High Voltage Engineering by Prof M S Naidu, Prof V Kamaraju
By Prof M S Naidu, Prof V Kamaraju
The textual content is intended for the senior Undergraduate or Postgraduate scholar of electric or electric and Electronics Engineering who has opted for a direction on High-Voltage Engineering. The publication discusses the state-of-the artwork in HVE structures in info. Written in uncomplicated and pedagogical demeanour, the content material offers a holistic figuring out to the reader of the inception, operating ideas, benefits and downsides of HVE ideas and structures. The ebook has been designed retaining the requisites from a amateur engineer in viewpoint and hence a lot care has been taken to supply the most recent updates from the sector
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Example text
Symp. on High Voltage Engineering (ISH), Paper No. 06 (1979). 16. , “Field optimization of three dimensional high voltage equipment”, 11th ISH, London, Paper No. 75. P6 (1999). 17. , “Finite element solution for complex potential electric fields”, IEEE Trans. on Power Apparatus and systems, 86, pp. 1156–1161 (1977). 18. , “Electric Field of a Rod-Plane Spark gap”, IEE Proceedings, 117, pp. 283 (1970). 19. S. , “Digitial Computer Calculation of the Electric Potential and Field of a Rod gap”, IEEE Proceedings.
IEEE Transaction on power apparatus and systems, 97, 1156–1166 (1977). 10. , Steinbirglar, H. V. Fields”, IEEE Transactions on PAS, 93 1660–1668 (1974). 11. , “A Review of Charge Simulation Method and its Applications”, IEEE Transactions on Electrical Insulation, EI-24 No. 13–20 (1989). 12. F. , Boundary Element Techniques, Springer-Verlag (1984). 13. , “Recent developments in calculation of electric and magnetic fields related to high voltage engineering”, Key Note Speech, Proc. of 12th Int. Symp.
6. 7. 8. Vacuum Mineral Oil polybutanes and synthetic florinated hydrocarbon oils Solid-gas or Solid-liquid insulation breakdown strength V(x, y) = a + bx + cy V(x, y) = a + bx + cy + dxy The given field configuration is simulated by either discrete charges like point or line charge or with a continuous charge distribution. 9. The simulated charge in BEM method is the charge distribution at the surface such as at the electrode surface or around the axis. 10. When the field configuration is two-dimensional and has axial symmetry.