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www.bhrgroup.com © BHR Group 2017 Project 2.2: Effect of Particle Concentration on Break-up Kinetics using different Bead Fill Ratios on Milling Clusters of Nanoscale Silica Particles Dr Nigel Heywood; Brian Perkins [email protected] Mobile: +44 (0) 7847 627044 Direct dial: +44 (0) 330 119 19 87 24-25 May 2017 DOMINO Spring Meetings Confidential to DOMINO Members

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Page 1: Project 2.2: Effect of Particle Concentration on Break-up ...domino.bhrgroup.com/Portals/0/Meeting Presentations/Spring 2017/… · Project 2.2: Effect of Particle Concentration on

www.bhrgroup.com © BHR Group 2017

Project 2.2: Effect of Particle Concentration on Break-up Kinetics using different Bead Fill Ratios on Milling Clusters of Nanoscale Silica Particles

Dr Nigel Heywood; Brian Perkins [email protected] Mobile: +44 (0) 7847 627044

Direct dial: +44 (0) 330 119 19 87

24-25 May 2017 DOMINO Spring Meetings Confidential to DOMINO Members

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© BHR Group 2017 2

Introduction- Background Stirred bead mills have been used in industry quite widely for fine and ultrafine grinding of high concentration slurries:

Inkyo et al. (2006), Journal of Colloid and Interface Science 304, 535-540

• minerals

• ceramic materials

• pigments

• chemical products

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© BHR Group 2017 3

Operation modes

Series of mills

Re-circulation

Batch

Re-circulation

Mills in series

Schwedes and Bunge, Advanced Powder Technology,1992

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© BHR Group 2017 4

Background

The milling process (when recirculation mode is used) is affected by several factors:

• Stirrer (accelerator) speed

• Grinding bead size

• Grinding bead filling volume (“Fill Ratio”)

• Solids concentration

• Continuous phase viscosity

• Recirculation flowrate

• Residence time and number of tank turnovers (determined by flowrate and volume)

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© BHR Group 2017 5

WAB SBM

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© BHR Group 2017 6

WAB DYNO Mill operated in re-circulation loop of a stirred tank

Three accelerators; diameter: 0.064 m

Gross dispersion volume in the chamber measured at 495 ml

Actual effective volume is less due to presence of beads

DYNO®-Mill ML WAB brochure DYNO®-Mill ML WAB brochure

Experimental Setup

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© BHR Group 2017 17-218/05/2017 7

Previous DOMINO work with a stirred bead mill

The stirred bead mill has been used for the following systems:

Aerosil 200V-in-water

► Solid concentration: 1 – 15 wt.%

Zinc oxide in water

► Solid concentration: 5 wt.%

Nanoclay in polyol

► Solid concentration: 3 wt.%

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© BHR Group 2015 8

Previous DOMINO work with Aerosil 200V in Water using a SBM to 2013 (from DOM 65 report)

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© BHR Group 2017 9

Previous Recent DOMINO work with 15 % Aerosil 200V in Water using a SBM in 2014

(tip speed 8 m/s, dispersion volume 2 litres; 42.5 litre/h)

Bead size Fill ratio

1.0 mm 65%

0.8 mm 65%

1.0 mm 50%

1.0/0.3 mm 65%

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© BHR Group 2017 10

2015/2016: Aerosil 200V in Distilled Water using a (tip speed 8 m/s, dispersion volume 4 litres; 1.0 mm bead size)

Aerosil 200V

Concentration

Fill ratio

Flowrate

through mill,

l/h

2014/2015

Work

(all at 42.5 l/h)

10% 45% 40 -

10% 55% 40 -

10% 65% 40 -

15% 45% 40 -

15% 55% 40 50%

15% 65% 40 65%

(15% 65% 20) -

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© BHR Group 2017 11

Objectives of current study and scope of work

To investigate the effects of nanocluster concentration and bead fill ratio on mechanism and kinetics of break-up using a stirred bead mill • 5% w:w Aerosil 200V was dispersed in distilled water

• Using a tip speed 8 m/s, dispersion volume 4 litres; 1.0 mm bead size, 40.9 l/h flowrate.

• Results for 10% and 15% w:w presented at May 2016 SCM • Results for 5%, 10% and 15% compared here to see if fines and

coarse particle generation at 5% concentration is a function of fill ratio (found not to be at 15%, but possibly at 10%)

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© BHR Group 2017 12

Definition of “Bead Ratio” or “Fill Ratio”

Net volume of bead mill, Vm, = total volume inside mill minus volume occupied by accelerators

“Volume of beads”, Vb, is volume of beads and air when beads poured randomly into a graduated cylinder

Bead or Fill Ratio = Vb/Vm x 100%

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© BHR Group 2017 13

Experimental- Protocol and operating conditions

Pre-dispersion preparation:

► Aerosil 200V was weighed at a concentration of 5% w:w and hand-mixed into distilled water, giving a total volume of 4 litres

► This blend was then mixed at 120 rpm for 30 min in a baffled tank equipped with a pitched blade turbine

Samples were taken at regular intervals once milling started.

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© BHR Group 2017 14

Experimental- Protocol and operating conditions

Aerosil 200V concentrations : 5%, 10% and 15%

Fill ratios: 45% , 55% and 65%

Experiments at accelerator tip speed of 8 m/s

A peristaltic pump was used providing a flow rate of around 40.9 l/h

Tank volume: 4 litres

1 mm TOSOH beads

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Materials- Dispersed phase ► Aerosil® 200V is a fumed hydrophilic silica manufactured by Evonik Ind.

► The primary particle is 12 nm

► Electron microscopy and particle size measurements have shown smallest aggregates of around 50-60 nm

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© BHR Group 2017 16

Dispersion Analysis (Particle Size Distribution)

Beckman-Coulter LS 230

Laser diffraction (0.4 – 2000 mm) + PIDS (Polarization Intensity Differential Scattering) (0.04 – 0.4 mm)

40 nm – 2000 mm

Refractive index of silica: 1.46 + 0.01 i

Samples were taken from the stirred tank

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Break up of nanoparticle clusters

Primary Particles

Aggregates

Agglomerates Erosion

Rupture

Shattering

0

5

10

15

20

25

0.01 0.1 1 10 100 1000

Particle Size, µm

Vo

lum

e %

Erosiont=0t>0t>>0t→∞

0

5

10

15

20

25

0.01 0.1 1 10 100 1000

Particle Size, µm

Vo

lum

e %

Erosiont=0t>0t>>0t→∞

t=0t>0t>>0t→∞

0

5

10

15

20

25

0.01 0.1 1 10 100 1000

Particle Size, µm

Vo

lum

e %

Rupturet=0t>0t>>0t→∞

0

5

10

15

20

25

0.01 0.1 1 10 100 1000

Particle Size, µm

Vo

lum

e %

Rupturet=0t>0t>>0t→∞

t=0t>0t>>0t→∞

Shattering

0

5

10

15

20

25

0.01 0.1 1 10 100 1000

Particle Size, µm

Vo

lum

e %

Rupturet=0t>0t>>0t→∞

t=0t>0t>>0t→∞

Ozcan-Taskin, N. G., et al., Chem Eng Res Des (2009), doi:10.1016/j.Cherd.2008.12.012

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Evolution of PSD- 5% Aerosil 200V : 45% Fill Ratio

Evolution of PSD indicates erosion as the predominant break up mechanism

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© BHR Group 2017 19

Evolution of PSD- 5% Aerosil 200V : 55% Fill Ratio

Evolution of PSD indicates erosion as the predominant break up mechanism

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© BHR Group 2017 20

Evolution of PSD- 5% Aerosil 200V : 65% Fill Ratio

Evolution of PSD indicates erosion as the predominant break up mechanism

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© BHR Group 2017 21

Evolution of PSD- 10% Aerosil 200V : 45% Fill Ratio (2016)

Evolution of PSD indicates erosion as the predominant break up mechanism

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© BHR Group 2017 22

Evolution of PSD- 10% Aerosil 200V : 55% Fill Ratio (2016)

Evolution of PSD indicates erosion as the predominant break up mechanism

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© BHR Group 2017 23

Evolution of PSD- 10% Aerosil 200V : 65% Fill Ratio (2016)

Evolution of PSD indicates erosion as the predominant break up mechanism

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© BHR Group 2017 24

Evolution of PSD- 15% Aerosil 200V : 45% Fill Ratio (2016)

Evolution of PSD indicates erosion as the predominant break-up mechanism

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© BHR Group 2017 25

Evolution of PSD- 15% Aerosil 200V : 55% Fill Ratio (2016)

Evolution of PSD indicates erosion as the predominant break-up mechanism

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© BHR Group 2017 26

Evolution of PSD- 15% Aerosil 200V : 65% Fill Ratio (2016)

Evolution of PSD indicates erosion as the predominant break-up mechanism

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© BHR Group 2017 27

Analysis of Particle Size Distribution (PSD)

“Fines” always defined as particles < 1 µm

“Coarse” always defined as particles > 1 µm

Sauter mean diameter, d32, µm

► Defined as the diameter of a sphere that has the same volume/surface area ratio as a particle of interest

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© BHR Group 2017 28

Evolution of d32 for fines – 5%, 10% and 15% Aerosil in water

After 20 mins, Sauter mean diameter of “fines” is of the order of 120- 140 nm (0.12 to 0.14 micron) in agreement with previous results with Aerosil 200V in water

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© BHR Group 2017 29

Fines generation rate- 10% Aerosil in Distilled Water

At 10%, break-up kinetics seems slightly greater at higher fill ratios after 20 mins

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© BHR Group 2017 30

Fines generation rate- 15% Aerosil in Distilled Water

At 15% Aerosil, break-up rate appears independent of fill ratio

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© BHR Group 2017 31

Fines generation rate- 5% Aerosil in Distilled Water

As the fill ratio is increased from 45% to 65%, break-up rate appears to be largely constant over time at 5% Aerosil 200V, same as 15%

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© BHR Group 2017 32

Number of Tank Turnovers, Nt, Effective Mill Volume, Veff and Cumulative Residence Time (RT), Tcr

Number of Tank Turnovers (dimensionless), Nt

► Nt = Volume flowrate Q (litre/min)*time (min)/Tank Volume, Vt (litre)

► Volume flowrate, Q = 40/60 (litre/min)

► Tank volume, Vt = 4 litre

Effective Mill Volume (litre)

► Veff= Vm-0.62*Vb

► Vb/Vm * 100% - Fill Ratio

Cumulative Residence Time (min)

► Tcr = Veff/Q*Nt = Veff*time/Vt

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© BHR Group 2017 33

Effective (or “Free”) Volume in Bead Mill, Veff

Fill Ratio Veff

(litre)

45% 0.357

55% 0.326

65% 0.296

0% 0.495

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© BHR Group 2017 34

Fines generation rate- 10% Aerosil in Distilled Water

At 10% Aerosil, break-up kinetics greater at higher fill ratios after RT of 2 mins

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© BHR Group 2017 35

Fines generation rate- 15% Aerosil in Distilled Water

At 15% Aerosil, break-up rate confirmed as independent of fill ratio when related to cumulative residence time within bead mill

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© BHR Group 2017 36

Fines generation rate- 5% Aerosil in Distilled Water

Break-up kinetics in terms of RT shows no Fill Ratio dependence

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© BHR Group 2017 37

Fines Generation Rate : 5%, 10%, 15% Aerosil in Distilled Water

Fines generation rate appears to be slightly faster at 15% Aerosil concentration

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© BHR Group 2017 38

Evolution of d32 coarse particles at 10% Aerosil 200V

At 10%, rate of reduction in coarse d32 greater at higher fill ratios after 30 mins

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© BHR Group 2017 39

Evolution of d32 coarse particles at 15% Aerosil 200V

At 15%. rate of reduction in coarse d32 seems independent of fill ratio

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© BHR Group 2017 40

Evolution of d32 coarse particles at 5% Aerosil 200V

At 5%, no effect of Fill Ratio on Coarse Particle Size Development

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© BHR Group 2017 41

Evolution of d32 coarse particles at 10% Aerosil 200V, RT Plot

At 10%. rate of reduction in coarse d32 seems faster at higher fill ratios

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© BHR Group 2017 42

Evolution of d32 coarse particles at 15% Aerosil 200V, RT Plot

At 15%. rate of reduction in coarse d32 seems independent of fill ratio

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© BHR Group 2017 43

Evolution of d32 coarse particles at 5% Aerosil 200V, RT Plot

At 5%. RT plot shows rate of reduction in coarse d32 independent of fill ratio

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© BHR Group 2017 44

Evolution of d32 coarse particles at 5, 10, 15% Aerosil 200V, RT Plot

Rate of reduction in coarse d32 appears to be greater for the 5% up to 3 residence times compared with 10% and 15%. Is the difference significant?

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© BHR Group 2017 45

Conclusions

Deagglomeration of 5% w:w Aerosil 200V in distilled water studied using a stirred bead mill to

► establish effect of bead fill ratio on break-up kinetics and mechanisms

► compare break-up behaviour with 10% and 15% data obtained in DOMINO year 2015/2016. Fill ratios were 45%, 55% and 65%.

Predominant mechanism of break-up was found to be erosion, irrespective of Aerosil concentration and bead fill ratio.

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© BHR Group 2017 46

Conclusions

Sauter mean diameter d32 of “fines” (aggregates) was of the order of 120 to 140 nm for 5% Aerosil concentration and fill ratio combinations after 20 minutes for a 4-litre dispersion

► in agreement with previous results (2015/2016) with Aerosil 200V in distilled water using 10% and 15% w:w 200V.

As bead fill ratio is increased from 45% to 65%

► break-up rate (as defined through the % volume of “fines” in total PSD) appears independent of fill ratio

► confirmed when fines % expressed in terms of cumulative residence time (RT) in mill

Fines % is possibly faster at higher Aerosil concentrations

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© BHR Group 2017 47

Possible Future Work with WAB Mill

Suggestions for Members?

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www.bhrgroup.com © BHR Group 2017

The experimental work was performed by Brian Perkins

Thank you for your attention

Dr Nigel Heywood

[email protected] Mobile: +44 7847 627044

Direct dial: +44 (0) 330 119 19 87