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Chapter 40: General System Of Circuits

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FieldValue
SourceTheory and Calculation of Transient Electric Phenomena and Oscillations
Year1909
Section IDtheory-calculation-transient-electric-phenomena-oscillations-chapter-33
Locationlines 12217-12884
Statuscandidate
Word Count1813
Equation Candidates In Section0
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Quote Candidates In Section0
CHAPTER XL GENERAL SYSTEM OF CIRCUITS. (A) Circuits containing resistance and inductance only. 95. Let, upon a general system or network of circuits con- nected with each other directly or inductively, and containing resistance and inductance, but no capacity, a system of e.m.fs., ey be impressed. These e.m.fs. may be of any frequency or wave shape, or may be continuous or anything else, but are supposed to be given by their equations. They may be free of transient terms, or may contain transient terms depending upon the currents in the system. In the latter case, the dependency of the e.m.f. upon the currents must obviously be given. Then, in each branch circuit, ^5~=0, (1) where e = total impressed e.m.f.; r. = resistance; L = induc- tance, of the circuit or branch of circuit traversed
... or inductively, and containing resistance and inductance, but no capacity, a system of e.m.fs., ey be impressed. These e.m.fs. may be of any frequency or wave shape, or may be continuous or anything else, but are supposed to be given by their equations. They may be free of transient terms, or may contain transient terms depending upon the currents in the system. In the latter case, the dependency of the e.m.f. upon the currents must obviously be given. Then, in each branch circuit, ^5~=0, (1) where e = total impressed e.m.f.; r. = resistance; L = in ...
CHAPTER XL GENERAL SYSTEM OF CIRCUITS. (A) Circuits containing resistance and inductance only. 95. Let, upon a general system or network of circuits con- nected with each other directly or inductively, and containing resistance and inductance, but no capacity, a system of e.m.fs., ey be impressed. These e.m.fs. may be of any frequency or wave shape, or may be continuous or anything else, but are supposed to be given by their equations. They may be free of transient terms, or may contain transient terms depending upon the current ...
... gives A-o =0- (11) The n equations (11) must be identities, that is, the coefficients of £~aJ must individually disappear. Each equation (11) thus gives m equations between the constants a, A, b, c, for i = 1, 2, . . . m, and since n equations (11) exist, we get altogether mn equations of the form where -0, q = 1, 2, 3,. . . n and i = 1, 2, 3,. . . m. (12) In addition hereto, the n terminal conditions, or values of current iK" for t = 0: iK°, give by substitution in (9) n further equations, (13) There thus exist (mn + n) eq ...
... ions which represent the transient term. 96. As an example of the application of this method may be considered the following case, sketched diagrammatically in Fig. 42: An alternator of e.m.f. E cos (6 - 00) feeds over resistance rl the primary of a transformer of mutual reactance xm. The secondary of this transformer feeds over resistances r2 and rs the primary of a second transformer of mutual reactance xmo, and the secondary of this second transformer is closed by resist- ance r4. Across the circuit between the two transformers and the two resista ...
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  • Transients / damping: Separate the temporary term from the final steady-state term and compare with differential-equation response language.
  • 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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