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Lecture 3: Single-Energy Transients In Continuous Current Circuits

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FieldValue
SourceElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients
Year1914
Section IDelectric-discharges-waves-impulses-1914-lecture-03
Locationlines 1659-2484
Statuscandidate
Word Count2625
Equation Candidates In Section31
Figure Candidates In Section0
Quote Candidates In Section0
LECTURE III. SINGLE-ENERGY TRANSIENTS IN CONTINUOUS- CURRENT CIRCUITS. 13. The simplest electrical transients are those in circuits in which energy can be stored in one form only, as in this case the change of stored energy can consist only of an increase or decrease ; but no surge or oscillation between several forms of energy can exist. Such circuits are most of the low- and medium-voltage circuits, — 220 volts, 600 volts, and 2200 volts. In them the capac- ity is small, due to the limited extent of the circuit, resulting from the low voltage, and at the low voltage the dielectric energy thus is negligible, that is, the circuit stores appreciable energy only by the magnetic field. A circuit of considerable capacity, but negligible inductance, if of high resistance, would also give one form
... its, — 220 volts, 600 volts, and 2200 volts. In them the capac- ity is small, due to the limited extent of the circuit, resulting from the low voltage, and at the low voltage the dielectric energy thus is negligible, that is, the circuit stores appreciable energy only by the magnetic field. A circuit of considerable capacity, but negligible inductance, if of high resistance, would also give one form of energy storage only, in the dielectric field. The usual high-voltage capacity circuit, as that of an electrostatic machine, while of very small inductanc ...
LECTURE III. SINGLE-ENERGY TRANSIENTS IN CONTINUOUS- CURRENT CIRCUITS. 13. The simplest electrical transients are those in circuits in which energy can be stored in one form only, as in this case the change of stored energy can consist only of an increase or decrease ; but no surge or oscillation between sev ...
... its, — 220 volts, 600 volts, and 2200 volts. In them the capac- ity is small, due to the limited extent of the circuit, resulting from the low voltage, and at the low voltage the dielectric energy thus is negligible, that is, the circuit stores appreciable energy only by the magnetic field. A circuit of considerable capacity, but negligible inductance, if of high resistance, would also give one form of energy storage only, in the dielectric field. The usual high-voltage capacity circuit, as that of an electrostatic machine, while of very small inductance, al ...
... % io A C c c ..1. 1 Fig. 10. — Magnetic Single-energy Transient. negligible capacity), a magnetic field $0 10' Lio interlinks with the coil. Assuming now that the voltage eo is suddenly withdrawn, without changing 19 20 ELECTRIC DISCHARGES, WAVES AND IMPULSES. the constants of the coil circuit, as for instance by short- circuiting the terminals of the coil, as indicated at A. With no voltage impressed upon the coil, and thus no power supplied to it, current i and magnetic flux $ of the coil must finally be zero. ...
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electric-discharges-waves-impulses-1914-eq-candidate-0045Fig. 10. — Magnetic Single-energyline 1719
electric-discharges-waves-impulses-1914-eq-candidate-004611 A, the flux is constant and denoted by $0 up to the moment ofline 1753
electric-discharges-waves-impulses-1914-eq-candidate-0047Fig. 11. — Characteristics of Magnetic Single-energy Transient.line 1782
electric-discharges-waves-impulses-1914-eq-candidate-0048Co up to to, and drops to 0 at ^o- However, since after ^0 a currentline 1790
electric-discharges-waves-impulses-1914-eq-candidate-0049SINGLE-ENERGY TRANSIENTS. 21line 1797
electric-discharges-waves-impulses-1914-eq-candidate-0050Zet = n$olO-« = Lio. (2)line 1842
electric-discharges-waves-impulses-1914-eq-candidate-0051T = -. (4)line 1871
electric-discharges-waves-impulses-1914-eq-candidate-0052Using the time constant 7” = - as unit of length for the abscissa,line 1913
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  • Magnetism: Track flux, reluctance, permeability, magnetizing force, and loss language against modern magnetic-circuit terminology.
  • Transients / damping: Separate the temporary term from the final steady-state term and compare with differential-equation response language.
  • Field language: Read for whether field language is mechanical, geometrical, causal, descriptive, or simply a convenient engineering model.
  • Waves / transmission lines: Map Steinmetz’s wave and line language onto modern distributed constants, propagation velocity, standing waves, and reflections.
  • Lightning / surges: Connect the passage to switching surges, traveling waves, reflections, insulation stress, and protection practice.
  • Magnetism: Centrifugal/divergent magnetic-field readings are interpretive overlays, not automatic historical claims.
  • Transients / damping: Transient collapse, impulse, and surge behavior can be compared with alternative field language, but only as a clearly marked reading.
  • Field language: Field-pressure or field-gradient interpretations can be explored here only after the explicit source passage and modern engineering translation are kept distinct.
  • Waves / transmission lines: Standing/traveling wave passages may support richer field interpretations; the page keeps those readings separate from verified Steinmetz wording.
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