The effects of nanoparticles and organic additives with controlled dispersion on dielectric properties of polymers: Charge trapping and impact excitation

This work presents a comprehensive investigation into the effects of nanoparticles and organic additives on the dielectric properties of insulating polymers using reinforced silicone rubber as a model system. TiO2 and ZrO2 nanoparticles (d = 5 nm) were well dispersed into the polymer via a bimodal surface modification approach. Organic molecules with the potential of voltage stabilization were further grafted to the nanoparticle to ensure their dispersion. These extrinsic species were found to provide deep traps for charge carriers and exhibited effective charge trapping properties at a rather small concentration (∼1017 cm−3). The charge trapping is found to have the most significant effect on breakdown strength when the electrical stressing time is long enough that most charges are trapped in the deep states. To establish a quantitative correlation between the trap depth and the molecular properties, the electron affinity and ionization energy of each species were calculated by an ab initio method and were compared with the experimentally measured values. The correlation however remains elusive and is possibly complicated by the field effect and the electronic interactions between different species that are not considered in this computation. At high field, a super-linear increase of current density was observed for TiO2 filled composites and is likely caused by impact excitation due to the low excitation energy of TiO2 compared to ZrO2. It is reasoned that the hot charge carriers with energies greater than the excitation energy of TiO2 may excite an electron-hole pair upon collision with the NP, which later will be dissociated and contribute to free charge carriers. This mechanism can enhance the energy dissipation and may account for the retarded electrical degradation and breakdown of TiO2 composites.

[1]  L. Schadler,et al.  On the Nature of High Field Charge Transport in Reinforced Silicone Dielectrics: Experiment and Simulation , 2016, 1606.02683.

[2]  H. Ploehn,et al.  Bimodal Polymer Brush Core-Shell Barium Titanate Nanoparticles: A Strategy for High-Permittivity Polymer Nanocomposites , 2015 .

[3]  L. Schadler,et al.  Bimodal “matrix-free” polymer nanocomposites , 2015 .

[4]  L. Lundgaard,et al.  Influence of molecular additives on positive streamer propagation in ester liquids , 2014, 2014 IEEE 18th International Conference on Dielectric Liquids (ICDL).

[5]  D. Coker,et al.  Single electron states in polyethylene , 2014 .

[6]  L. Schadler,et al.  Dielectric breakdown strength of epoxy bimodal-polymer-brush-grafted core functionalized silica nanocomposites , 2014, IEEE Transactions on Dielectrics and Electrical Insulation.

[7]  L. Schadler,et al.  Ligand engineering of polymer nanocomposites: from the simple to the complex. , 2014, ACS applied materials & interfaces.

[8]  L. Schadler,et al.  Enhanced charge trapping in bimodal brush functionalized silica-epoxy nanocomposite dielectrics , 2014, 2014 IEEE Conference on Electrical Insulation and Dielectric Phenomena (CEIDP).

[9]  B. Han,et al.  Mechanisms on electrical breakdown strength increment of polyethylene by aromatic carbonyl compounds addition: a theoretical study , 2013, Journal of Molecular Modeling.

[10]  A. Walsh,et al.  Band alignment of rutile and anatase TiO₂. , 2013, Nature materials.

[11]  P. Åstrand,et al.  Excitation energies and ionization potentials at high electric fields for molecules relevant for electrically insulating liquids , 2013 .

[12]  L. Brinson,et al.  Effect of Interfacial Energetics on Dispersion and Glass Transition Temperature in Polymer Nanocomposites , 2013 .

[13]  Ying Li,et al.  Bimodal surface ligand engineering: the key to tunable nanocomposites. , 2013, Langmuir : the ACS journal of surfaces and colloids.

[14]  L. Schadler,et al.  Grafting Bimodal Polymer Brushes on Nanoparticles Using Controlled Radical Polymerization , 2012 .

[15]  L. Lundgaard,et al.  Effects of N,N-dimethylaniline and trichloroethene on prebreakdown phenomena in liquid and solid N-tridecane , 2011, IEEE Transactions on Dielectrics and Electrical Insulation.

[16]  L. Schadler,et al.  A review on the importance of nanocomposite processing to enhance electrical insulation , 2011, IEEE Transactions on Dielectrics and Electrical Insulation.

[17]  P. Åstrand,et al.  Field dependence on the molecular ionization potential and excitation energies compared to conductivity models for insulation materials at high electric fields , 2011 .

[18]  S. Gubanski,et al.  High efficiency voltage stabilizers for XLPE cable insulation , 2009 .

[19]  M. Iizuka,et al.  Suppression of electrical tree initiation in LDPE by additives of polycyclic compound , 2009, IEEE Transactions on Dielectrics and Electrical Insulation.

[20]  Walter R. Duncan,et al.  Theoretical studies of photoinduced electron transfer in dye-sensitized TiO2. , 2007, Annual review of physical chemistry.

[21]  F. Flores,et al.  Energy level alignment at metal/organic semiconductor interfaces: "pillow" effect, induced density of interface states, and charge neutrality level. , 2007, The Journal of chemical physics.

[22]  Y. Yamano Roles of polycyclic compounds in increasing breakdown strength of LDPE film , 2006, IEEE Transactions on Dielectrics and Electrical Insulation.

[23]  T. Tanaka,et al.  Dielectric nanocomposites with insulating properties , 2005, IEEE Transactions on Dielectrics and Electrical Insulation.

[24]  G. Teyssedre,et al.  Charge transport modeling in insulating polymers: from molecular to macroscopic scale , 2005, IEEE Transactions on Dielectrics and Electrical Insulation.

[25]  T. Maeno,et al.  Space charge behavior in low density polyethylene at pre-breakdown , 2005, IEEE Transactions on Dielectrics and Electrical Insulation.

[26]  H. Ghosh,et al.  Dynamics of Interfacial Electron Transfer from Photoexcited Quinizarin (Qz) into the Conduction Band of TiO2 and Surface States of ZrO2 Nanoparticles , 2004 .

[27]  Chenming Hu,et al.  Metal-dielectric band alignment and its implications for metal gate complementary metal-oxide-semiconductor technology , 2002 .

[28]  Wong,et al.  Electron capture by the image charge of a metal nanoparticle , 2000, Physical review letters.

[29]  O. Lesaint,et al.  On the relationship between streamer branching and propagation in liquids: influence of pyrene in cyclohexane , 2000 .

[30]  J. Robertson Band offsets of wide-band-gap oxides and implications for future electronic devices , 2000 .

[31]  K. Seki,et al.  ENERGY LEVEL ALIGNMENT AND INTERFACIAL ELECTRONIC STRUCTURES AT ORGANIC/METAL AND ORGANIC/ORGANIC INTERFACES , 1999 .

[32]  I. B. Martini,et al.  Effect of Structure on Electron Transfer Reactions between Anthracene Dyes and TiO2 Nanoparticles , 1998 .

[33]  A. Becke Density-functional thermochemistry. III. The role of exact exchange , 1993 .

[34]  Hermann Stoll,et al.  Results obtained with the correlation energy density functionals of becke and Lee, Yang and Parr , 1989 .

[35]  Parr,et al.  Development of the Colle-Salvetti correlation-energy formula into a functional of the electron density. , 1988, Physical review. B, Condensed matter.

[36]  A. K. Jonscher,et al.  Low-frequency dispersion in carrier-dominated dielectri , 1978 .

[37]  A. K. Jonscher,et al.  The ‘universal’ dielectric response , 1977, Nature.

[38]  C. Duke,et al.  Charge-Induced Relaxation in Polymers , 1976 .

[39]  H. Saltsburg,et al.  Charge transfer in metal/atactic polystyrene contacts , 1976 .