foams of polyurethane/mwnt nanocomposites for efficient emi … l... · 2009-10-08 · prepared by...

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Introduction Introduction Introduction Introduction Due to the steady growth of communication technology and the adverse effects of electromagnetic radiations on the human body and electronic devices, it is critical to reduce the electromagnetic interference (EMI) and its impact on medical apparatus and electronic engineering. In that context, polymer/multi-walled carbon nanotubes (MWNT) nanocomposites are proposed for their high EMI shielding performance. 1-11 The strategy is to render the polymer conductive by adding MWNTs and to promote wave absorption by foaming the polymer-based composite. These MWNT/PU polymeric foams thus show a promising EMI shielding efficiency due to their high capacity to absorb electromagnetic radiation at low MWNT content. Foams of Polyurethane/MWNT Nanocomposites Foams of Polyurethane/MWNT Nanocomposites Foams of Polyurethane/MWNT Nanocomposites Foams of Polyurethane/MWNT Nanocomposites for Efficient EMI Reduction for Efficient EMI Reduction for Efficient EMI Reduction for Efficient EMI Reduction Y.Y. Chen, Y.Y. Chen, Y.Y. Chen, Y.Y. Chen, a,b a,b a,b a,b L. Urbanczyk, L. Urbanczyk, L. Urbanczyk, L. Urbanczyk, a J-M. Thomassin, M. Thomassin, M. Thomassin, M. Thomassin, a C. Detrembleur, C. Detrembleur, C. Detrembleur, C. Detrembleur, a C. Jerome C. Jerome C. Jerome C. Jerome a a Center for Education and Research on Macromolecules (CERM), University of Liege, Sart-Tilman, B6, 4000 Liege, Belgium. b FAME, Institut Polytechnique de Grenoble, Grenoble 38031, France. [email protected] 4. Electrical properties High electrical conductivity is directly related to good EMI shielding effectiveness, while low permittivity is required in order to avoid wave reflection and promote wave absorption. Therefore, accurate foaming conditions must be found to reach both high conductivity and low permittivity. 2. Nanocomposite preparation 1 and 2 wt% MWNT (NC7000, Nanocyl™, Belgium)/PU(Desmopan 2590A, Bayer, Germany) composites were prepared by melt blending in a twin-screw internal mixer (180°C, 60 rpm, 5 min) and then molded into 2mm thick sheets under a hot press (180°c) for 5min. Fig 1: a) Behavior of nanocomposite foams under EMI radiation, b) difference between an EMI shield by reflection and by absorption. The MWNT/polymer foam can effectively protect an electronic device from waves interference thanks to its capacity to absorb the waves instead of reflecting them. Fig 2: Schematic representation of the two-steps batch foaming process with CO 2 . Fig 3: Characterization of non-foamed MWNT/PU nanocomposites; a) homogeneous dispersion of MWNTs observed by TEM, b) rheological behavior of pure PU and PU/MWNT nanocomposites with an increasing MWNT content. a) MWNTs are very well-dispersed within PU matrix. The percolation threshold is reached with a low carbon nanotubes loading (1wt%), as proved by rheological analysis. In fact, the nanocomposites show solid-like behavior at low frequency range. 10 0 10 1 10 2 10 3 10 4 10 5 storage modulus (Pa )2 4 6 8 0.1 2 4 6 8 1 2 4 6 8 10 frequency (Hz )PU PU+1%MWNT PU+2%MWNT b )Effect of MWNT addition on electrical properties 1. Absorption of electromagnetic waves 3. Nanocomposite foams preparation The nanocomposite is saturated in scC 2 for 24h at 40°C and 60-300bar. The vessel is then quickly depressurized and the sample is transferred in a hot press (120°C) for 2min in order to allow cell EMI shield by reflection EMI shield by absorption High pressure vessel Polymer sample Polymer/gas solution Saturation with scCO 2 Fast release of gas No foaming (too low T°) Bubble nucleation and growth Hot silicon bath Foam quenched Size stabilized Cold water/ice bath High pressure vessel Polymer sample Polymer/gas solution Saturation with scCO 2 Fast release of gas No foaming (too low T°) Bubble nucleation and growth Hot silicon bath Foam quenched Size stabilized Cold water/ice bath Conclusions Conclusions Conclusions Conclusions MWNT/PU composites with an uniform porous structure have been successfully prepared by melt blending and accordingly foamed with scC 2 . We have shown that the cellular morphology and foam density can be controlled by varying the foaming parameters. The electrical properties, which are directly related to EMI shielding effectiveness, are improved by adding MWNTs (conductivity) and foaming (permittivity). Although the results obtained here still need optimization in order to be competitive, these MWNT/PU polymeric foams are very promising EMI shielding materials due to their high capacity to absorb electromagnetic radiation at low MWNT content. References References References References 1 Thomassin, J.M. Pagnoulle, C. Bednarz, L. Huynen, I. Jerome, R. Detrembleur, C. J. Mater. Chem. 2008 2008 2008 2008, 18, 2. 2 Yuen, S.M. Ma, C.C.M. Chuang, C.Y. Yu, .C. Wu, S.Y. Yang, C.C. Wei, M.H. Compos. Sci. Technol. 2008 2008 2008 2008, 68, 63. 3 Huynen, I. Bednarz, L. Thomassin, J.M. Pagnoulle, C. Jerome, R. Detrembleur, C. in 2008 38th European Microwave Conference, IEEE, 2008 2008 2008 2008, 5. 4 J r me, R. Pagnoulle, Detrembleur, C. Thomassin, J.-M. Huynen, I. Bailly, C. Bednarz, L. Daussin, R. Saib, A. Baudouin, A.-C. Laloyaux . PCT Int. Appl. 2008 2008 2008 2008, W 2008068042. 5 Thomassin, J.M. Lou, . Pagnoulle, C. Saib, A. Bednarz, L. Huynen, I. Jerome, R. Detrembleur, C. J. Phys. Chem. C , 200 200 200 200 , 111, 11186. 6 hang, C.S. Ni, . . Fu, S.Y. urashiki, . Compos. Sci. Technol. 200 200 200 200 , 6 , 2 3. Yang, Y.L. Gupta, M.C. Dudley, .L. Lawrence, R.W. J. Nanosci. Nanotechnol. 200 200 200 200 , , 54 . 8 Saib, A. Bednarz, L. Daussin, R. Bailly, C. Lou, . Thomassin, J.M. Pagnoulle, C. Detrembleur, C. Jerome, R. Huynen, I. IEEE Trans. Microw. Theory Tech. 2006 2006 2006 2006, 54, 2 45. Yang, Y.L. Gupta, M.C. Dudley, .L. Lawrence, R.W. Adv. Mater. 2005 2005 2005 2005, 1 , 1 . 10 8 6 4 2 permittivity 26x10 9 24 22 20 18 16 14 frequency (Hz )d=1090 kgm^-3 d=480 kgm^-3 d=460 kgm^-3 d=300 kgm^-3 b )1.0 0.8 0.6 0.4 0.2 concuctivity (S/m )26x10 9 24 22 20 18 16 14 frequecy (Hz )d=1090 kgm^-3 d=480 kgm^-3 d=460 kgm^-3 d=300 kgm^-3 a )Effect of foam density on electrical properties PU/2wt%MWNT Effect of foaming conditions and MWNT content on cell size and foam density Effect of MWNT addition on cellular morphology 0.4 0.3 0.2 0.1 0.0 conductivity (S/m )26x10 9 24 22 20 18 16 14 frequency (Hz) PU PU+1%MWNT PU+2%MWNT a )Fig. 4: Porous structure of a) pure PU and b) PU/2%MWNT observed by SEM. C) Cell size distribution of pure PU and nanocomposite foams. 7 6 5 4 3 2 cell diameter (um) 300 250 200 150 100 P(Pa) PU PU+1%MWNT PU+2%MWNT a) Effect of MWNT addition on electrical properties The composites foams have smaller cell size and narrower cell size distribution compared to neat PU foam. The nanofiller acts as a heterogeneous nucleating agent, increasing the cell density. 4.0 3.5 3.0 2.5 2.0 1.5 1.0 premittivity 26x10 9 24 22 20 18 16 14 Frequency (Hz )PU PU+1%MWNT PU+2%MWNT b )Fig 6: a) Conductivity and b) permittivity of pure and nanocomposite foams (d~0.4 g/cm³) as a function of wave frequency. Fig 7: a) Conductivity and b) permittivity of PU/2wt%MWNT foams as a function of foam density. Foams with lower density lead to low permittivity, high absorption, and low conductivity. Decreasing the foam density leads to lower permittivity but also to lower conductivity (lower EMI shielding effectiveness). The carbon nanotube content as well as foaming conditions must therefore be optimized in order to find a compromise between high conductivity and low permittivity, which will result in excellent EMI shielding performance. a) PU b) PU+2%MWNT depressurized and the sample is transferred in a hot press (120°C) for 2min in order to allow cell growth. The foam is finally quenched in an ice/water bath. 0 5 10 15 20 25 30 35 40 45 50 1 1,4 1,8 2,2 2,6 3 3,4 3,8 4,2 4,6 5 5,4 5,8 6,2 6,6 7 7,4 Cell size (μm) Fraction % PU PU/1%MWNT PU/2%MWNT 450 400 350 300 250 density(kg*m^-3) 300 250 200 150 100 P(Pa) PU PU+1%MWNT PU+2%MWNT b) While pure PU foam is isolative, MWNT addition renders the foam conductive, but it also increases the foam permittivity. The effect is more pronounced at 2wt% loading. Acknowledgements Acknowledgements Acknowledgements Acknowledgements The authors are grateful for the financial support to BELSPO, in the frame of network IAP 6/27 and to the “Région Wallonne” for its financial support in the frame of the MULTIMASEC project. Y-Y. Chen thanks the FAME program. C.D. is “Maître de Recherche” by F. R. S.-FNRS, Belgium and J-M. Thomassin is “Chercheur Scientifique Logistique post-doctoral” by F. R. S.-FNRS. P (bar) Fig 5: a) cell diameter decreases with increase of saturation pressure and MWNT content, b) foam density decreases and then increases with the pressure and is higher for nanocomposite foams. P (bar)

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Page 1: Foams of Polyurethane/MWNT Nanocomposites for Efficient EMI … L... · 2009-10-08 · prepared by melt blending in a twin-screw internal mixer (180°C, 60 rpm, 5 min) and then molded

IntroductionIntroductionIntroductionIntroductionDue to the steady growth of communication technology and the adverse effects of electromagnetic radiations on the human body and electronic devices, it is critical to reduce the electromagnetic interference (EMI) and its impact on medical apparatus and electronic engineering. In that context, polymer/multi-walled carbon nanotubes (MWNT) nanocomposites are proposed for their high EMI shielding performance.1-11 The strategy is to render the polymer conductive by adding MWNTs and to promote wave absorption by foaming the polymer-based composite. These MWNT/PU polymeric foams thus show a promising EMI shielding efficiency due to their high capacity to absorb electromagnetic radiation at low MWNT content.

Foams of Polyurethane/MWNT Nanocomposites Foams of Polyurethane/MWNT Nanocomposites Foams of Polyurethane/MWNT Nanocomposites Foams of Polyurethane/MWNT Nanocomposites for Efficient EMI Reductionfor Efficient EMI Reductionfor Efficient EMI Reductionfor Efficient EMI Reduction

Y.Y. Chen,Y.Y. Chen,Y.Y. Chen,Y.Y. Chen,a,ba,ba,ba,b L. Urbanczyk,L. Urbanczyk,L. Urbanczyk,L. Urbanczyk,aaaa JJJJ----M. Thomassin, M. Thomassin, M. Thomassin, M. Thomassin, a C. Detrembleur,C. Detrembleur,C. Detrembleur,C. Detrembleur,aaaa C. JeromeC. JeromeC. JeromeC. Jeromeaaaaa Center for Education and Research on Macromolecules (CERM), University of Liege, Sart-Tilman, B6, 4000 Liege, Belgium.

b FAME, Institut Polytechnique de Grenoble, Grenoble 38031, France. [email protected]

4. Electrical propertiesHigh electrical conductivity is directly related to good EMI shielding effectiveness, while lowpermittivity is required in order to avoid wave reflection and promote wave absorption. Therefore,accurate foaming conditions must be found to reach both high conductivity and low permittivity.

2. Nanocomposite preparation1 and 2 wt% MWNT (NC7000, Nanocyl™, Belgium)/PU(Desmopan 2590A, Bayer, Germany) composites were prepared by melt blending in a twin-screw internal mixer (180°C, 60 rpm, 5 min) and then molded into 2mm thick sheets under a hot press (180°c) for 5min.

Fig 1: a) Behavior of nanocomposite foams under EMI radiation, b) difference between an EMI shield by reflection and by absorption.

The MWNT/polymer foam can effectively protect an electronic device from waves interference thanks to its capacity to absorb the waves instead of reflecting them.

Fig 2: Schematic representation of the two-steps batch foaming process with CO2.

Fig 3: Characterization of non-foamed MWNT/PU nanocomposites; a) homogeneous dispersion of MWNTs observed by TEM, b) rheological behavior of pure PU and PU/MWNT nanocomposites with an increasing MWNT content.

a)

� MWNTs are very well-dispersed within PU matrix.� The percolation threshold is reached with a low carbon nanotubes loading(1wt%), as proved by rheological analysis.In fact, the nanocomposites show solid-like behavior at low frequency range.

100

101

102

103

104

105

stor

age

mod

ulus

(Pa

)

2 4 6 80.1

2 4 6 81

2 4 6 810

frequency (Hz )

PUPU+1%MWNTPU+2%MWNT

b )

Effect of MWNT addition on electrical properties

1. Absorption of electromagnetic waves

3. Nanocomposite foams preparationThe nanocomposite is saturated in scC 2 for 24h at 40°C and 60-300bar. The vessel is then quicklydepressurized and the sample is transferred in a hot press (120°C) for 2min in order to allow cell

EMI shield by reflection EMI shield by absorption

High pressurevessel

Polymer sample Polymer/gassolution

Saturation withscCO2

Fast release of gas

No foaming(too low T°)

Bubble nucleationand growth

Hot silicon bath

Foam quenched����Size stabilized

Cold water/ice bathHigh pressure

vessel

Polymer sample Polymer/gassolution

Saturation withscCO2

Fast release of gas

No foaming(too low T°)

Bubble nucleationand growth

Hot silicon bath

Foam quenched����Size stabilized

Cold water/ice bath

Conclusions Conclusions Conclusions Conclusions MWNT/PU composites with an uniform porous structure have been successfully prepared by melt blending and accordingly foamed with scC 2. We have shown that the cellular morphology and foam density can be controlled by varying the foaming parameters. The electrical properties, which are directly related to EMI shielding effectiveness, are improved by adding MWNTs (conductivity) and foaming (permittivity). Although the results obtained here still need optimization in order to be competitive, these MWNT/PU polymeric foams are very promising EMI shielding materials due to their high capacity to absorb electromagnetic radiation at low MWNT content.References References References References 1 Thomassin, J.M. Pagnoulle, C. Bednarz, L. Huynen, I. Jerome, R. Detrembleur, C. J. Mater. Chem. 2008200820082008, 18, 2.

2 Yuen, S.M. Ma, C.C.M. Chuang, C.Y. Yu, .C. Wu, S.Y. Yang, C.C. Wei, M.H. Compos. Sci. Technol. 2008200820082008, 68, 63.

3 Huynen, I. Bednarz, L. Thomassin, J.M. Pagnoulle, C. Jerome, R. Detrembleur, C. in 2008 38th European Microwave Conference, IEEE, 2008200820082008, 5. 4 J r me, R. Pagnoulle, Detrembleur, C. Thomassin, J.-M. Huynen, I. Bailly, C. Bednarz, L. Daussin, R. Saib, A. Baudouin, A.-C. Laloyaux . PCT Int. Appl. 2008200820082008, W

2008068042.

5 Thomassin, J.M. Lou, . Pagnoulle, C. Saib, A. Bednarz, L. Huynen, I. Jerome, R. Detrembleur, C. J. Phys. Chem. C , 200200200200 , 111, 11186.

6 hang, C.S. Ni, . . Fu, S.Y. urashiki, . Compos. Sci. Technol. 200200200200 , 6 , 2 3.

Yang, Y.L. Gupta, M.C. Dudley, .L. Lawrence, R.W. J. Nanosci. Nanotechnol. 200200200200 , , 54 . 8 Saib, A. Bednarz, L. Daussin, R. Bailly, C. Lou, . Thomassin, J.M. Pagnoulle, C. Detrembleur, C. Jerome, R. Huynen, I. IEEE Trans. Microw. Theory Tech. 2006200620062006, 54, 2 45.

Yang, Y.L. Gupta, M.C. Dudley, .L. Lawrence, R.W. Adv. Mater. 2005200520052005, 1 , 1 .

10

8

6

4

2

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ittivi

ty

26x109242220181614frequency (Hz )

d=1090 kgm -̂3d=480 kgm -̂3d=460 kgm -̂3d=300 kgm -̂3

b )1.0

0.8

0.6

0.4

0.2

conc

uctiv

ity

(S/m

)

26x109242220181614frequecy (Hz )

d=1090 kgm -̂3d=480 kgm -̂3d=460 kgm -̂3d=300 kgm -̂3

a )

Effect of foam density on electrical properties PU/2wt%MWNT

Effect of foaming conditions and MWNT content on cell size and foam density

Effect of MWNT addition on cellular morphology 0.4

0.3

0.2

0.1

0.0

cond

uctiv

ity

(S/m

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26x109242220181614frequency (Hz)

PUPU+1%MWNTPU+2%MWNT

a )

Fig. 4: Porous structure of a) pure PU and b) PU/2%MWNT observed by SEM. C) Cell size distribution of pure PU and nanocomposite foams.

7

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4

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2

cell

diam

eter

(um

)

300250200150100P(Pa)

PUPU+1%MWNTPU+2%MWNT

a)

Effect of MWNT addition on electrical properties

� The composites foams have smaller cell size and narrower cell size distribution compared to neat PU foam. �The nanofiller acts as a heterogeneous nucleating agent, increasing the cell density.

4.0

3.5

3.0

2.5

2.0

1.5

1.0

prem

ittiv

ity

26x109

242220181614Frequency (Hz )

PUPU+1%MWNTPU+2%MWNT

b )

Fig 6: a) Conductivity and b) permittivity of pure and nanocomposite foams (d~0.4 g/cm³) as a function of wave frequency.

Fig 7: a) Conductivity and b) permittivity of PU/2wt%MWNT foams as a function of foam density. Foams with lower density lead to low permittivity, high absorption, and low conductivity.

Decreasing the foam density leads to lower permittivity but also to lower conductivity (lower EMI shielding effectiveness). The carbon nanotube content as well as foaming conditions must therefore be optimized in order to find a compromise between high conductivity and low permittivity, which will result in excellent EMI shielding performance.

a) PU b) PU+2%MWNT

depressurized and the sample is transferred in a hot press (120°C) for 2min in order to allow cellgrowth. The foam is finally quenched in an ice/water bath.

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PU/1%MWNT

PU/2%MWNT

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300250200150100P(Pa)

PUPU+1%MWNTPU+2%MWNT

b)

While pure PU foam is isolative, MWNT addition renders the foam conductive, but it also increases the foam permittivity. The effect is more pronounced at 2wt% loading.

Acknowledgements Acknowledgements Acknowledgements Acknowledgements The authors are grateful for the financial support to BELSPO, in the frame of network IAP 6/27 and to the “Région Wallonne” for its financial support in the frame of the MULTIMASEC project. Y-Y. Chen thanks the FAME program. C.D. is “Maître de Recherche” by F. R. S.-FNRS, Belgium and J-M. Thomassin is “Chercheur Scientifique Logistique post-doctoral” by F. R. S.-FNRS.

P (bar)Fig 5: a) cell diameter decreases with increase of saturation pressure and MWNT content, b) foam density decreases and then increases with the pressure and is higher for nanocomposite foams.

P (bar)