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Chapter 5: Resistance, Inductance, And Capacity In Series Condenser Charge And Discharge

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FieldValue
SourceTheory and Calculation of Transient Electric Phenomena and Oscillations
Year1909
Section IDtheory-calculation-transient-electric-phenomena-oscillations-chapter-27
Locationlines 4072-5311
Statuscandidate
Word Count2722
Equation Candidates In Section0
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Quote Candidates In Section0
CHAPTER V. RESISTANCE, INDUCTANCE, AND CAPACITY IN SERIES. CONDENSER CHARGE AND DISCHARGE. 29. If a continuous e.m.f . e is impressed upon a circuit contain- ing resistance, inductance, and capacity in series, the stationary condition of the circuit is zero current, i = o, and the poten- tial difference at the condenser equals the impressed e.m.f., et =• e, no permanent current exists, but only the transient current of charge or discharge of the condenser. The capacity C of a condenser is defined by the equation . de that is, the current into a condenser is proportional to the rate of increase of its e.m.f. and to the capacity. It is therefore and e-^-lidt (1) is the potential difference at the terminals of a condenser of capacity C with current i in the circuit to
CHAPTER V. RESISTANCE, INDUCTANCE, AND CAPACITY IN SERIES. CONDENSER CHARGE AND DISCHARGE. 29. If a continuous e.m.f . e is impressed upon a circuit contain- ing resistance, inductance, and capacity in series, the stationary condition of the circuit is zero current, i = o, and the poten- tial difference at the condenser ...
... pressed upon a circuit contain- ing resistance, inductance, and capacity in series, the stationary condition of the circuit is zero current, i = o, and the poten- tial difference at the condenser equals the impressed e.m.f., et =• e, no permanent current exists, but only the transient current of charge or discharge of the condenser. The capacity C of a condenser is defined by the equation . de that is, the current into a condenser is proportional to the rate of increase of its e.m.f. and to the capacity. It is therefore and e-^-lidt (1) is t ...
... 10.2 £-200' sin 980*; the condenser potential is e, - 1000 { 1 - e" 20° ' (cos 980 t + 0.21 sin 980 0 } . 62 TRANSIENT PHENOMENA 41. Since the equations of current and potential difference (42) to (47) contain trigonometric functions, the phenomena are periodic or waves, similar to alternating currents. They r differ from the latter by containing an exponential factor e 2 L , which steadily decreases with increase of t. That is, the sue- 16UUI — f ^ f N, c = « 1QOO volts L = = 1 X)mh 1 X \ T = 40 oh, as ...
... the dependent vari- able, i, and its differential quotients, and as such is integrated by an exponential function of the general form i = Ae-*. (6) (This exponential function also includes the trigonometric functions sine and cosine, which are exponential functions with imaginary exponent a.) CONDENSER CHARGE AND DISCHARGE 49 Substituting (6) in (5) gives this must be an identity, irrespective of the value of t, to make (6) the integral of (5). That is, a?L-ar+- = Q. (7) A is still indefinite, and therefore determined by the terminal condit ...
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  • Dielectricity / capacity: Check whether the passage treats capacity, condensers, displacement, or dielectric stress as field storage rather than only circuit algebra.
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  • Dielectricity / capacity: A Wheeler-style reading may emphasize dielectric compression, field stress, and stored potential, but this page treats that as interpretation unless Steinmetz explicitly says it.
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