Proceedings of the First International Conference on Self Healing Materials 18-20 April 2007, Noordwijk aan Zee, The Netherlands Christopher W. Bielawski TOWARD CONDUCTIVE, SELF-HEALING MATERIALS Christopher W. Bielawski The University of Texas at Austin, Department of Chemistry and Biochemistry, 1 University Station, A5300, Austin, TX 78712 USA Tel: 512-232-3839 Fax: 512-471-8696 e-mail: bielawski@cm.utexas.edu URL: http://www.cm.utexas.edu/directory/christopher_bielawski A novel class of organometallic polymers based on multitopic N-heterocyclic carbenes and transition metals was shown to have potential as an electrically-conductive, self-healing material. These structurally-dynamic materials were found to display conductivities on the order of 10-3 S·cm-1. Thin films of these materials were prepared on silicon wafers, then scored and imaged using scanning electron microscopy (SEM). Heating the scored films allowed the material to undergo a unique depolymerization process and flow into the vacant regions, as observed by SEM and surface profilometry. A proposal for how these features may be incorporated into a device that displays electrically-driven, self-healing functions is presented. Keywords: self-healing, conductive polymers, dynamic polymers Stress induced microcrack formation is a main culprit of fatigue in mechanical materials and failure in electronic componentry [1]. Contemporary research has focused on solving this deleterious problem by developing “self-healing materials.” Notable examples include epoxybased composites containing encapsulated healing agents [2-4] and thermally-remendable plastics [5,6]. However, the materials used in these systems are electrically-insulating, which precludes their use in related applications. By installing features into these materials that enable electron conductivity, a number of useful features may be realized. For example, through electronic feedback, one may obtain instantaneous status of a material’s structural integrity. This feature could lead to new approaches for detecting and quantifying microcracks and/or materials that are capable of recording their stress/load histories. Other possibilities include using externally-applied electric fields to drive the self-healing process. Materials exhibiting self-healing and conductive properties can be expected to offer advantages in consumer electronics, alternatives to sophisticated redundant electronic systems, and many other applications. In order to realize a self-healing material with conductive properties, the development of a new responsive polymer with the following three features was needed: (a) the polymer must be electrically-conductive, (b) the polymerization process must be dynamic and respond to changes in external stimuli, and (c) main-chain unsaturation, a key requirement for conductivity, must be conserved or increased upon polymerization (see Eq. 1). For practical reasons, the polymerization process should also not involve the formation of by-products. Finally, a polymer with modular components was desired to facilitate systematic tuning of material and electronic properties. 1 © Springer 2007 Proceedings of the First International Conference on Self Healing Materials 18-20 April 2007, Noordwijk aan Zee, The Netherlands Christopher W. Bielawski Although a broad range of polymerizations comprised of dynamic interactions are known, the resulting polymers are not conductive [7-14]. To create polymers with these characteristics a chemical interaction that is both dynamic and extends electronic communication is necessary. The interaction between N-heterocyclic carbenes (NHCs) and transition metals is known to be reversible and the electronic communication of these systems has been well-studied [15,16]. To utilize this interaction in polymeric materials, compounds possessing more than one NHC unit (e.g., 1) were needed. R N R N R N N R N R N R R N N R n 2 N R N N R N R R E E R N R N N R N R R N E 1 E N R 3 M R N R N N R N R R N R N n N R ar ene li nker M transition metal E electr ophile R N M 4 N R n N R Figure 1: Dynamic equilibria between difunctional NHCs, electrophiles, transition metals, and their respective polymers Through a series of synthetic developments, a range of multifunctional NHCs were prepared [17, 18]. The bis(NHC) scaffold was designed to contain many modular components, including the N-substituent, aryl linker, and heteroatoms. Collectively, these compounds proved to be versatile building blocks for the synthesis of polymeric materials, as they could be homopolymerized to form poly(enetetraamine)s (2), reacted with difunctional electrophiles to produce alternating copolymers (3), and combined with transition metals to obtain welldefined organometallic polymers (4) [19-22]. As described below, each of the polymers obtained from these reactions display unique characteristics vital for development of conductive, self-healing materials. Depending on the size of the N-substituent and temperature, the poly(enetetraamine)s (2) were found to exist in equilibrium with free monomer in solution [19]. As expected, smaller N-substituents favored polymer formation, whereas higher temperatures, as well as larger Nsubstituents, resulted in an increase of free monomer. Evidence for this phenomena was obtained using NMR spectroscopy in conjunction with UV-Vis spectroscopy. The latter indicated that the effective conjugation length of these polymers increased with molecular weight. Even though polymers 2 were only stable under oxygen-free conditions, the thermal control over this reversible polymerization reaction coupled with their electronic characteristics indicate these materials hold potential in conductive, self-healing materials. Efforts toward utilizing these compounds in such applications are underway. 2 © Springer 2007 Proceedings of the First International Conference on Self Healing Materials 18-20 April 2007, Noordwijk aan Zee, The Netherlands Christopher W. Bielawski The synthesis of alternating copolymers 3 (E = N3) capitalized on our recently reported results of reacting NHCs with azides to afford 1,3-disubstituted-triazenes [23]. By combining free bis(NHC)s with bis(azide)s (e.g., 1,3-diazidobenzene), a new class of conjugated polytriazenes were prepared. More recently, we have focused efforts on studying the reversible reaction of NHCs with isothiocyanates. Similarly, free bis(NHC)s are currently being combined with bis(isothiocyanate)s [24] to form reversible, conjugated polymers. Characterization of these materials, as well as the evaluation of their potential as self-healing materials, is currently in progress. Organometallic polymers (4) with molecular weights up to 1.8 × 106 Da and excellent thermal stabilities (up to 300 °C) were also prepared using bis(NHC)s [20]. Variations of 4 included: primary alkyl, benzyl, and aryl N-substituents, benzo, biphenyl, or dioxin aryl linkers, and the use of Pd or Pt as the transition metal. It was discovered that the molecular weights of polymers 4 could be controlled through the use of chain-transfer agents (CTAs), and that these structurally dynamic polymers exhibited conductivities of the order of 10-3 S•cm-1. However, due to the high affinity of these metals for NHCs, structurally-dynamic properties were observed only at elevated temperatures. However, in order to utilize metals with weaker affinities for NHCs, an extra source of chelation was needed. This was achieved by incorporating chelating N-o-phenol moieties in the basic bis(NHC) structure. This enhanced stability allowed access to polymers containing Ni in addition to Pd and Pt [21]. Due to the combination of structurally dynamic and conductive character, the potential of organometallic polymers 4 as conductive, self-healing materials was investigated using scanning electron microscopy (SEM). Notably, as a result of their high conductivities, the deposition of gold was found to be unnecessary to obtain visible images of these materials. Thin films (800 nm) were first cast on silicon wafers and, to emulate microcrack formation, the films were scored with a sharp razor blade. After imaging (Figure 2A), the films were then heated (200 °C, 25 min) and then re-imaged (Figure 2B). Comparison of the images obtained pre- and post-thermal treatment clearly indicated that rough edges introduced by the razor blade were smoothened Since the dynamic behavior of the system was previously established in solution, it was predicted that the presence of solvent might facilitate the reformation of broken NHC-metal bonds. Hence, a thin film of material was cast on a silicon wafer, and a crack was introduced and imaged in a manner analogous to the one described above (Figure 2C). The wafer was then heated (150 °C, 2 h) in a compartmentalized sealed vessel. A pool of solvent (dimethylsulfoxide) was placed in a contiguous compartment such that solvent vapor would facilitate healing. Comparison of the SEM image of the treated film (Figure 2D) indicated that the crack induced by the razor blade was now reloaded with material. This observation was supported using surface profilometry, which indicated that the depth of the crack had been significantly reduced (800 nm → ~0 nm) in the healed films. Efforts toward eliminating the reliance on solvent vapor to facilitate this process are currently underway. 3 © Springer 2007 Proceedings of the First International Conference on Self Healing Materials 18-20 April 2007, Noordwijk aan Zee, The Netherlands A B C D Christopher W. Bielawski Figure 2: Scanning electron micrographs of a scored organometallic polymer film before (A) and after (B) exposure to heat (200 ºC, 15 min); a scored organometallic polymer film before (C) and after (D) exposure to heat (150 ºC, 2 h) in the presence of solvent vapor. Arrows indicate a common point of reference Shown in Figure 3 is a generalized depiction of how a conductive, self-healing material may operate once incorporated into a device. Microcrack formation should decrease the total number of electron percolation pathways within the material resulting in a concomitant rise in electrical resistance. Integration of the material into a circuit containing an ammeter / voltmeter, could allow the drop in conductivity (or rise in resistance) to trigger an increase in the applied electric field. Since the microcrack is the source of the increased resistance, this voltage bias should result in the generation of heat localized at the microcrack. By harnessing the produced thermal energy, the system may be electrically-driven back to its original lowresistance/high-current state. AMPS VOLTS AMPS AMPS e e crack formation polymerization VOLTS Voltage is biased; The higher resistance is used to generate heat which facilitates self-healing. Microcrack disrupts conductivity; Resistance increases. Material is electrically conductive. e VOLTS crack repair multifunctional monomer polymeric network network with microcrack a snapshot of the self-healing process Figure 3: Operation of an electrically-conductive, self-healing material 4 © Springer 2007 Proceedings of the First International Conference on Self Healing Materials 18-20 April 2007, Noordwijk aan Zee, The Netherlands Christopher W. Bielawski Collectively, these results suggest that self-healing capabilities were observed in materials with electrically-conductive properties. However, many challenges must be solved before their potential is fully realized. Most importantly, the dependency on solvent vapor to facilitate healing must be eliminated. Incorporating bulky N-alkyl groups into the multifunctional NHCs should descrease polymer viscosity, helping material to flow into microcracks upon depolymerization. In order for these polymeric materials to be broadly useful, their conductivities must be enhanced to ≥ 1 S·cm-1. We believe this may be achieved by matching the reduction-oxidation potentials of the transition metal with the N-heterocyclic carbene through substrate modification [25]. Efforts toward these goals, as well as exploring the potential of these materials in a variety of electronic applications, are in progress. ACKNOWLEDGEMENTS We are grateful to the U.S. Army Research Office (W911NF-05-1-0430), the Welch Foundation (F-1621), the Petroleum Research Fund as administered by the American Chemical Society (44077-G1), and The University of Texas at Austin for generous financial support. REFERENCES [1] J. A. Sauer and M. Hara “Effect of molecular variables on crazing and fatigue of polymers,” Adv. Polym. Sci., vol. 91/92, pp. 69-118, 1990. [2] S. R. White, N. R. Sottos, P. H. Geubelle, J. S. Moore, M. R. Kessler, S. R. Sriram, E. N. Brown, and S. Viswanathan “Autonomic healing of polymer composites,” Nature, vol. 409, pp. 794-797, 2001. [3] J. D. Rule, E. N. Brown, N. R. Sottos, S. R. 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