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Lecture 2: The Electric Field

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FieldValue
SourceElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients
Year1914
Section IDelectric-discharges-waves-impulses-1914-lecture-02
Locationlines 1003-1658
Statuscandidate
Word Count2159
Equation Candidates In Section38
Figure Candidates In Section0
Quote Candidates In Section0
LECTURE II. THE ELECTRIC FIELD. 7. Let, in Fig. 7, a generator G transmit electric power over line A into a receiving circuit M. While power flows through the conductors A, power is con- sumed in these conductors by JV[ conversion into heat, repre- sented by ^2r. This, however, Fig. 7. is not all, but in the space surrounding the conductor cer- tain phenomena occur: magnetic and electrostatic forces appear. Fig. 8. — Electric Field of Conductor. The conductor is surrounded by a magnetic field, or a magnetic flux, which is measured by the number of lines of magnetic force $. With a single conductor, the lines of magnetic force are concentric circles, as shown in Fig. 8. By the return conductor, the circles 10 THE ELECTRIC FIELD. 11 are crowded together between the conductors,
LECTURE II. THE ELECTRIC FIELD. 7. Let, in Fig. 7, a generator G transmit electric power over line A into a receiving circuit M. While power flows through the conductors A, power is con- sumed in these conductors by JV[ conversion into heat, repre- sented by ^2r. This, however, Fig. 7. is not all, b ...
... A into a receiving circuit M. While power flows through the conductors A, power is con- sumed in these conductors by JV[ conversion into heat, repre- sented by ^2r. This, however, Fig. 7. is not all, but in the space surrounding the conductor cer- tain phenomena occur: magnetic and electrostatic forces appear. Fig. 8. — Electric Field of Conductor. The conductor is surrounded by a magnetic field, or a magnetic flux, which is measured by the number of lines of magnetic force $. With a single conductor, the lines of magnetic force are concentric ...
... iving circuit M. While power flows through the conductors A, power is con- sumed in these conductors by JV[ conversion into heat, repre- sented by ^2r. This, however, Fig. 7. is not all, but in the space surrounding the conductor cer- tain phenomena occur: magnetic and electrostatic forces appear. Fig. 8. — Electric Field of Conductor. The conductor is surrounded by a magnetic field, or a magnetic flux, which is measured by the number of lines of magnetic force $. With a single conductor, the lines of magnetic force are concentric circles, as shown ...
... circuit. $ = L^.* (1) The magnetic field represents stored energy ly. To produce it, power, p, must therefore be supplied by the circuit. Since power is current times voltage : P = e'i, (2) * n^, if the flux <l> interlinks the circuit n fold. 12 ELECTRIC DISCHARGES, WAVES AND IMPULSES. to produce the magnetic field $ of the current i, a voltage e' must be consumed in the circuit, which with the current i gives the power p, which supplies the stored energy w of the magnetic field $. This voltage e' is called the inductance voltage, or voltag ...
Concept CandidateHits In SectionStatus
Ether3seeded
Light2seeded
Magnetic permeability2seeded
Velocity of light2seeded
Term CandidateHits In SectionStatus
ether3seeded
Candidate IDOCR / PDF-Text CandidateSource Location
electric-discharges-waves-impulses-1914-eq-candidate-0007$ = L^.* (1)line 1063
electric-discharges-waves-impulses-1914-eq-candidate-0008P = e’i, (2)line 1069
electric-discharges-waves-impulses-1914-eq-candidate-0009e’ = L§ (4)line 1088
electric-discharges-waves-impulses-1914-eq-candidate-0010^ = — (5)line 1108
electric-discharges-waves-impulses-1914-eq-candidate-00119. Exactly analogous relations exist in the dielectric field.line 1116
electric-discharges-waves-impulses-1914-eq-candidate-0012^ = Ce. (6)line 1122
electric-discharges-waves-impulses-1914-eq-candidate-0013p = i’e, (7)line 1129
electric-discharges-waves-impulses-1914-eq-candidate-0014i’ = C* (9)line 1149
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