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The Influence of Spherical Cavity Surface Charge Distribution on PD Events

The Influence of Spherical Cavity Surface Charge Distribution on PD Events
The Influence of Spherical Cavity Surface Charge Distribution on PD Events
Modelling of partial discharge (PD) events allows a better understanding of the phenomena itself. In this work, an improved model representing PD behaviour within a spherical cavity in a homogeneous dielectric material has been developed to study the influence of cavity surface charge distribution on the electric field distribution in the cavity and the material. Comparison of measurement and simulation results has been undertaken to validate the model.
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Illias, H A
882c48a3-4f17-474b-954f-dfb8584db498
Chen, G
3de45a9c-6c9a-4bcb-90c3-d7e26be21819
Lewin, P L
78b4fc49-1cb3-4db9-ba90-3ae70c0f639e
Illias, H A
882c48a3-4f17-474b-954f-dfb8584db498
Chen, G
3de45a9c-6c9a-4bcb-90c3-d7e26be21819
Lewin, P L
78b4fc49-1cb3-4db9-ba90-3ae70c0f639e

(2011) The Influence of Spherical Cavity Surface Charge Distribution on PD Events. UHVnet 2011, United Kingdom. 18 - 19 Jan 2011. p. 21 .

Record type: Conference or Workshop Item (Other)

Abstract

Modelling of partial discharge (PD) events allows a better understanding of the phenomena itself. In this work, an improved model representing PD behaviour within a spherical cavity in a homogeneous dielectric material has been developed to study the influence of cavity surface charge distribution on the electric field distribution in the cavity and the material. Comparison of measurement and simulation results has been undertaken to validate the model.

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More information

Published date: 18 January 2011
Additional Information: Event Dates: 18-19 January 2011
Venue - Dates: UHVnet 2011, United Kingdom, 2011-01-18 - 2011-01-19
Organisations: Electronics & Computer Science, EEE

Identifiers

Local EPrints ID: 271870
URI: http://eprints.soton.ac.uk/id/eprint/271870
PURE UUID: e523f7cd-9002-44eb-87ac-060171a2cea8

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Date deposited: 06 Jan 2011 23:49
Last modified: 18 Jul 2017 06:37

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