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ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France poncelet@enitiaa"nantes.fr SIZE DISTRIBUTION ? Denis poncelet ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France poncelet@enitiaa"nantes.fr Size ? ! Diameter = first property of the capsules ! Define largelly the membrane or coating surface, then quantity the mechanical resistance the fluidisation and flowing properties the active loading and quantity ! Needed for most modelling of the membrane formation the release profile the biocatalyst kinetics #mass transfer$ ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France poncelet@enitiaa"nantes.fr Size ? From a few micrometers ... to a few millimeters ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France poncelet@enitiaa"nantes.fr Size distribution ? ! Mono"dispersion ? do not believe pictures ! Narrow size distribution allows better microcapsule formation control easier modelling more homogeneous properties ! Narrow size distribution = higher cost & lower production

Size ? Size distribution - IMPASCIENCE · • Sampling is the key point • Use raw data, avoid conversion • Make tendencies not absolute values. ENITIAA, UMR CNRS 6144 GEPEA, Nantes,

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Page 1: Size ? Size distribution - IMPASCIENCE · • Sampling is the key point • Use raw data, avoid conversion • Make tendencies not absolute values. ENITIAA, UMR CNRS 6144 GEPEA, Nantes,

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

SIZE DISTRIBUTION ?Denis poncelet

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

Size ?! Diameter = first property of the capsules

! Define largelly

• the membrane or coating surface, then quantity

• the mechanical resistance

• the fluidisation and flowing properties

• the active loading and quantity

! Needed for most modelling of

• the membrane formation

• the release profile

• the biocatalyst kinetics #mass transfer$

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

Size ?

From a few micrometers ... to a few millimeters

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

Size distribution ?

! Mono"dispersion ?

• do not believe pictures

! Narrow size distribution allows

• better microcapsule formation control

• easier modelling

• more homogeneous properties

! Narrow size distribution

! ! ! = higher cost & lower production

Page 2: Size ? Size distribution - IMPASCIENCE · • Sampling is the key point • Use raw data, avoid conversion • Make tendencies not absolute values. ENITIAA, UMR CNRS 6144 GEPEA, Nantes,

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

Size distribution ?

Controlled release

!

dc

dt= "D

(c " c')

e

!

ln(c " co

c# " co) = "k t

Burst e%ect ? ... no size distribution

Burst

!

ln(c " co

c# " co)

!

t!

c = 6% co

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

Size distribution ?

Mechanical resistance

!

vbreakage ÷ d4

d = 500 to 1000 !m

vbreakage varies from 1 to 16

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

How to measure the size ?

! Sieving analysis

! Microscopy

! Counting

! Laser di%raction

! Acoustic spectroscopy

http://en.wikipedia.org/wiki/Particle_size_distribution

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

Size distribution

Page 3: Size ? Size distribution - IMPASCIENCE · • Sampling is the key point • Use raw data, avoid conversion • Make tendencies not absolute values. ENITIAA, UMR CNRS 6144 GEPEA, Nantes,

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

0

0,50

1,00

1,50

2,00

0 1,00 2,00 3,00 4,00

Histograms

!

f =dF

dx=

1

" 2#exp

$(x$x)

2

2 " 2

x = log#d$

100 &

75 &

50 &

25 &

0 &

f F

xd 1 10 100 1000 10 000 !m

0

1

2

3

4

0 100,00 200,00 300,00 400,00

& of particles per 20 µm

!

Fx = f dx

0

x

" or f #x0

x

$

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

0

1

2

3

4

0 100,00 200,00 300,00 400,00

Histograms

0

0,50

1,00

1,50

2,00

0 50 100 150 200 250 300 350 400

& of particles per class

& of particles per 20 µm

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

Frequency !Frequency

! Numeric, fn #microscope$

! Volumic, fv #Malvern$

! Massic, fm #sieving$

! ...

!

fs = k x3

fn

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

Fv versus Fn

• Sampling is the key point• Use raw data, avoid conversion• Make tendencies not absolute values

Page 4: Size ? Size distribution - IMPASCIENCE · • Sampling is the key point • Use raw data, avoid conversion • Make tendencies not absolute values. ENITIAA, UMR CNRS 6144 GEPEA, Nantes,

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

Artefacts

< 5 &

0,5 µm

Most probably defaults assimilated to particles

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

Mean size ?

! Median = diameter of 50 & cumulative frequency = d50&

! Mode = diameter of maximum frequency

! Mean size ?

• numeric #microscope$

• volume #Malvern$

• surface

!

dn = d10 =ni di"ni"

= fn di

!

d43 =ni di

4"

ni di3"

=vi di"vi"

= fv di

!

ds = d32 =ni di

3"

ni di2"

=si di"si"

= fs di =1

as!

dv = d30 =ni di 3"ni"

3

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

Mean size ?

Mean size could be computed for all distributions

Multi"peaks ? multi"means ?

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

Which mean ?

! Function of the applications / model

EmulsificationMass transfer

!

d32

Fluidisation

!

d10

LoadingYield

!

d30

Sometime, mix of mean diameters

Page 5: Size ? Size distribution - IMPASCIENCE · • Sampling is the key point • Use raw data, avoid conversion • Make tendencies not absolute values. ENITIAA, UMR CNRS 6144 GEPEA, Nantes,

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

Size dispersion ?

! standard deviation, !

• graphically #!$

• ! = #d64&"d16&$/2 #!$

! Distribution

• numeric or volumic

• normal or log"normal

0

0,50

1,00

1,50

2,00

1,00 1,50 2,00 2,50 3,00

!

!

" 2 =fi (xi # x)

2$fi$

!

0

0,50

1,00

1,50

2,00

0 100,00 200,00 300,00 400,00

? ?

100 &

75 &

50 &

25 &

0 &

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

Standard deviation ?

0

0,50

1,00

1,50

2,00

1,00 1,50 2,00 2,50 3,00

! multi"peaks ?

• !’ = ! / d50&

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

Span ?

! Span = = #d90&"d10&$/d50&

! relative dispersion

! could be applied to all distributions

! take into consideration most particles

! deviations often under d10& and over d90&

0

0,50

1,00

1,50

2,00

1,00 1,50 2,00 2,50 3,00

100 &

75 &

50 &

25 &

0 &

ENITIAA, UMR CNRS 6144 GEPEA, Nantes, France ! ! ! ! ! ! poncelet@enitiaa"nantes.fr

Conclusions

! Even #apparently$ simple measurement needs standard

! Use simplest tool to measure the size

! Beware of the sampling

! Define your mean value

• mode or median are easier

• avoid conversion between distribution

! Use span to define dispersion

! Size distribution are not absolute value