Introduction Many products are manufacturing through compaction of - - PowerPoint PPT Presentation

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Introduction Many products are manufacturing through compaction of - - PowerPoint PPT Presentation

Charley Wu Chemical and Process Engineering University of Surrey, Guildford, UK 0 @charleywu @ C.Y.WU@surrey.ac.uk Introduction Many products are manufacturing through compaction of dry powders, involving powder flow into a confined space.


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SLIDE 1

Charley Wu Chemical and Process Engineering University of Surrey, Guildford, UK

0 @charleywu

@ C.Y.WU@surrey.ac.uk

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SLIDE 2

Introduction

Many products are manufacturing through compaction of dry powders, involving powder flow into a confined space.

w; 1p1 q:1:,:1m11

·Pharmaceutical ·Catalyst

  • Automotive

·Chemical , •Ceramic , ·Magnetic ·Food

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SLIDE 3

Typical Manufacturing Process

UNIVERSITY OF

  • i...=;;;... SURREY

~

Upper punch

I

compacts I

..

I

Lower punch I

..........................

Die Filling Compaction Ejection

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SLIDE 4

Why Die Filling Is Important?

Any problem during die filling will have a direct impact on the quality

  • f the final products.

Failure during die filling can lead to

  • Tablets of inaccurate dose!
  • Products with large weight variation
  • Products with non-uniform contents that detrimentally affect the

functionality

  • Gears of uneven strength and with weakest links.
  • Distortion (and complete failure) during subsequent processes, such

as sintering.

"If your doctor prescribed half a tablet a day, which half would you want to take? "(Malvern Instruments} 2008).

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SLIDE 5

Methodology (Exp. + Modelling)

D A combined experimental and numerical approach was employed to understand the die filling process. D A model die filling system was developed. D Die filling behaviour was visualised using a high speed video system. D Quantitative analysis was also performed using

  • PEPT -> particle velocity
  • A pressure sensor -> time evolution of deposited

mass.

  • An air pressure sensor -> air pressure build-up

D Mechanistic analysis was performed using DEM-CFO

'

SURREY

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SLIDE 6

. t I t

L

SUNUIVERRRSITYEYOF

A typical expenmen a se -up

~

High speed video

.,J'

Air pressure sensor

J

Iii

L ~

e:.. 22001

~

J

_F~

~

J

<C .,J

·:ml ...................... .

~+ am BO

75

  • 70

~ J

~

I

]

30

Mass pressure sensor

32 34 38 38

Time (s)

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SLIDE 7

PEPT Study

(Positron Emission Particle Tracking)

'

SURREY

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SLIDE 8

PEPT Study

30 trajectories of individual particles

L

UNIVERSITY OF

~

SllR.REY

Spherical microcrystalline cellulose ( Celphere, CP102 )

Initial position of the shoe

  • .-5' ~~ ~

'• V'i\7 v "' v7 'V w v"v

··-.

..

  • '2>
  • .
  • 0 •

.

. ()

  • o

6

  • 9
  • Die

Wu, C.-Y., X.F. Fan, F. Motazedian, J.P.K. Seville, D.J. Parker, A.C.F. Cocks, (2010). A Quantitative Investigation of Powder Flow during Die Filling Using Positron Emission Particle Tracking (PEPT). Proceedings of the Institution of Mechanical Engineers, Part E, Journal of Process Mechanical Engineering. 224(3): 169-175.

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SLIDE 9

DEM-CFO

The flow of particles is modelled using DEM.

The interaction between particles are rigorously modelled using theoretical contact mechanics:

  • Hertz-Mindlin-Deresiewicz for

elastic particles

  • JKR for adhesive particles

The interaction between air and particles is considered. The flow of air is modelled using CFO. Particle equations of motion: 8(Epf)

  • --+

at

8(Epfu) + '\7.

fUU )=

at

  • Vpf +V·Tf

Epfg

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SLIDE 10

DEM-CFO Validation

D Validation of DEM models is important. D Qualitatitive validation is easy, is it convincing? D Case-to-case quantitative validation is difficult.

" .

8 •

~

\

Experimental DEM-CFO

  • +
  • Guo Y, Wu C-Y, Thornton C. (2013) Modeling Gas-Particle Two-Phase Flows with Complex and Moving Boundaries using DEM-CFO with an Immersed Boundary Method. A/CHE

JOURNAL, 59 (4), pp. 1075-1087

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SLIDE 11

DEM-CFO with Non-spherical Particles '

SURREY

D Multi-sphere -> approximate particle shapes using clumped spheres. D Utilize the rigorous contact laws for modelling particle-particle interaction

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SLIDE 12

)

!(_ SUNUIVERRRSITYEYOF Die filling with real particles (Wu et al. 2016

~

Real crystal DEM approximation

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SLIDE 13

Flow from a stationary feeder

In Vacuum

InAir Ps =1500 kg/m

3 , dP =50 µm

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SLIDE 14

Flow from a stationary feeder

In Vacuun1

InAir

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SLIDE 15

Flow from a stationary feeder

  • 0. 7
.-,-.-r-.,-,-,-~-.-.-,-,-.-m.-.-.-r-.-.-.-,.-y-r-c-r-,-,-~-r-r-r-r-.-.-.~

06~0

................... .A

........................

~

...............

a

.......................

A."'.I"'i'*°"~

.

...........

llf!'

..... ..

0.50 0.40 0.30- 0.20 0.10 0.09

According to Beverloo equation, M* is in the range of 0.55-0.65.

.A. In vacuum ~

ln air ]Group 1

  • [n vacuum

1-n air

}Group 2

e In vacuum

Q In air

)Group3

T In vacuum }

\J Jn air

Group 4

......... Constant in vacuum

  • Power law in air
  • .os~,~-~

1~

10

4

I ~

10

6

I~

10

8

At<P

p

Normalised mass flowrate

M

Normalised particle density

<I>

= Ps

P

Pa

Archimedes Number

(

  • ) d3

A = Pa Ps

Pa gi p

r

1]2

This is in excellent agreement with Berveloo constants obtained experimentally (C is in the range of 0.55-0.65, for spherical particle c~0.58, see Seville et al. 1997).

Guo Y., Kafui K.D., Wu C.Y., Thornton C. and Seville J.P.K., (2009), A coupled DEM/CFO analysis of the effect of air on powder flow during die filling. A/CHE Journal, 55

(1 ): 49-62.

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SLIDE 16

Flow from a stationary feeder

'

SURREY

0.70~ 06~0

................................

..................................................................

~

. .

. ~

.... ~

.~

....

..

0.50 0.40 0.30 0.20 0.08 3

10

Air sensitive

  • In vacuum

!:;::. Jn air }Group I

  • In vacuum

0 In air

}Group 2

e In vacuum

0 ln air

}Group 3

T In vacuum }

'7 1

. Group4

v n atr

......... Constant in vacuum

  • Power law in air

Ar" </J

p Air inert

Guo Y., Kafui K.D., Wu C.Y., Thornton C. and Seville J.P.K., (2009), A coupled DEM/CFO analysis of the effect of air on powder flow during die filling. A/CHE Journal, 55

(1 ):

49-62.

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SLIDE 17

Flow from a moving feeder

(Fine sand, Vshoe=300 mm/s) (MCC, Vshoe=50 mm/s)

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SLIDE 18

Flow from a moving feeder

In Air ,.-~

,

In Air ~-=-

V=35 mm/s V=70 mm/s

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SLIDE 19

Flow from a moving feeder

0.8

~

0.6

.....

~ ;...,

.......... ..........

~

0.4

0.2 I I

I

/cruv

el\ i

  • In vacuum

0 In air

  • Fitting curve in vacuum
  • Fitting curve in air

8 =(99 .33/v )1 68

shoe

/

8 =(4 7 .26/v )

119 shoe

50 100 150 200 Shoe speed v 1 (nun/s)

S lOe

'

SURREY

D There is a critical filling speed during die filling, above which the die cannot be completely filled. D The critical filling speed is a function of powder properties, and process system parameters D For a given process system, the critical filling speed is dominated by powder

  • properties. This can also be

used to assess powder flowability.

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SLIDE 20

Flow from a moving feeder

C11t1cal Ftllu1c Spet-!d •

nu11 ~ •

200

CP30:'

Flo\'\' Ftu1ction 50 .

.\.ng.J.e of

repose

1.6

l\fr1~

Flo\\· R~1te 1

g ~ 1

'-

Good flowability Poor flowability

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SLIDE 21

Flow from a moving feeder

200

,,,-.....

rfj

] 150

......_,.

>

(.) 100

50

  • MCC PH102

e

MCC PH101

... MCCDG

+ Mannitol

D Mix 1

8

Mix2 Mix3

  • Eq.(9)
  • ... .
  • L-~-L-~

10 20 30

Flow index rljJ (mm)

40

'

SURREY

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SLIDE 22

A Mathematical Model for Die Filling

400

40

  • Experimental
  • Experimental

Model

300

30

  • Model
  • M>
  • ... -

l:ID

20

:~

200

  • Mt

~a

Mt

·-

lg

2

~

10 100

D

100

200

300 400 500

200 400

600

800 Filling speed (mm/s) Fiming speed (mm/s)

(a) (b)

  • Experimental

60 40

  • Experimental

so

Model

  • Model
  • 3D

Ga 40

  • illa
  • ~

30

..,. 2D

...,

ftl ftl

::!: 20 ::!:

10

  • 10

200

400

600

D 50

l!.00

150

200 250 Flllng speed (mm/s) Filling speed (mm/s)

(c) (d)

The variation of the deposited mass with the filling speeds for a) Silibeads 300; b) Cenopheres 500; c) Mannitol and d) Alumina 4.

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SLIDE 23

A Mathematical Model for Die Filling

  • QI)
  • ......

300 250 200

  • COE Experimental
  • -Full model

S300

e GBLSmm

E 150

  • u

>

100

I C500

~

so

Mann1to9

MCCOG

11

1.E+o3

1.E+o4

1

.. E+os

1.E+06 1.E+07

1

.. E+o8

1.E+o9 1.E+lO

The critical filling speed obtained in the closed die experiments as a function of~

(=Ar.<J>)

Ar= PaPsgd;

<I>= PP

')

rr

Pa

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SLIDE 24

Conclusions

D Powder into a confined space depends upon powder properties, die geometry and filling conditions. D The influence of air presence can be significant. D DEM-CFO is capable of capturing the major features during die filling. D Critical filling speed could be used to characterise powder flowability. D Based on air sensitivity classification obtained by Guo et al. (2010), a model was developed to predict the deposited mass and the critical filling speed.

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SLIDE 25

Acknowledgements

EPSRC IFPRI AstraZeneca Sanofi Pfizer

  • Dr. Yu Guo
  • Dr. Chunlei Pei
  • Dr. Serena Schiano
  • Mr. Joesry El Hebieshy
  • Ms. Anastasiya Zakhvatayeva
  • Dr. Colin Thornton
  • Dr. Ling Zhang

EPSRC

Engineering and Physical Sciences Research Council