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Chapter 9: Divided Circuit

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FieldValue
SourceTheory and Calculation of Transient Electric Phenomena and Oscillations
Year1909
Section IDtheory-calculation-transient-electric-phenomena-oscillations-chapter-31
Locationlines 9228-10474
Statuscandidate
Word Count3576
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CHAPTER IX. DIVIDED CIRCUIT. 72. A circuit consisting of two branches or multiple circuits 1 and 2 may be supplied, over a line or circuit 3, with an impressed e.m.f., e0. Let, in such a circuit, shown diagrammatically in Fig 31, rv Lv Cl and r2, L2, Cz — resistance, inductance, and capacity, respectively, of the two branch circuits 1 and 2; r0, L0, C0 = Co Fig. 31. Divided circuit. resistance, inductance, and capacity of the undivided part of the circuit, 3. Furthermore let e = potential difference at terminals of branch circuits 1 and 2, it and i2 respectively = currents in branch circuits 1 and 2, and i3 = current in undivided part of circuit, 3. Then ia = il + i2 and e.m.f. at the terminals of circuit 1 is of
... DIVIDED CIRCUIT. 72. A circuit consisting of two branches or multiple circuits 1 and 2 may be supplied, over a line or circuit 3, with an impressed e.m.f., e0. Let, in such a circuit, shown diagrammatically in Fig 31, rv Lv Cl and r2, L2, Cz — resistance, inductance, and capacity, respectively, of the two branch circuits 1 and 2; r0, L0, C0 = Co Fig. 31. Divided circuit. resistance, inductance, and capacity of the undivided part of the circuit, 3. Furthermore let e = potential difference at terminals of branch circuits 1 and 2, it and i2 respec ...
... e.m.f. at the terminals of circuit 1 is of circuit 2 is e = di 121 (2) (3) 122 TRANSIENT PHENOMENA and of circuit 3 is (4) Instead of the inductances, L, and capacities, C, it is usually preferable, even in direct-current circuits, to introduce the reactances, x = 2 nfL = inductive reactance, xc = = con- 2 7T/G densive reactance, referred to a standard frequency, such as / = 60 cycles per second. Instead of the time t, then, an angle 0 = 2 nft (5) is introduced, and then we have di x di dd di ^ * (6) i/iift - 2 Kfo f ...
... terminals of branch circuits 1 and 2, it and i2 respectively = currents in branch circuits 1 and 2, and i3 = current in undivided part of circuit, 3. Then ia = il + i2 and e.m.f. at the terminals of circuit 1 is of circuit 2 is e = di 121 (2) (3) 122 TRANSIENT PHENOMENA and of circuit 3 is (4) Instead of the inductances, L, and capacities, C, it is usually preferable, even in direct-current circuits, to introduce the reactances, x = 2 nfL = inductive reactance, xc = = con- 2 7T/G densive reactance, referred to a standard ...
... 3 the engineer who is mainly familiar with the effect of inductance in alternating-current circuits. Substituting therefore (5) and (6) in equations (2), (3), (4), gives the e.m.f. in circuit 1 as dL e = rli1 + xl -r1 + a in circuit 2 as dL ' C * = r** + **-fi + *ctJi,M', (8) in circuit 3 as e = e a. r { 4. x -h. _j_ x I { ^. /Q\ 0 03 ' 0 J/j ' CQ I 3 J v*^/ tZC7 «/ hence, the potential differences at the condenser terminals are /di< i,dd = e-r1i1- xt— S (10) e2= <J *i dd = e- r2i2 -*,-^> (11) and e3 = xco I i3dd = e0- e - r0i ...
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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.
  • Impedance / reactance: Translate historical opposition terms into modern impedance, admittance, conductance, susceptance, and complex-plane notation.
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