1. Introduction.
It is often stated that an ideal lightning arrester should quickly relieve the system of excess voltages, but should not allow any flow of the dynamic current of the system.
It is shown in this paper that the statement is vague and unscientific and that it is almost impossible to design a truly ideal arrester by the principle of a discharger.
2. Solution using the effective values of alternating electrical quantities.
After discussing the series resistance of a horn arrester, the superiority of a multigap type is demonstrated. A formula is derived which gives the magnitude of the series resistance required for a give numeber of air gaps.
The shunt resistance is then determined that would make the arc unstable. The discharge characteristic of an aluminum cell arrester is also considered. It is shown that the volt-ampere characteristic, which simply gives the relation between effective values, is entirely inadequate to cope with the discharge phenomena, which generally contain complicated and abrupt changes of instantaneous values.
3. Solution considering the instantaneous phenomena.
In order to understand the instantaneous phenomena, the dynamic characteristics muts be considered. But the dynamic characteristic is indeterminate unless the form and the magnitude of the lightning disturbance are given.
It is especially difficult to discuss the discharge of an aluminum cell lightning arrester since its dynamic characteristic has yet been very little studied.
4. Behaviour under abnormal voltages.
Refering to the following three cases, it is shown that, even if the arrest- er behaves so well as to perfectly satisfy the generally accepted conditions, the useful A.C. is apt to be discharged while the disturbing forms of potential are retained in the line, so that the step out of synchronous machines becomes inevitable.
i When the lightning is a high frequency oscillation of short duration.
ii When the lightning is a high frequency sustained oscillation.
iii When the lightning is a low frequency or a static potential.
5. A device on the alum num cell arrestor.
The possibility of utilizing the static capacity of the cell arrester as a high frequency absorber is pointed out. The author-proposes for this purpose the use of a shorter air gap with series resistance and also a static condenser in parallel with the simple air gap hitherto employed.
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