DocumentCode
1260699
Title
Overdamped condenser oscillations
Author
Steinmetz, Charles P.
Author_Institution
General Electric Co.
Volume
43
Issue
5
fYear
1924
fDate
5/1/1924 12:00:00 AM
Firstpage
424
Lastpage
428
Abstract
In the classical equations of the discharge of a condenser of capacity C into an external circuit of resistance r and inductance L, it is found that the discharge is oscillatory if
, and is impulsive if
As the perfect condenser can never be realized in practise, it is the purpose of this paper to show the effect of the condenser leakage on the discharge wave. The imperfect condenser is represented by the perfect condenser C shunted by the conductance. This condenser discharges into the circuit L and r as above. The mathematical discussion shows that no matter what the relation between r and
, there, may always exist some value of g for which the discharge is oscillatory. This is the case when
It is to be borne in mind that the above holds true only when r, L, C, and g are constant. If the resistance is that of a, third class conductor, the discharge will always be oscillatory. An apparent paradox is found in the statement that the current may be more than 90 deg. out of phase with the voltage. A study of the derived equations, rememberingthat the current under consideration is only one of the two components forming the total discharge current
of the condenser (the leakage current g e being the other), will show that this is true, grams will further confirm the theory.
, and is impulsive if
As the perfect condenser can never be realized in practise, it is the purpose of this paper to show the effect of the condenser leakage on the discharge wave. The imperfect condenser is represented by the perfect condenser C shunted by the conductance. This condenser discharges into the circuit L and r as above. The mathematical discussion shows that no matter what the relation between r and
, there, may always exist some value of g for which the discharge is oscillatory. This is the case when
It is to be borne in mind that the above holds true only when r, L, C, and g are constant. If the resistance is that of a, third class conductor, the discharge will always be oscillatory. An apparent paradox is found in the statement that the current may be more than 90 deg. out of phase with the voltage. A study of the derived equations, rememberingthat the current under consideration is only one of the two components forming the total discharge current
of the condenser (the leakage current g e being the other), will show that this is true, grams will further confirm the theory.fLanguage
English
Journal_Title
A.I.E.E., Journal of the
Publisher
ieee
ISSN
0095-9804
Type
jour
DOI
10.1109/JAIEE.1924.6534780
Filename
6534780
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