the % of material greater than a certain size © 2011 HORIBA, Ltd. All rights reserved.
  • 44. Poll! © 2011 HORIBA, Ltd. All rights reserved.
  • 45. Conclusions  Parameters should reflect product performance But don’t make your life more difficult than it needs to be! See Webinar TR007 Setting Size Specifications and Technical Note 161 for more information  Look to appropriate standards ISO 13320, USP <429> can provide guidance  Avoid monitoring the extremes whenever possible Better to use D(4,3) when you want spec. to be sensitive to presence of large particles © 2011 HORIBA, Ltd. All rights reserved.
  • 46. Outline The Basics Define Parameters Choose Parameters Interpret Results © 2011 HORIBA, Ltd. All rights reserved.
  • 47. Advanced Result Interpretation © 2011 HORIBA, Ltd. All rights reserved.
  • 48. General Multiple Modes Multiple peaks can be better described individually D10 D50 D90 © 2011 HORIBA, Ltd. All rights reserved.
  • 49. Laser Diffraction Multiple Scattering Watch for finer “particles” appearing with increasing concentration © 2011 HORIBA, Ltd. All rights reserved.
  • 50. Multiple Scattering Multiple Scattering Example 2.50E+00 1 Bottle 2.00E+00 2 Bottles 3 Bottles Light Intensity 4 Bottles 1.50E+00 5 Bottles 6 Bottles 1.00E+00 7 Bottles 8 Bottles 5.00E-01 9 Bottles 10 Bottles 0.00E+00 45 50 55 60 65 70 75 Detector Number (higher detector numbers for smaller particles) Multiple Scattering Example Zoom 6.00E-01 1 Bottle 5.00E-01 2 Bottles 3 Bottles 4.00E-01 Light Intensity 4 Bottles 5 Bottles 3.00E-01 6 Bottles 7 Bottles 2.00E-01 8 Bottles 1.00E-01 9 Bottles 10 Bottles 0.00E+00 65 70 75 Detector Number (higher detector numbers for smaller particles) © 2011 HORIBA, Ltd. All rights reserved.
  • 51. Laser Diffraction Dispersing Agglomerates Watch for no change in coarsest particles with changing energy 2 bar 1 bar 3 bar © 2011 HORIBA, Ltd. All rights reserved.
  • 52. Laser Diffraction Breaking Particles Watch for finer particles being created with increasing energy High = 3 bar Mid = 2 bar Low = 1 bar © 2011 HORIBA, Ltd. All rights reserved.
  • 53. Conclusions Look at the distribution graph See the forest AND the trees Precision != Accuracy Vary measurement and calculation parameters © 2011 HORIBA, Ltd. All rights reserved.
  • 54. For More Details Visit www.horiba.com/us/particle Contact us directly at labinfo@horiba.com Visit the Download Center to find this recorded presentation and many more on other topics © 2011 HORIBA, Ltd. All rights reserved.

Notes de l'éditeur

  1. Particle size is specified in fractions of a meter. The most common designation is micrometers or microns. A micron is one millionth of a meter. Most measured particles fall into this range. There are applications in which the particles may be very small, in which they may be specified in nanometers. These applications are usually in the colloid region and are measured with electron microscopes or dynamic light scattering devices
  2. Particle size distributions can take on a large number of shapes and sizes. It would be impossible for a practical analyzer design to properly display all of these curves. For this reason, particle size distributions are represented by a series of segments or channels known collectively as a histogram. As shown in the figure, a histogram is a stepwise approximation to a continuous distribution. The number of segments or channels is variable. However, if there are too few channels, the distribution will not be well represented. If there are too many, the data become cumbersome. The number of channels selected then becomes a matter of choice based on design, practicality and aesthetics. Because we have a distribution of sizes, we will need to use several statistical measures to describe the whole. Median, mean, or mode describe the center of the distribution in different ways. Percentiles can be used to define specific points along the distribution. Standard deviation or CV can be used to describe the width of the distribution.
  3. Here are additional mean diameters that we can calculate for our simple distribution.
  4. Here is the equation used to calculate the D[4,3], which is sensitive to the presence of coarse particles. It may make sense to include this specification if the presence of coarse particles is detrimental to product performance, but be aware each new value included in a specification implies one more way for the product to fail the spec.
  5. From this example, we can see that for a non-Gaussian distribution, the mean, median and mode are at different points in the distribution. It is important to realize the differences between these three measures of the center of a distribution.
  6. Standard deviation is a statistical measure of the width of a distribution. One standard deviation is the width which contains 68.27% of the total distribution. Two standard deviations contain 95.45% of the total distribution.
  7. When setting particle size specifications on drug substances, keep several thoughts in mind. Laser diffraction is inherently a very repeatable technique. If multiple measurements of the same sample generate high RSD’s then work at your sampling, dispersion and standard operating procedures until they reach the ranges suggested in this presentation. You final specifications should be set depending on the product performance, and then tightened to take into account errors from sampling, measurement, etc.
  8. Ten (10) bottles of Whitehouse PS202 (3-30um) glass beads added to the LA-950. The percent transmittance of each light source (red laser and blue LED) are shown to illustrate how the LA-950 reports “concentration”. The Verifications were established for D10, D50, and D90 values according to the NIST certification, material uncertainty, and ISO-based instrument tolerance (5, 3, 5%). The D10 values do not pass Verification starting at bottle number 3. D50 falls out of range at bottle number 7.
  9. Using the Intensity Graph feature of the LA-950, we can extract the light scattering intensity for each detector angle (i.e. light scattering pattern) used during measurement. All 10 measurements had the light scattering pattern extracted and are graphed here in relation to each other. Typical multiple scattering behavior shows us non-linear increase in scattered light intensity at wide angles (indicated here by increasing detector number). We see that the first two bottles exhibit very similar light scattering patterns and that the dissimilarity increases with added material and increased particulate concentration. Note that the light scattering pattern appears normalized in the top graph (displaying the entire detector range used for measurement). The lower number (i.e. lower angle, larger particle) detectors exhibit smaller light intensity values as concentration increases. This is the behavior we expect. The scattered light that should be hitting these lower number detectors is instead being re-directed (re-diffracted) by additional particles.