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Journal Club Theme of Jan. 15 2008: Active Nanocomposites

Active or smart materials are materials that exhibit couplings between multiple physical domains, such as mechanical and electrical—piezoelectric materials, or thermal and mechanical—as in shape memory alloys and polymers. Nanotechnology may offer opportunities to reenergize the area of smart materials by addressing current shortfalls and expanding the scope of available material space. Some scholars in the mechanics community have focused on nanocomposites to elucidate and predict the level of mechanical enhancement that nanoparticles such as carbon nanotubes can bring to polymers and composites. In general, researchers agree that the internal interfacial area in nanocomposites, rather than the relative volume fraction of constituents, is the critical characteristic that is crucial in explaining and determining this enhancement. There is a need and opportunity for mechanicians and materials scientists to come together and investigate the less-studied area of electrical and electromechanical enhancement in polymer nanocomposites.

T. J. Lewis laid out the theoretical work for such an opportunity (TJ Lewis ‘Interfaces: nanometric dielectrics’ Journal of Physics D: Appl Phys 38, pp202-212, 2005). Lewis raises the possibility that the presence of nanoparticles in polymers can give rise to electromechanical coupling not otherwise present in the pristine polymer. Further, he stresses the role of the interface, where properties, whether mechanical, electrical or coupled, will have their origin in the behavior of the interfacial interaction zone. This increasingly dominating interface is a seat of polarization and charge separation, which can take on a passive or an active role. In a passive interface, the macroscopic property of interest is the effective dielectric permittivity which can be analyzed using a number of methods based on Maxwell-Garnett. In an active interface, the application of an electric field induces a mechanical stress. The coupling results in piezoelectric and electrostrictive phenomena, and arises from the co-operative behavior of nanoscale interfaces. In continuum mechanics, the interface in nanocomposites has in some cases been considered to be a third phase with its own mechanical properties. Lewis suggests that this third phase also possesses its own dielectric and hence electrostrictive behavior, which can be “activated” under the application of a strong field.

The promise of unique electrical and dielectric properties in nano-filled materials inspired Nelson et al. (JK Nelson and Y Hu, ‘Nanocomposite dielectrics-properties and implications’ Journal of Physics D: Appl Phys 38, pp213-222, 2005) to investigate polymer nanocomposite dielectrics. These researchers saw improvement in dielectric properties, such as orders of magnitude increase in voltage endurance and dielectric strength, which they attribute to bonding at the interface, and to the formation of a double layer in the interfacial region which influences space charge distribution.

More recently, Owens et al. (FJ Owens, JRP Jayakody, SG Greenbaum, ‘Characterization of single walled carbon nanotube:polyvinylene difluoride composites’, Composites Science and Technology 66, pp1280-84, 2006) reported an electron donor-acceptor interaction between single wall carbon nanotube and the fluorine dipole in PVDF, offering an experimental evidence of induced polarization at the interface of a nanocomposite. These two examples suggest that the interfacial zone, in addition to being the area of particle-polymer bonding, plays an important role in determining the dielectric behavior of the composite.

Dielectric nanocomposites afford us opportunities to extend our exploration of interfaces beyond mechanical properties. Our increased understanding of the role of the interface in polymer nanocomposites would allow us to engineer materials with a prescribed dielectric behavior, or to tailor active materials to yield desired performance such as low actuation voltage, high electromechanical strain, and fast response time. While the three papers proposed (listed again below) are meant to initiate a discussion on the impact of nanocomposites as either passive or active dielectrics, any discussion on the potential of nanocomposites beyond mechanical reinforcement is welcome.

  1. TJ Lewis ‘Interfaces: nanometric dielectrics’ Journal of Physics D: Appl Phys 38, pp202-212, 2005
  2. JK Nelson and Y Hu, ‘Nanocomposite dielectrics-properties and implications’ Journal of Physics D: Appl Phys 38, pp213-222, 2005
  3. FJ Owens, JRP Jayakody, SG Greenbaum, ‘Characterization of single walled carbon nanotube:polyvinylene difluoride composites’, Composites Science and Technology 66, pp1280-84, 2006

Comments

Actually, studying the dielectric properties of nanocomposites, and more precisely the carbon nanotubes (CNT)-polymer nanocomposites, is gaining more attention due to the extraordinary properties of the CNTs. And as you mentioned, the big part of the enhancement comes from the interface since the surface area between the matrix and the nano-fillers is really important. I came across a paper, written by Q.Z. Xue et al. that presents a model that predicts the effective electrical conductivity of CNT-composites incorporating the interface effect (KY Yan, QZ Xue, QB Zheng and LZ Hao ‘The interface effect of the effective electrical conductivity of carbon nanotube composites' Nanotechnology 18 (2007) 255705 (6pp)). In this model, based on average field theory, the interface is considered as a third phase having its own properties.

The large disparity in properties between carbon nanotubes and the polymers in which they are often imbedded leads to large expectations in terms of the effective properties the resulting nanocompiste, particularly when using 'back of the envelope' calculations such as the rule of mixtures.  However, characterization efforts have often found that the measured properties for nanocomposites are not as predicted by such methods.  This has certainly been the case in terms of the elastic properties and thermal and electrical conductivities where interface effects have been identified as potentially having a large influence on the nanocomposite properties; the elastic properties being influenced by weak van der Waals interactions, the thermal properties influenced by an interface thermal resistance, and the electrical properties influenced by electron hopping which may be treated as an interface.  In our recent efforts on modeling nanocomposites on the micromechanics level, we have certainly seen the potential for such interface effects to have a large influence on the effective properties. As most of the interface of the nanotube is along its axis, this seems to further emphasize the importance of being able to control nanotube alignment or orientation. However, regardless of nanotube orientation, the question we have often been faced with is what exactly the properties of the interface are and how can they measured?  At present, some of these properties can be assessed using lower length scale (atomistic) simulations, but this can not perfectly substitute for a direct physical measurement.  Thus it will certainly be interesting to me to see how not only the progress in modeling and characterizing the nanocomposite dielectric properties in terms of the influence of the interface, but also to see what strategies exist for probing these properties in the lab.

Amira and Gary, Thank you for the interesting references. Indeed, it seems one aspect of nanocomposite characterization that can move modeling forward is developing experimental means to probe the interface. As both of you pointed out, modeling the interface as a third phase is an option but it is still not clear what properties/characteristics should be prescribed. Certainly, researchers have used spectroscopy such as Raman and FTIR (such as in the Owens et al. paper I mentioned above) to probe the nanoparticle-polymer interaction. Those results may allow us to ‘qualify’ the type of interface but cannot yield to ‘quantification’.

Frank Fisher's picture

Another effect regarding the interface/interphase region in semi-crystalline polymer nanocomposites that I am now just starting to really appreciate is the impact that the nanoparticles can have on both the level of crystallinity as well as the crystal polymorphs present in the nanocomposite. To expand on the previous thoughts in this blog, this raises the very interesting question of how to distinguish/differentiate the effects of changes in crystallinity versus interface/interphase effects (such as an annular region ofrestricted mobility polymer due to interactions with the nanoparticle) versus the actual effects of the actual nanoinclusion itself on the effective nanocomposite properties.

For example, a paper from the Giannelis group in Advanced Materials in 2004 (see below) showed that the addition of appropriately surface-modified nanoparticles (5 wt% nanoclay) in PVDF resulted in an order-of-magnitude increase in toughness of the polymer. This large toughness enhancement was largely attributed to an increase in the amount of beta phase (at the expense of the alpha phase) of the semicrystalline PVDF present in the nanocomposite. Because the piezoelectric properties of PVDF are largely attributed to the beta crystal phase, this offers some interesting possibilities regarding using nanoparticles to control crystal morphologies and phase in these types of nanocomposites.

If you’re further interested in this work I would very highly recommend the article highlighted above and given below, and the references therein...

D Shah, P.Maiti, E. Gunn, DF Schmidt, DD Jiang, CA Batt, and EP Giannelis 'Dramatic enhancements in toughness of Polyvinylidene flouride nanocomposites via nanoclay-directed crystal structure and morphology' Advanced Materials 16, pp 1173-1177, 2004

Dear Sir,

At the outset I sincerely convey my regards for your research which sounds about the recent trend of technology of todays world.

Further I write, I am Dr.Arindam Mukherji, recently appointed as Scientist -C in our research organisation (IRMRA) which is under the Ministry of Commerce and Industry,Govt. Of India lke to persue my acedamic as well as research career under you in any suitable opening if you feel so.I am very much desperate to get myself involved in proper research atmosphere and team, which can only be possible at your end.

I am very much possitive towards about your responds.So please find my resume for your kind perusal.

 

With regards

Dr.Arindam Mukherji

Scientist-C,

Asst.Director

IRMRA

Dear Frank, 

Great point! As you mention, nanoparticles can certainly influence polymer morphology by influencing degree as well as type of crystallinity. The example of PVDF you mention is significant because the enhancement is not limited to mechanical properties, but it also affects the piezoelectric properties by transforming alpha-phase into beta-phase. This is a very nice result. Along those lines, there is a nice work by Li et al. on effect of interface (weak vs strong interactions) on polymer morphology. The authors show that a 'strong' interface results in restriction of polymer mobility and an overall decrease in crystallinity--nanoconfinement effect you mention in your post--while a 'weak' interface leads to enhanced crystallinity. This is yet another indication that not all interfaces are created equal! When modeling and predicting the performance of nanocomposites, it is important to have some clear insight into the type of interaction that can take place between the particular nanofiller and the polymer matrix.

 

 

Please note that the enhanced toughness in the paper by Giannelis group refers to an increase in elongation to break.  I wonder how the fracture resistance is affected. 

Dear Sir,

At the outset I sincerely convey my regards for your research which sounds about the recent trend of technology of todays world.

Further I write, I am Dr.Arindam Mukherji, recently appointed as Scientist -C in our research organisation (IRMRA) which is under the Ministry of Commerce and Industry,Govt. Of India lke to persue my acedamic as well as research career under you in any suitable opening if you feel so.I am very much desperate to get myself involved in proper research atmosphere and team, which can only be possible at your end.

I am very much possitive towards about your responds.So please find my resume for your kind perusal.

 

With regards

Dr.Arindam Mukherji

Scientist-C,

Asst.Director

IRMRA

Thank you Dr Zoubeida for pointing out Lewis' reference to me. As he has rightly pointed out, the interface will become increasingly prominent and its physics has to be properly accounted for especially when the size of the structure under consideration reaches nanometric dimensions.

Consider a standard capacitor (consisting of a dielectric layer sandwiched between metal electrodes) of macroscopic dimensions subject to a potential difference say 'V' across its ends. The objective is to find the electric field/potential/polarization vector profile along its length. If one goes by standard electrostatics, it can be worked out the electric field/polarization is constant in the dielectric...and both these fields drop abruptly to zero inside the metal i.e both these fields have jumps at the 'interface'. However, if one shrinks the capacitor to nanometric dimensions, the interface becomes as large as the dimensions of the dielectric layer..so if one assumes that the dielectric constant varies smoothly (what is the meaning of smooth at the atomic level?) then the electric field/polarization field wont have any jumps. Though this consideration may not be of any consequence while analysing large structures, it can have far reaching consequences for nano devices. 

I feel that characterization of interfaces is an important issue. Also i am not sure if good analytical models exist to model the interface. The following is one reference which i found which models the dielectric property at a insulator/insulator interface

F. Stern, Phys. Rev. B. 17, 5009 (1978)

 

 

 

Dear Xiaodong,

Thank you for bringing up this very important point of dispersion of nanoparticles in epoxy and other polymer matrices. Indeed, due to the high surface area of nanoparticles, van der Waals interaction lead to their bundling, whcih renders processing and dispersion very challenging. As you point out, the bundling reduces the interaction area with the polymer, which in turn will affect properties. I took a look at the abstract of your article in the J. of nanoscience and nanotechnology. It looks very interesting. I ordered the article through our library and look forward to communicating with you again once I receive it.

Best of luck on your research,

Zoubeida

Hi Ravi,

I am glad you appreciated Lewis's paper. The model capacitor example you mention is a good one. As you shrink the capacitor thickness, you start creating field nonlinearities even when applying a uniform field across the surface of the capacior. In a nanocomposite, that effect (distance between nanotubes for example) should have interesting implications in terms of enhanced dielectric properties. We do need more tools and methods for modeling the dieelctric behavior. Some of the articles mentioned in this thread seem to be echoing that same message. So I am very optimistic about seeing more work in the area of dielectric modeling of the interface in nanocomposites.

Warm regards,

Zoubeida

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