Pub Date : 2016-07-03DOI: 10.1109/ICD.2016.7547762
G. Callender, P. Rapisarda, P. Lewin
Models of partial discharge (PD) activity have been widely used to investigate PD activity in cylindrical and spherical voids within insulation material. PD activity is known to alter void geometry due to the erosion of insulation material from the deployed charge. In this work, a PD model is produced to investigate the impact of void erosion on PD activity. The model is validated by reproducing measured phase resolved PD (PRPD) patterns for a spherical void in a homogeneous dielectric material. The impact of void erosion is then investigated by running the model with different void geometries. The results from the model show that the PRPD patterns depend heavily on the level of erosion due to the impact of the erosion on the electric field at the void surface.
{"title":"Investigation of void erosion on partial discharge activity using simulation","authors":"G. Callender, P. Rapisarda, P. Lewin","doi":"10.1109/ICD.2016.7547762","DOIUrl":"https://doi.org/10.1109/ICD.2016.7547762","url":null,"abstract":"Models of partial discharge (PD) activity have been widely used to investigate PD activity in cylindrical and spherical voids within insulation material. PD activity is known to alter void geometry due to the erosion of insulation material from the deployed charge. In this work, a PD model is produced to investigate the impact of void erosion on PD activity. The model is validated by reproducing measured phase resolved PD (PRPD) patterns for a spherical void in a homogeneous dielectric material. The impact of void erosion is then investigated by running the model with different void geometries. The results from the model show that the PRPD patterns depend heavily on the level of erosion due to the impact of the erosion on the electric field at the void surface.","PeriodicalId":306397,"journal":{"name":"2016 IEEE International Conference on Dielectrics (ICD)","volume":"10 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2016-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"133490384","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2016-07-03DOI: 10.1109/ICD.2016.7547813
Peng Zhang, Jianying Li, H. Jin, Hao Zhang
In this paper, the zirconia toughened alumina (ZTA) ceramics were fabricated by pressureless sintering method. Dielectric relaxation characteristics of both alumina and ZTA ceramics were investigated using thermally stimulated depolarization current (TSDC) method and the relaxation parameters were calculated from the experimental TSDC curves. In addition, the relationship between zirconia doping and dielectric relaxation properties was analyzed. The results showed that doping of zirconia can affect the defect dipoles distributions in ZTA ceramics, and introduces a new relaxation peak at 478K. This new relaxation process may be attributed to the reorientation of dipoles of dopant and oxygen vacancy pairs generated in cubic zirconia grains.
{"title":"Thermally stimulated depolarization processes in zirconia toughened alumina ceramics","authors":"Peng Zhang, Jianying Li, H. Jin, Hao Zhang","doi":"10.1109/ICD.2016.7547813","DOIUrl":"https://doi.org/10.1109/ICD.2016.7547813","url":null,"abstract":"In this paper, the zirconia toughened alumina (ZTA) ceramics were fabricated by pressureless sintering method. Dielectric relaxation characteristics of both alumina and ZTA ceramics were investigated using thermally stimulated depolarization current (TSDC) method and the relaxation parameters were calculated from the experimental TSDC curves. In addition, the relationship between zirconia doping and dielectric relaxation properties was analyzed. The results showed that doping of zirconia can affect the defect dipoles distributions in ZTA ceramics, and introduces a new relaxation peak at 478K. This new relaxation process may be attributed to the reorientation of dipoles of dopant and oxygen vacancy pairs generated in cubic zirconia grains.","PeriodicalId":306397,"journal":{"name":"2016 IEEE International Conference on Dielectrics (ICD)","volume":"46 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2016-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"133591680","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2016-07-03DOI: 10.1109/ICD.2016.7547646
N. Chalashkanov, S. Dodd, L. Dissado, J. Fothergill
The aim of this study was to investigate the difference in the pulse sequence analysis (PSA) plots of partial discharge (PD) data obtained from electrode-bound voids and electrical trees in epoxy resin samples. Electrical discharge tests were performed on a set of epoxy resin samples containing needle voids, which were obtained by a partial extraction of tungsten needle electrode. Two epoxy resin systems were used in this study, Araldite CY1301 and Araldite CY1311. The two resins have different dielectric properties, which allowed the effect of material conductivity on the discharge activity in the void to be investigated. Complementary electrical tree growth experiments were performed on a set of samples with a conventional needle-plane electrode configuration. The effects of the material properties, temperature and moisture absorbed in the dielectric samples were also investigated. The results show that additional material characterization is needed to supplement the PSA plots in order to achieve a reliable diagnostic tool.
{"title":"A comparison between PSA plots of partial discharges in needle voids and electrical trees","authors":"N. Chalashkanov, S. Dodd, L. Dissado, J. Fothergill","doi":"10.1109/ICD.2016.7547646","DOIUrl":"https://doi.org/10.1109/ICD.2016.7547646","url":null,"abstract":"The aim of this study was to investigate the difference in the pulse sequence analysis (PSA) plots of partial discharge (PD) data obtained from electrode-bound voids and electrical trees in epoxy resin samples. Electrical discharge tests were performed on a set of epoxy resin samples containing needle voids, which were obtained by a partial extraction of tungsten needle electrode. Two epoxy resin systems were used in this study, Araldite CY1301 and Araldite CY1311. The two resins have different dielectric properties, which allowed the effect of material conductivity on the discharge activity in the void to be investigated. Complementary electrical tree growth experiments were performed on a set of samples with a conventional needle-plane electrode configuration. The effects of the material properties, temperature and moisture absorbed in the dielectric samples were also investigated. The results show that additional material characterization is needed to supplement the PSA plots in order to achieve a reliable diagnostic tool.","PeriodicalId":306397,"journal":{"name":"2016 IEEE International Conference on Dielectrics (ICD)","volume":"9 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2016-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"133679949","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2016-07-03DOI: 10.1109/ICD.2016.7547605
G. Bélijar, S. Diaham, L. Laudebat, Z. Valdez-Nava, T. Lebey, T. Jones
This study treats the influence upon the bulk dielectric properties of epoxy resin loaded with barium titanate (BaTiO3) particles when an ac electric field is used to form the particles into chains. A particle chain formation model, coupled with finite element method (FEM) solution of the Laplace's equation leads to estimates for permittivity as a function of the composite structure. Simulation results are then compared with experimental measurements that corroborate the time-dependent evolution of the dielectric permittivity.
{"title":"Particle chain formation in a liquid polymer under ac electric field: Model and experiments","authors":"G. Bélijar, S. Diaham, L. Laudebat, Z. Valdez-Nava, T. Lebey, T. Jones","doi":"10.1109/ICD.2016.7547605","DOIUrl":"https://doi.org/10.1109/ICD.2016.7547605","url":null,"abstract":"This study treats the influence upon the bulk dielectric properties of epoxy resin loaded with barium titanate (BaTiO3) particles when an ac electric field is used to form the particles into chains. A particle chain formation model, coupled with finite element method (FEM) solution of the Laplace's equation leads to estimates for permittivity as a function of the composite structure. Simulation results are then compared with experimental measurements that corroborate the time-dependent evolution of the dielectric permittivity.","PeriodicalId":306397,"journal":{"name":"2016 IEEE International Conference on Dielectrics (ICD)","volume":"3 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2016-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"133828152","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2016-07-03DOI: 10.1109/ICD.2016.7547533
T. Tanaka
A nanocomposite system consists of nanoscale organic polymer spaces and islandic inorganic nano-particles. In this paper, a concept of quantum dots (QDs) is introduced to explain various dielectric properties of nanocomposites. Nano-particles are regarded as QDs rather than simple carrier traps. QDs exhibit negative permittivity. They also show Coulomb blockade effect, and inversely accept charge injection if they are subjected to high electric field beyond its barrier threshold. This concept can interpret key phenomena appearing in nanocomposites such as the reduction of permittivity, the threshold of space charge formation, the high field conduction and dielectric breakdown. Space charge formation and treeing phenomena are analyzed in more detail. A threshold for charge injection to QDs are obtained as the order of 100 kV/mm from the experimental data associated with both space charge and treeing.
{"title":"A novel concept for electronic transport in nanoscale spaces formed by islandic multi-cored nanoparticles","authors":"T. Tanaka","doi":"10.1109/ICD.2016.7547533","DOIUrl":"https://doi.org/10.1109/ICD.2016.7547533","url":null,"abstract":"A nanocomposite system consists of nanoscale organic polymer spaces and islandic inorganic nano-particles. In this paper, a concept of quantum dots (QDs) is introduced to explain various dielectric properties of nanocomposites. Nano-particles are regarded as QDs rather than simple carrier traps. QDs exhibit negative permittivity. They also show Coulomb blockade effect, and inversely accept charge injection if they are subjected to high electric field beyond its barrier threshold. This concept can interpret key phenomena appearing in nanocomposites such as the reduction of permittivity, the threshold of space charge formation, the high field conduction and dielectric breakdown. Space charge formation and treeing phenomena are analyzed in more detail. A threshold for charge injection to QDs are obtained as the order of 100 kV/mm from the experimental data associated with both space charge and treeing.","PeriodicalId":306397,"journal":{"name":"2016 IEEE International Conference on Dielectrics (ICD)","volume":"73 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2016-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"115694196","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2016-07-03DOI: 10.1109/ICD.2016.7547726
Takahiro Nakamura, K. Ozawa, A. Kumada, K. Hidaka, T. Kato, T. Yamagiwa
Epoxy resins are widely used as insulating material in electrical apparatus. As such epoxy resins are non-transparent due to the effect of fillers, it is hard to optically observe electrical treeing in them. In this paper, we observe electrical trees in unfilled and filled epoxy resins by X-ray phase contrast imaging. When X-ray passes through very small tubular material such as electrical trees, edge-enhancement images are obtained. It makes easier to detect trees, but, on the other hand, wave-optical analysis is necessary to obtain a tree diameter accurately from an apparent tree diameter in an X-ray image. Through the computational wave-optical analysis, it turns out that the apparent tree diameter converges to a certain value with decreasing the diameter of measured tree. In addition, optimal arrangement of the equipment and minimum detective value are investigated based on this calculation. In case of unfilled epoxy, minimum detective value in the condition of optimal arrangement is found to be 3.5μm.
{"title":"Observation of electrical treeing in epoxy resin by X-ray phase contrast imaging","authors":"Takahiro Nakamura, K. Ozawa, A. Kumada, K. Hidaka, T. Kato, T. Yamagiwa","doi":"10.1109/ICD.2016.7547726","DOIUrl":"https://doi.org/10.1109/ICD.2016.7547726","url":null,"abstract":"Epoxy resins are widely used as insulating material in electrical apparatus. As such epoxy resins are non-transparent due to the effect of fillers, it is hard to optically observe electrical treeing in them. In this paper, we observe electrical trees in unfilled and filled epoxy resins by X-ray phase contrast imaging. When X-ray passes through very small tubular material such as electrical trees, edge-enhancement images are obtained. It makes easier to detect trees, but, on the other hand, wave-optical analysis is necessary to obtain a tree diameter accurately from an apparent tree diameter in an X-ray image. Through the computational wave-optical analysis, it turns out that the apparent tree diameter converges to a certain value with decreasing the diameter of measured tree. In addition, optimal arrangement of the equipment and minimum detective value are investigated based on this calculation. In case of unfilled epoxy, minimum detective value in the condition of optimal arrangement is found to be 3.5μm.","PeriodicalId":306397,"journal":{"name":"2016 IEEE International Conference on Dielectrics (ICD)","volume":"31 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2016-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"116967134","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2016-07-03DOI: 10.1109/ICD.2016.7547744
M. Unge
The conduction mechanism in a material is to a large extent determined by the nature of the electronic states. Localized states give hopping conduction and delocalized states band transport. In amorphous materials there may be a transition from localized states at the band edges to delocalized states higher up in the band. Here we use linear scaling density functional theory and a percolation method to determine electron mobility in amorphous polyethylene. The electron mobility edge is determined to ~ 0.2 eV.
{"title":"Electron mobility edge in amorphous polyethylene","authors":"M. Unge","doi":"10.1109/ICD.2016.7547744","DOIUrl":"https://doi.org/10.1109/ICD.2016.7547744","url":null,"abstract":"The conduction mechanism in a material is to a large extent determined by the nature of the electronic states. Localized states give hopping conduction and delocalized states band transport. In amorphous materials there may be a transition from localized states at the band edges to delocalized states higher up in the band. Here we use linear scaling density functional theory and a percolation method to determine electron mobility in amorphous polyethylene. The electron mobility edge is determined to ~ 0.2 eV.","PeriodicalId":306397,"journal":{"name":"2016 IEEE International Conference on Dielectrics (ICD)","volume":"10 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2016-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"124631132","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2016-07-03DOI: 10.1109/ICD.2016.7547554
Jing Sun, Peihong Zhang
The interface is critical for the design of nanocomposites with desirable properties, this research try to prove the influence of interface bonding strength between nanofiller and matrix on the dielectric properties (dielectric spectroscopy and conduction current) of epoxy nanocomposites. In this experiments, nanofiller/ethanol suspensions were prepared by ultrasonic vibration method, the four kinds of epoxy resin nanocomposites with 3wt% concentration were made, respectively. The zeta potential of the suspensions were measured by ESA method. The dielectric spectroscopy and the conduction current characteristics of nanocomposite were tested. The zeta potential of the four kinds of suspensions according to the order from small to large is ZnO, MgO, Al2O3 and SiO2 successively, SiO2 nanocomposites shown the lowest permittivity, in addition, the conduction current of the SiO2 composites was also lowest among them except the MgO composites. The results indicate that the higher zeta potential can represent strong interface bonding and make the permittivity and conduction current of the nanocomposites decrease, this is due to the lower polarization strength. In this paper, the addition of SiO2 nanoparticles can provide advantageous performance of epoxy nanocomposites among the four kinds of nanofillers. The interface bonding strength has a major influence on the dielectric property of composites.
{"title":"Study on the effect of interface bonding strength on the dielectric properties of epoxy nanocomposites","authors":"Jing Sun, Peihong Zhang","doi":"10.1109/ICD.2016.7547554","DOIUrl":"https://doi.org/10.1109/ICD.2016.7547554","url":null,"abstract":"The interface is critical for the design of nanocomposites with desirable properties, this research try to prove the influence of interface bonding strength between nanofiller and matrix on the dielectric properties (dielectric spectroscopy and conduction current) of epoxy nanocomposites. In this experiments, nanofiller/ethanol suspensions were prepared by ultrasonic vibration method, the four kinds of epoxy resin nanocomposites with 3wt% concentration were made, respectively. The zeta potential of the suspensions were measured by ESA method. The dielectric spectroscopy and the conduction current characteristics of nanocomposite were tested. The zeta potential of the four kinds of suspensions according to the order from small to large is ZnO, MgO, Al2O3 and SiO2 successively, SiO2 nanocomposites shown the lowest permittivity, in addition, the conduction current of the SiO2 composites was also lowest among them except the MgO composites. The results indicate that the higher zeta potential can represent strong interface bonding and make the permittivity and conduction current of the nanocomposites decrease, this is due to the lower polarization strength. In this paper, the addition of SiO2 nanoparticles can provide advantageous performance of epoxy nanocomposites among the four kinds of nanofillers. The interface bonding strength has a major influence on the dielectric property of composites.","PeriodicalId":306397,"journal":{"name":"2016 IEEE International Conference on Dielectrics (ICD)","volume":"61 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2016-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"128720790","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2016-07-03DOI: 10.1109/ICD.2016.7547694
Yujiao Tang, Z. An, F. Shan, F. Zheng, Yewen Zhang
We have reported that hydrophobicity of silicone rubber (SIR) can be significantly enhanced by direct fluorination. In this work, surface fluorinated SIR samples, together with the unfluorinated (virgin) ones were corona treated using a multi-needle-to-plate electrode system, to further evaluate corona resistance of the fluorinated SIR layer. ATR-IR analyses suggest that there may be oxidation of the partially fluorinated methyl groups and cleavage of Si-C bonds during the corona treatment, but the cleavage led to formation of Si-F bonds rather than Si-OH bonds. SEM surface and cross section images show that the corona treatment did not change the fluorinated layer thickness, although surface morphology was changed to some degree. In contrast with this, the virgin surface layer was severely degraded or ablated, forming a degraded layer on which aggregates of silica particles and/or degradation products of the SIR matrix material were left. Measurements of water contact angle and surface potential decay further confirm good resistance of the fluorinated layer to corona discharge.
{"title":"Corona aging and hydrophobicity of surface fluorinated silicone rubbers","authors":"Yujiao Tang, Z. An, F. Shan, F. Zheng, Yewen Zhang","doi":"10.1109/ICD.2016.7547694","DOIUrl":"https://doi.org/10.1109/ICD.2016.7547694","url":null,"abstract":"We have reported that hydrophobicity of silicone rubber (SIR) can be significantly enhanced by direct fluorination. In this work, surface fluorinated SIR samples, together with the unfluorinated (virgin) ones were corona treated using a multi-needle-to-plate electrode system, to further evaluate corona resistance of the fluorinated SIR layer. ATR-IR analyses suggest that there may be oxidation of the partially fluorinated methyl groups and cleavage of Si-C bonds during the corona treatment, but the cleavage led to formation of Si-F bonds rather than Si-OH bonds. SEM surface and cross section images show that the corona treatment did not change the fluorinated layer thickness, although surface morphology was changed to some degree. In contrast with this, the virgin surface layer was severely degraded or ablated, forming a degraded layer on which aggregates of silica particles and/or degradation products of the SIR matrix material were left. Measurements of water contact angle and surface potential decay further confirm good resistance of the fluorinated layer to corona discharge.","PeriodicalId":306397,"journal":{"name":"2016 IEEE International Conference on Dielectrics (ICD)","volume":"47 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2016-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"129547078","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2016-07-03DOI: 10.1109/ICD.2016.7547702
Y. Wang, Kai Wu, Jinhua Dong, Chong Zhang, Wenpeng Li
Our previous studies showed that the aging parameter, i.e. the n-value, of XLPE was quite different from that of XLPE nanocomposites. In order to investigate the effects of space charge on aging parameter under DC voltage, the n-values of XLPE and its nanocomposites were measured under AC voltage in this report, because few space charge exits in the sample under AC voltage. Step-stress tests were carried out under AC voltage to measure the n-value. The results showed that the aging parameters of XLPE and its nanocomposites under AC voltage were close, i.e. 7.3 and 6.6, respectively. This suggests that space charge accumulation plays an important role in DC aging.
{"title":"Estimating aging parameter of XLPE and its nanocomposites under AC voltage using step-stress test","authors":"Y. Wang, Kai Wu, Jinhua Dong, Chong Zhang, Wenpeng Li","doi":"10.1109/ICD.2016.7547702","DOIUrl":"https://doi.org/10.1109/ICD.2016.7547702","url":null,"abstract":"Our previous studies showed that the aging parameter, i.e. the n-value, of XLPE was quite different from that of XLPE nanocomposites. In order to investigate the effects of space charge on aging parameter under DC voltage, the n-values of XLPE and its nanocomposites were measured under AC voltage in this report, because few space charge exits in the sample under AC voltage. Step-stress tests were carried out under AC voltage to measure the n-value. The results showed that the aging parameters of XLPE and its nanocomposites under AC voltage were close, i.e. 7.3 and 6.6, respectively. This suggests that space charge accumulation plays an important role in DC aging.","PeriodicalId":306397,"journal":{"name":"2016 IEEE International Conference on Dielectrics (ICD)","volume":"2 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2016-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"129913209","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
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