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High Voltage Circuit Breakers by Ruben D. Garzon

By Ruben D. Garzon

This newly revised and up-to-date reference offers good methods to the layout, choice, and utilization of high-voltage circuit breakers-highlighting compliance concerns pertaining to new and getting older gear to the evolving criteria set forth via the yankee nationwide criteria Institute and the foreign Electrotechnical fee. This variation good points the newest advances in mechanical and dielectric layout and alertness from a simplified qualitative perspective.High Voltage Circuit Breakers: layout and functions gains new fabric on touch resistance, insulating movie coatings, and fretting; temperature on the aspect of touch; short-time heating of copper; erosion and electromagnetic forces on contacts; ultimate pace and circuit breaker specifications; "weld" holiday and phone jump; elements influencing dielectric energy; air, SF6, vacuum, and stable insulation; and dielectric loss and partial discharges, and comprises up-to-date chapters on capacitance switching; switching sequence and shunt reactors; transitority overvoltages; and some great benefits of tracking.

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Among these works, probably the most significant technical contribution can be found in the investigations of Hermann and Ragaller [IS]. They developed a model that accurately describes the performance of air and SF, interrupters. What is different in this model is that the effects of turbulence downstream from the throat of the nozzle are taken into consideration. In this model the following assumptions are made: a) There is a temperature profile that encompasses three regions; the first one embodies the arc core, the second covers the arc's surrounding thermal layer, and the third consists of the external cold gas.

The second peak occurs on phase B at approximately 120" or (t = 2d3w). Since the ac components are identical we can easily see which peak is larger by comparing the dc components. Starting with phases B and C, we can see that they start at the same value (I, / 2 ) . We also know, without looking at the absolute quantitative values, that since the decay at 60" is less than at 120°, the peak of the current on phase C is larger. Next comparing the peaks of phases A and C, we can see that the dc component on A starts with twice the value of the component of C, but by the time A reaches its peak it has decayed more than the C component.

J. J. C. Ludwig, A simple model for hgh current arcs stabilized by forced convection, Journal Applied Physics, 46: 3352-3360, 1975. 12. B. W. Swanson and R. M. Roidt, Numerical solutions for an SF, arc, Proceedings IEEE, 59: 493-501, 1971. Copyright © 2002 by Taylor & Francis 26 Chapter I 13. G. Frind and J. A. Rich, Recovery Speed of an Axial Flow Gas Blast Interrupter, IEEE Transactions Pow. App. Syst. -93, 1675, 1974. 14. D. T. Tuma and J. J. Lowke, Prediction of properties of arcs stabilized by forced convection, J.

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