2018
DOI: 10.1109/tdei.2018.007086
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DC electrical tree initiation in silicone rubber under temperature gradient

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Cited by 40 publications
(10 citation statements)
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“…It can be seen that the calculated value 5.14 × 10 8 V/m of the equation is quite close to the simulated electric field intensity value 5.50 × 10 8 V/m, indicating that the extremely high electric field may reduce the potential barrier on the tip surface and result in the Fowler–Nordheim tunneling effect, which can induce electron emission from the needle tip [ 23 , 24 ]. The electron emission current density ( j ) under high electric field can be obtained by Equation (2) [ 25 ]: where A , T , φ, E , ɛ 0 ɛ r and k are the constant depending on metal parameters, metal temperature in Kelvin, metal work function, electric field of the needle tip, dielectric constant and Boltzmann’s constant. Obviously, the is linearity to the and thus the electron emission current density increases with increasing electric field intensity.…”
Section: Discussionmentioning
confidence: 99%
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“…It can be seen that the calculated value 5.14 × 10 8 V/m of the equation is quite close to the simulated electric field intensity value 5.50 × 10 8 V/m, indicating that the extremely high electric field may reduce the potential barrier on the tip surface and result in the Fowler–Nordheim tunneling effect, which can induce electron emission from the needle tip [ 23 , 24 ]. The electron emission current density ( j ) under high electric field can be obtained by Equation (2) [ 25 ]: where A , T , φ, E , ɛ 0 ɛ r and k are the constant depending on metal parameters, metal temperature in Kelvin, metal work function, electric field of the needle tip, dielectric constant and Boltzmann’s constant. Obviously, the is linearity to the and thus the electron emission current density increases with increasing electric field intensity.…”
Section: Discussionmentioning
confidence: 99%
“…In Figure 9 a, the E 0 higher than 10 8 V/m could lead to a considerable Fowler–Nordheim tunnel effect (see Equation (1)) and induce the emission of electrons from the tip of the needle [ 24 , 25 , 26 , 27 ]. Ionization occurs when electrons with high energy collide with molecules in the polymer (process ①).…”
Section: Discussionmentioning
confidence: 99%
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“…These electrons escape from the trap and become hot electrons. The high temperature will trigger more hot electrons, causing the SIR molecular chains to break [37]. The high number of hot electrons produced by thermal stimulation is the main reason for the decrease of the tree inception voltage as the GD temperature rises with each HV side temperature, as shown in Figure 2.…”
Section: Trap Distributionmentioning
confidence: 99%
“…The increasing number of injected charges is one of the reasons for the lower tree inception voltage as the HV temperature rises, as shown in Figure 6. The injection current occurring in the interface between the high-voltage electrode and the SIR sample can be obtained by the Schottky formula [37], [38]. The increase in the HV side temperature leads to a decrease in the Schottky barrier and increases the injected charge.…”
Section: Trap Distributionmentioning
confidence: 99%