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www.bhrgroup.com BHR Group is a trading name of VirtualPiE Limited © BHR Group 2015
Deagglomeration of Carbon Black Dispersions Using the Ultrasonicator
Dr Gül Özcan-Taşkın [email protected] Mobile: +44 (0) 77856 21659
Direct dial: +44 (0) 330 119 19 01
23- 24 September 2015 DOMINO Autumn Meetings
Confidential to DOMINO Members
© BHR Group 2015 19-20/05/2015 2
Introduction- Background
During 2014 project meetings, DOMINO members were invited to make propositions for new materials to be used within DOMINO
Carbon black and graphite were materials favoured by members during September 2014 Meetings
© BHR Group 2015 19-20/05/2015 3
Materials
Two pre-dispersions of carbon black were received from membership to be processed using energy intensive devices: N134 and N234
These materials are typically used to reinforce natural and synthetic rubber products
The pre-dispersions were prepared by using a batch rotor-stator following the same protocol, i.e. under the same operating conditions
Particle concentration is 4% w:w for both
© BHR Group 2015 19-20/05/2015 4
Introduction- Objectives and scope of work
The overall objectives of the WP have been to assess
► the fineness of carbon black dispersions obtained using power intensive process devices and
► the kinetics of deagglomeration and stability of carbon black dispersions
Two carbon black dispersions were processed using the Microfluidizer M110-P and reported during May Meetings. One of these is now processed using the ultrasonicator.
© BHR Group 2015 5
Background- Microfluidizer M-110P
Z type interaction chamber: for deagglomeration; auxillary chamber upstream
Generic images obtained from Microfluidics website
© BHR Group 2015 8
Results- Power input
Pt
VP
i
i
P - power, W
Vi - volume of impulse, m3
ti - time of impulse, s
P - pressure drop, Pa
Pressure Power P/m*
(psi) (M Pa) (W) (W/kg)
5000 35 146 29333
10000 69 416 78146
20000 138 1471 249441
* based on mass per pulse (4.9- 5.9 ml)
© BHR Group 2015 9
Results- Power input
Pt
VP
i
i
P - power, W
Vi - volume of impulse, m3
ti - time of impulse, s
P - pressure drop, Pa
Pressure Power P/m*
(psi) (M Pa) (W) (W/kg)
5000 35 146 29333
10000 69 416 78146
20000 138 1471 249441
* based on mass per pulse (4.9- 5.9 ml)
© BHR Group 2015 10
Results- Power input
Process device
P (W)
Mass (kg) considered
P/m (W/kg)
In-line rotor-stator 60- 3600 100 0.6- 35.5
Ultrasonicator 55- 90 2 27.5- 45
Microfluidizer* 148- 1469 0.006** 2.9x104- 2.5x105
*4897 W/kg for 300 ml dispersion ** Pulse volume
© BHR Group 2015 19-20/05/2015 11
Conclusions (May 2015)
There are minor differences in terms of PSD between the two pre-dispersions supplied : N134 and N234
Break up appears to occur through rupture
Very little change in size noted during processing. Comparable final size range with both dispersions : ~2 to 20 µm
N234 dispersion reaches the finest size in 1 pass, N134 takes 4 passes and appears to be slightly coarser than N234.
Dispersions are stable over the 4 months tested
© BHR Group 2015 19-20/05/2015 12
Comparison of the pre-dispersions
0
1
2
3
4
5
6
7
8
1 10 100
Vo
lum
e %
Diameter (Microns)
N234
N134
PSDs of the two pre-dispersions are comparable
© BHR Group 2015 19-20/05/2015 13
Conclusions (May 2015)
There are minor differences in terms of PSD between the two pre-dispersions supplied : N134 and N234
Break up appears to occur through rupture
Very little change in size noted during processing. Comparable final size range with both dispersions : ~2 to 20 µm
N234 dispersion reaches the finest size in 1 pass, N134 takes 4 passes and appears to be slightly coarser than N234.
Dispersions are stable over the 4 months tested
© BHR Group 2015 19-20/05/2015 14
Deagglomeration of N134 dispersion using the Microfluidizer
0
1
2
3
4
5
6
7
8
9
10
0.5 5 50 500
Vo
lum
e %
Diameter (Microns)
pre-dispersion1 pass2 pass3 pass4 pass
Following on from a significant size reduction after 1 pass, further break up occurs gradually during further passes through what appears to be a rupture type break up
© BHR Group 2015 19-20/05/2015 15
0
1
2
3
4
5
6
7
8
9
10
1 10 100
Vo
lum
e %
Diameter (Microns)
pre-dispersion1 pass2 pass3 pass
Deagglomeration of N234 dispersion using the Microfluidizer
Single pass through the Microfluidizer is sufficient to obtain the finest possible dispersion with this formulation.
© BHR Group 2015 19-20/05/2015 16
Conclusions (May 2015) and future work
There are minor differences in terms of PSD between the two pre-dispersions supplied : N134 and N234
Break up appears to occur through rupture
Very little change in size noted during processing. Comparable final size range with both dispersions : ~2 to 20 µm
N234 dispersion reaches the finest size in 1 pass, N134 takes 4 passes and appears to be slightly coarser than N234.
Further work can be performed using
► the ultrasonicator and
► with a dispersing agent
© BHR Group 2015 19-20/05/2015 17
Comparison of final PSDs
0
1
2
3
4
5
6
7
8
9
10
1 10 100
Vo
lum
e %
Diameter (Microns)
Final
N234
N134
© BHR Group 2015 19-20/05/2015 22
N234 (before processing) SEM Micrographs
© BHR Group 2015 19-20/05/2015 23
N234 (before processing) SEM Micrographs (2)
© BHR Group 2015 19-20/05/2015 24
N234 (after processing) SEM Micrographs
© BHR Group 2015 19-20/05/2015 25
N234 (after processing) SEM Micrographs
© BHR Group 2015 19-20/05/2015 26
Conclusions (May 2015) and future work
There are minor differences in terms of PSD between the two pre-dispersions supplied : N134 and N234
Break up appears to occur through rupture
Very little change in size noted during processing. Comparable final size range with both dispersions : ~2 to 20 µm
N234 dispersion reaches the finest size in 1 pass, N134 takes 4 passes and appears to be slightly coarser than N234.
Dispersions are stable over the 4 months tested
© BHR Group 2015 19-20/05/2015 27
Comparison of Sauter mean diameters
0
2
4
6
8
10
12
14
0 0.5 1 1.5 2 2.5 3 3.5 4
N134
N234
Nb of passes
d3
2 (
µm
)
© BHR Group 2015 19-20/05/2015 28
Conclusions (May 2015)
There are minor differences in terms of PSD between the two pre-dispersions supplied : N134 and N234
Break up appears to occur through rupture
Very little change in size noted during processing. Comparable final size range with both dispersions : ~2 to 20 µm
N234 dispersion reaches the finest size in 1 pass, N134 takes 4 passes and appears to be slightly coarser than N234.
Dispersions are stable over the 4 months tested
© BHR Group 2015 19-20/05/2015 30
N234 Ageing of Samples
0
1
2
3
4
5
6
7
8
9
10
0.1 1 10 100 1000
Vo
lum
e %
Diameter (Microns)
N234 - fresh
N234 - 4 months
Dispersions are stable over the 4 months period tested.
© BHR Group 2015 19-20/05/2015 31
Conclusions (May 2015) and future work
There are minor differences in terms of PSD between the two pre-dispersions supplied : N134 and N234
Break up appears to occur through rupture
Very little change in size noted during processing. Comparable final size range with both dispersions : ~2 to 20 µm
N234 dispersion reaches the finest size in 1 pass, N134 takes 4 passes and appears to be slightly coarser than N234.
Dispersions are stable over the 4 months tested
Further work can be performed using
► the ultrasonicator and
► with a dispersing agent
© BHR Group 2015 19-20/05/2015 32
Contents
Introduction- background
Experimental
► Equipment
► Materials
Results and discussions
Conclusions and future work
© BHR Group 2015 33
Experimental set up
N234 was processed using the ultrasonic processor Hielscher
UP200S Ultrasound Disperser (24 kHz )
Titanium, 14 mm diameter sonotrode
100% Amplitude
Calculated power output: ~89 W
Total mass of dispersion: ~ 180 mg
P/V = ~ 494 W/kg
Samples taken at pre-determined time intervals
© BHR Group 2015 34
Particle Size Distribution Measurements
Beckman Coulter LS230
Laser diffraction (0.4 – 2000 mm) + PIDS (Polarization Intensity Differential Scattering) (0.04 – 0.4 mm)
Refractive index for carbon black: 1.84+0.85i
(ASTM Carbon Black Reference Materials: Particle Sizing Using a Brookhaven Instruments BI-DCP, Disc Centrifuge Photosedimentometer by W. W. Tscharnuter, L. Zu, Bruce B. Weiner)
PSD measurements:
► on fresh samples then
► after 24 h
© BHR Group 2015 35
Evolution of PSD in time using the ultrasonicator
0
1
2
3
4
5
6
7
8
9
0.5 5 50 500
Dif
fere
nti
al V
olu
me
, %
Particle Diameter, Microns
4% Carbon black (N234) with ultrasonicator at 100% amplitude
t= 0 min
t= 2.5 min
t= 5 min
t= 10 min
t= 60 min
Insignificant change in PSD over a period of 60 min processing- in line with findings with Microfluidizer
© BHR Group 2015 36
Evolution of d32 in time
6
7
8
9
10
11
12
0 10 20 30 40 50 60 70
4% Carbon black(N234) with ultrasonicator at 100%
Processing time (min)
d3
2 (m
icro
ns)
© BHR Group 2015 37
Results of ageing test
6
7
8
9
10
11
12
0 10 20 30 40 50 60 70
4% Carbon black(N234) with ultrasonicator at 100%
N234- u-s
24 h aged
Processing time (min)
d3
2 (m
icro
ns)
The dispersions maintain their properties as also observed with those obtained with the Microfluidizer
© BHR Group 2015 38
Ageing test: PSD after 24 hours
0
1
2
3
4
5
6
7
8
9
0.5 5 50 500
Dif
fere
nti
al V
olu
me
, %
Particle Diameter, Microns
4% Carbon black (N234) with ultrasonicator at 100% amplitude
t= 0 min
t= 60 min
24 h ageing
© BHR Group 2015 39
Comparison with the Microfluidizer
0
1
2
3
4
5
6
7
8
9
10
1 10 100 1000
Dif
fere
nti
al V
olu
me
, %
Particle Diameter, Microns
4% Carbon black (N234) comparison of u-s and Microfluidizer
t= 0 August 2015 U-S
t= 0 April2015 MF
U-S 60 min
MF 3rd pass
© BHR Group 2015 40
Comparison with the Microfluidizer
5
6
7
8
9
10
11
12
13
14
15
0 5 10 15 20 25 30
4% Carbon black(N234)- Ultrasonicator and Microfluidizer
N234- u-s N234 MF
Processing time (min)
d3
2 (m
icro
ns)
© BHR Group 2015 41
Concluding remarks and future work
Two carbon black dispersions were processed using two power intensive process devices: Microfluidizer M-110P and the ultrasonicator.
This allowed a specific power input of ~500- 5000W/kg to be covered.
Very little change in PSD was noted during processing.
The samples were stable over the period tested.
These results provide a baseline for future work to study the effect of formulation.
© BHR Group 2015 19-20/05/2015 42
Acknowledgements
The work was performed by Brian Perkins
www.bhrgroup.com BHR Group is a trading name of VirtualPiE Limited © BHR Group 2015
Thank you
Dr Gül Özcan-Taşkın
[email protected] Mobile: +44 77856 21659
Direct dial: +44 (0) 330 119 19 01