Disruptive strength with transient voltages

1910 ◽  
Vol 29 (5) ◽  
pp. 747-776 ◽  
Author(s):  
Joseph L. R. Hayden ◽  
Charles P. Steinmetz
Keyword(s):  
1910 ◽  
Vol 29 (11) ◽  
pp. 1853-1857
Author(s):  
J. L. R. Hayden ◽  
Charles P. Steinmetz
Keyword(s):  

Author(s):  
Nilantha Sapumanage ◽  
Sankha Nanayakkara ◽  
Lasantha Chandimal ◽  
Mahendra Fernando ◽  
Pasan Hettiarachchi ◽  
...  
Keyword(s):  

1985 ◽  
Vol PER-5 (1) ◽  
pp. 41-42 ◽  
Author(s):  
H. Murase ◽  
I. Ohshima ◽  
H. Aoyagi ◽  
I. Miwa

1977 ◽  
Vol 124 (4) ◽  
pp. 383
Author(s):  
D.E. Fletcher ◽  
F. Iliceto ◽  
E. Cinieri ◽  
M. Cazzani ◽  
G. Santagostino
Keyword(s):  

2020 ◽  
Vol 4 (1) ◽  
pp. 67-72
Author(s):  
Plamen Antonov Stanchev ◽  
Mediha Enver Mehmed-Hamza

In the medium voltage electrical power lines, the most common fault is the phase to ground fault. The determining factors for selection of the neutral grounding mode of the medium voltage electrical power lines are the selectivity of the relay protection, the transient voltages during phase to ground fault, the magnitude of the fault currents, etc. The paper studies the influence of the transient resistance of phase to ground fault on the selectivity and sensitivity of the earth fault protection when the neutral of the power transformer is grounded through active resistance in medium voltage power grids.


Geophysics ◽  
1981 ◽  
Vol 46 (6) ◽  
pp. 932-933 ◽  
Author(s):  
T. Lee

Recently Pelton et al. (1978) used a Cole‐Cole relaxation model to simulate the transient voltages that are observed during an induced‐polarization survey. These authors took the impedance of the equivalent circuit Z(ω) to be [Formula: see text]They then gave the expression for the transient voltage [Formula: see text] as [Formula: see text]In equation (2), [Formula: see text] was misprinted as [Formula: see text]. In these equations, [Formula: see text] and [Formula: see text], [Formula: see text] and τ are constants to be determined for the given model. [Formula: see text] is the height of the step current that will flow in the transmitter. A disadvantage of equation (2) is that it is only slowly convergent for large t/τ. Pelton et al. (1978) used a τ which ranged from [Formula: see text] to [Formula: see text]. The purpose of this note is to provide an alternative expression for [Formula: see text] that is valid only at the later stages but which does not have this disadvantage. The trivial case of c = 1.0 is ignored.


1910 ◽  
Vol XXIX (2) ◽  
pp. 1125-1158 ◽  
Author(s):  
Joseph L. R. Hayden ◽  
Charles P. Steinmetz
Keyword(s):  

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