Theory and Calculation of Alternating Current Phenomena Visual Map

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Theory and Calculation of Alternating Current Phenomena, Chapter V, printed page 30, PDF page 58; Fig. 21

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Theory and Calculation of Alternating Current Phenomena, Chapter V, printed page 31, PDF page 59; Fig. 22

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Theory and Calculation of Alternating Current Phenomena, Chapter V, printed page 32, PDF page 60; Fig. 23

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Theory and Calculation of Alternating Current Phenomena, Chapter V, printed page 33, PDF page 61; Fig. 24

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Modern Guide Diagrams Keyed To This Source

Rotating Magnetic Field From Quadrature Fluxes

Modern reading aid for induction-machine field language in AC and Theoretical Elements sources.

symbolic-method, magnetism, phase, induction-motor

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Admittance Plane

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admittance, conductance, susceptance, symbolic-method

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Hysteresis Loss Law

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hysteresis, magnetic-loss, effective-resistance

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Engineering Number Plane

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complex-quantities, number, symbolic-method

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AC Symbolic Method Redraw Sheet

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symbolic-method, complex-quantities, phasor, operator-j

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Phasor And Symbolic Method

Modern reading aid for vector and complex-number representation of alternating quantities.

symbolic-method, complex-quantities, phase, phasor

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Hysteresis Loop

Modern guide for magnetic lag, loop area, and energy loss per cycle.

hysteresis, magnetism, magnetic-loss, effective-resistance

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Impedance And Reactance Triangle

Modern guide for resistance, reactance, impedance, phase angle, and symbolic quantities.

impedance, reactance, power-factor, symbolic-method

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Candidate Figure References

Candidate	Caption lead	Section	Routes
theory-calculation-alternating-current-phenomena-fig-006 Fig. 6	maximum variation of the sine is equal to the variation of the Fig. 6. Fig. 7.	Chapter 2: Instantaneous Values And Integral Values	source workbench
theory-calculation-alternating-current-phenomena-fig-007 Fig. 7	Fig. 6. Fig. 7. corresponding arc, and consequently the maximum variation of	Chapter 2: Instantaneous Values And Integral Values	source workbench
theory-calculation-alternating-current-phenomena-fig-010 Fig. 10	21 Fig. 10. phase angle — /3’ = — (a’ — ??]) = 10 A, and the equations of	Chapter 4: Vector Representation	source workbench
theory-calculation-alternating-current-phenomena-fig-016 Fig. 16	^E, Fig. 16. Fig. 17.	Chapter 4: Vector Representation	source workbench
theory-calculation-alternating-current-phenomena-fig-017 Fig. 17	Fig. 16. Fig. 17. the current by the angle, Q. The voltage consumed by the resist-	Chapter 4: Vector Representation	source workbench
theory-calculation-alternating-current-phenomena-fig-019 Fig. 19	Ei-< «; Fig. 19. The primary impressed e.m.f., Ep, must thus consist of the three components OEi, OEr, and OE^, and is, therefore, their	Chapter 4: Vector Representation	source workbench
theory-calculation-alternating-current-phenomena-fig-024 Fig. 24	33 Fig. 24. polar coordinates by a vector of opposite direction, and denoted	Chapter 5: Symbolic Method	source workbench
theory-calculation-alternating-current-phenomena-fig-025 Fig. 25	,,U— — L Fig. 25. Fig. 26.	Chapter 6: Topographic Method	source workbench
theory-calculation-alternating-current-phenomena-fig-026 Fig. 26	Fig. 25. Fig. 26. in the opposite direction, from terminal B to terminal A in op-	Chapter 6: Topographic Method	source workbench
theory-calculation-alternating-current-phenomena-fig-029 Fig. 29	NON-INDUCTIVE LOAD Fig. 29. Fig. 30.	Chapter 6: Topographic Method	source workbench
theory-calculation-alternating-current-phenomena-fig-030 Fig. 30	Fig. 29. Fig. 30. these currents are represented in Fig. 29 by the vectors 01 1 =	Chapter 6: Topographic Method	source workbench
theory-calculation-alternating-current-phenomena-fig-031 Fig. 31	CAPACIir AND RESISTANCE Fig. 31. Fig. 32.	Chapter 6: Topographic Method	source workbench
theory-calculation-alternating-current-phenomena-fig-032 Fig. 32	Fig. 31. Fig. 32. triangle, Ei^E^^Ez^, the voltages at the receiver’s circuit, Ei, E2,	Chapter 6: Topographic Method	source workbench
theory-calculation-alternating-current-phenomena-fig-033 Fig. 33	RESISTANCE AND LEAKAGE Fig. 33. 16 I TRANSMISSION	Chapter 6: Topographic Method	source workbench
theory-calculation-alternating-current-phenomena-fig-034 Fig. 34	90” LAG Fig. 34. and generator currents, /i”, 72°, I^, over the topographical char-	Chapter 6: Topographic Method	source workbench
theory-calculation-alternating-current-phenomena-fig-035 Fig. 35	RESISTANCE AND LEAKAGE Fig. 35. their difference of phase are plotted in Fig. 35 in rectangular	Chapter 6: Topographic Method	source workbench
theory-calculation-alternating-current-phenomena-fig-037 Fig. 37	represented by an increase of angle B in counter-clockwise rota- FiG. 37 tion. That is, the positive direction, or increase of time, is	Chapter 7: Polar Coordinates And Polar Diagrams	source workbench
theory-calculation-alternating-current-phenomena-fig-041 Fig. 41	^i Fig. 41. Fig. 42.	Chapter 7: Polar Coordinates And Polar Diagrams	source workbench
theory-calculation-alternating-current-phenomena-fig-042 Fig. 42	Fig. 41. Fig. 42. then appear in the vector representation of the time diagram or	Chapter 7: Polar Coordinates And Polar Diagrams	source workbench
theory-calculation-alternating-current-phenomena-fig-043 Fig. 43	E^-^ Fig. 43. Fig. 45.	Chapter 7: Polar Coordinates And Polar Diagrams	source workbench
theory-calculation-alternating-current-phenomena-fig-045 Fig. 45	Fig. 43. Fig. 45. lagging behind the voltage:	Chapter 7: Polar Coordinates And Polar Diagrams	source workbench
theory-calculation-alternating-current-phenomena-fig-046 Fig. 46	then means: Fig. 46. POLAR COORDINATES AND POLAR DIAGRAMS 51	Chapter 7: Polar Coordinates And Polar Diagrams	source workbench
theory-calculation-alternating-current-phenomena-fig-048 Fig. 48	^ Fig. 48. R’	Chapter 7: Polar Coordinates And Polar Diagrams	source workbench
theory-calculation-alternating-current-phenomena-fig-049 Fig. 49	7 1.8 Fig. 49. The sign in the complex expression of admittance is always opposite to that of impedance; this is obvious, since if the cur-	Chapter 8: Admittance, Conductance, Susceptance	source workbench
theory-calculation-alternating-current-phenomena-fig-051 Fig. 51	Eo E Fig. 51. M	Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-052 Fig. 52	Eo Fig. 52. Fig. 53.	Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-053 Fig. 53	Fig. 52. Fig. 53. 2. Reactance in Series with a Circuit	Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-054 Fig. 54	ohms inductance-’— reactance-^condensance Fig. 54. E^, are shown for various conditions of a receiver circuit and	Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-055 Fig. 55	0 Fig. 55. Fig. 56.	Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-056 Fig. 56	Fig. 55. Fig. 56. Fig. 57.	Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-057 Fig. 57	Fig. 56. Fig. 57. is, the current and e.m.f. in the supply circuit are in phase with	Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-058 Fig. 58	^w=+90 80 70 60 50 40 30 20 10 0 10 20 30 40 50 60 70 80 90 degrees lag-«- phase difference in consumer circuit-*- lead Fig. 58. In Figs. 59 and 60, the same curves are plotted as in Fig. 58, but in Fig. 59 with the r…	Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-059 Fig. 59	+1 +.9 +.8 +.7 +.6 +.5 +.4 +.3 +.2 +.1 0 -.1 -.2 -.3 -.4 -.5 -.6 reactance of consumer circuit Fig. 59. -.7 -.8 -.9-10	Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-060 Fig. 60	_ resistance of . consumer circuit Fig. 60. ,7 .6 .5 .4 .3 .2 .1 .0	Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-061 Fig. 61	1. .9 .8 .7 .6 .5 ,4 .3 .2 .1 0 -.1 -.2 -.3 -.1 -.5 -.6 -.7 -.8 -.9-L X — ^ Fig. 61. E	Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-062 Fig. 62	tro Fig. 62. Fig. 63.	Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-063 Fig. 63	Fig. 62. Fig. 63. 72	Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-065 Fig. 65	loss of power. Fig. 65. Then, if Eo = impressed e.m.f., the current in receiver circuit is	Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-067 Fig. 67	1 Fig. 67. 5. Constant Potential — Constant-current Transformation	Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-068 Fig. 68	supply, and inversely. Fig. 68 The generation of alternating-current electric power almost always takes place at constant potential. For some purposes,	Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-072 Fig. 72	0 Fig. 72. .03 ,03 M. .05 .00 .07 .OS	Chapter 10: Resistance And Reactance Of Transmission	source workbench
theory-calculation-alternating-current-phenomena-fig-076 Fig. 76	» Fig. 76. 10 20 30 10 50 60 7.0 .80 90 100	Chapter 10: Resistance And Reactance Of Transmission	source workbench
theory-calculation-alternating-current-phenomena-fig-077 Fig. 77	AMPERES LOAD « l Fig. 77. and the leading quadrature component of current required to compensate for the line reactance x at maximum current, im, is	Chapter 11: Phase Control	source workbench
theory-calculation-alternating-current-phenomena-fig-078 Fig. 78	::} Fig. 78. 87. Equation (28) shows that there are two values of x: Xi and X2; and corresponding thereto two values of 60:^01 and 602,	Chapter 11: Phase Control	source workbench
theory-calculation-alternating-current-phenomena-fig-081 Fig. 81	^ Fig. 81. The general character of these current waves is, that the maxi-	Chapter 12: Effective Resistance And Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-082 Fig. 82	then Fig. 82. — X^	Chapter 12: Effective Resistance And Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-086 Fig. 86	n = NUMBER OF TURNS Fig. 86. 350	Chapter 12: Effective Resistance And Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-087 Fig. 87	/ = FREQUENCY Fig. 87. 400	Chapter 12: Effective Resistance And Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-088 Fig. 88	200 250 Fig. 88. 300	Chapter 12: Effective Resistance And Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-089 Fig. 89	/=CYCLES Fig. 89. 300	Chapter 12: Effective Resistance And Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-090 Fig. 90	n=NUMBER OF TURNS Fig. 90. 350	Chapter 12: Effective Resistance And Reactance	source workbench
theory-calculation-alternating-current-phenomena-fig-092 Fig. 92	magnetic flux inclosed by the zone is SuV. Fig. 92. Hence, the e.m.f. generated in this zone is	Chapter 13: Foucault Or Eddy Currents	source workbench
theory-calculation-alternating-current-phenomena-fig-093 Fig. 93	93. Fig. 93. 110. Demagnetizing, or screening effect of eddy currents.	Chapter 13: Foucault Or Eddy Currents	source workbench
theory-calculation-alternating-current-phenomena-fig-094 Fig. 94	du Fig. 94. The current inclosed by this zone is /„	Chapter 13: Foucault Or Eddy Currents	source workbench
theory-calculation-alternating-current-phenomena-fig-096 Fig. 96	^ m Fig. 96. )J	Chapter 14: Dielectric Losses	source workbench
theory-calculation-alternating-current-phenomena-fig-097 Fig. 97	’ m Fig. 97. throughout the field section, but the voltage gradient in the	Chapter 14: Dielectric Losses	source workbench
theory-calculation-alternating-current-phenomena-fig-098 Fig. 98	do so. Fig. 98. Fig. 99.	Chapter 14: Dielectric Losses	source workbench
theory-calculation-alternating-current-phenomena-fig-099 Fig. 99	Fig. 98. Fig. 99. h’5	Chapter 14: Dielectric Losses	source workbench
theory-calculation-alternating-current-phenomena-fig-100 Fig. 100	JTTTTTTTTTTTTTTTTTTTTTTT- Fig. 100. In this case the intensity as well as phase of the current, and consequently of the counter e.m.f. of inductive reactance and	Chapter 15: Distributed Capacity, Inductance, Resistance, And Leakage	source workbench
theory-calculation-alternating-current-phenomena-fig-101 Fig. 101	iEo Fig. 101. Denoting in Fig. 101.	Chapter 15: Distributed Capacity, Inductance, Resistance, And Leakage	source workbench