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Chapter 7: Polar Coordinates And Polar Diagrams

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FieldValue
SourceTheory and Calculation of Alternating Current Phenomena
Year1916
Section IDtheory-calculation-alternating-current-phenomena-chapter-07
Locationlines 3619-4087
Statuscandidate
Word Count2051
Equation Candidates In Section25
Figure Candidates In Section7
Quote Candidates In Section0
CHAPTER VII POLAR COORDINATES AND POLAR DIAGRAMS 42. The graphic representation of alternating waves in rec- tangular coordinates, with the time as abscissae and the instan- taneous values as ordinates, gives a picture of their wave structure, as shown in Figs. 1 to 5. It does not, however, show their periodic character as well as the representation in polar coordi- nates, with the time as the angle or the amplitude — one complete period being represented by one revolution — and the instan- taneous values as radius vectors; the polar coordinate system, in which the independent variable, the angle, is periodic, obvi- ously lends itself better to the representation of periodic functions, as alternating waves. Thus the two waves of Figs. 2 and 3 are represented in polar coordinates in Figs. 36 and 37 as
CHAPTER VII POLAR COORDINATES AND POLAR DIAGRAMS 42. The graphic representation of alternating waves in rec- tangular coordinates, with the time as abscissae and the instan- taneous values as ordinates, gives a picture of their wave structure, as shown in Figs. 1 to 5. It does not, however, show their periodic character as well as the representation in polar coordi- nates ...
... differing from the crank diagram discussed in Chapter IV. It may be called the time diagram or polar diagram, and is used to a considerable extent in the literature, thus must be familiar to the engineer, though in the following we shall in graphic representation and in the symbolic representation based thereon, use the crank diagram of Chapters IV and V. In the time diagram as well as in the crank diagram, instead of the maximum value of the wave, the effective value, or square root of mean square, may be used as the vector, which is more convenient ...
... 40.) POLAR COORDINATES AND POLAR DIAGRAMS 49 Kirchhoff's laws now assume, for alternating sine waves, the form : (o) The resultant of all the e.m.fs. in a closed circuit, as found by the parallelogram of sine waves, is zero if the counter e.m.fs. of resistance and of reactance are included. (6) The resultant of all the currents toward a distributing point, as found by the parallelo- gram of sine waves, is zero. The power equation expressed graphically is as follows: The power of an alternating- current circuit is represented in polar coord ...
... GRAMS 42. The graphic representation of alternating waves in rec- tangular coordinates, with the time as abscissae and the instan- taneous values as ordinates, gives a picture of their wave structure, as shown in Figs. 1 to 5. It does not, however, show their periodic character as well as the representation in polar coordi- nates, with the time as the angle or the amplitude — one complete period being represented by one revolution — and the instan- taneous values as radius vectors; the polar coordinate system, in which the independent variable, th ...
Concept CandidateHits In SectionStatus
Ether1seeded
Term CandidateHits In SectionStatus
ether1seeded
Candidate IDOCR / PDF-Text CandidateSource Location
theory-calculation-alternating-current-phenomena-eq-candidate-019043. The sine wave. Fig. 1, is represented in polar coordinatesline 3655
theory-calculation-alternating-current-phenomena-eq-candidate-0191of the wave; and the amplitude of the diameter OC, ^ 0o = AOC,line 3658
theory-calculation-alternating-current-phenomena-eq-candidate-01921 = 1 cos {0 — ^o),line 3662
theory-calculation-alternating-current-phenomena-eq-candidate-0193where 0 = 2ir — is the instantaneous value of the ampHtudeline 3668
theory-calculation-alternating-current-phenomena-eq-candidate-0194for instance, at the amplitude, AOBi = 6i = 2w- (Fig- 38), theline 3676
theory-calculation-alternating-current-phenomena-eq-candidate-0195instantaneous value is OB’; at the amphtude, AOB2 = 62 =line 3680
theory-calculation-alternating-current-phenomena-eq-candidate-01962 Try, the instantaneous value is OB”, and negative, since inline 3682
theory-calculation-alternating-current-phenomena-eq-candidate-0197The angle, 0, so represents the time, and increasing time isline 3687
Candidate IDOCR / PDF-Text CandidateSource Location
theory-calculation-alternating-current-phenomena-fig-037represented by an increase of angle B in counter-clockwise rota- FiG. 37 tion. That is, the positive direction, or increase of time, isline 3691
theory-calculation-alternating-current-phenomena-fig-041^i Fig. 41. Fig. 42.line 3828
theory-calculation-alternating-current-phenomena-fig-042Fig. 41. Fig. 42. then appear in the vector representation of the time diagram orline 3831
theory-calculation-alternating-current-phenomena-fig-043E^-^ Fig. 43. Fig. 45.line 3856
theory-calculation-alternating-current-phenomena-fig-045Fig. 43. Fig. 45. lagging behind the voltage:line 3859
theory-calculation-alternating-current-phenomena-fig-046then means: Fig. 46. POLAR COORDINATES AND POLAR DIAGRAMS 51line 3872
theory-calculation-alternating-current-phenomena-fig-048^ Fig. 48. R’line 4049
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