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Ether And Field Language Evidence

Evidence status: generated from processed OCR/PDF text. Treat each hit as a source-location aid until the passage is checked against the scan.

4352 hits

Total text matches across processed Steinmetz sections.

15 sources

Sources containing at least one matched alias.

283 sections

Chapters, lectures, sections, or report divisions with matches.

Source-located passages where Steinmetz uses ether, field, force, stress, strain, pressure, tension, medium, displacement, or related older field vocabulary.

Source Evidence

Use the tables and snippets below to locate Steinmetz passages. Exact wording still needs scan verification before canonical quotation.

Modern Reading Prompt

Read these passages first as historical electrical field language. Translate only after checking whether Steinmetz is describing a mathematical field, a material medium, an analogy, or a physical ontology.

Interpretive Boundary

Ether-field readings may compare this language with later nonstandard vocabularies, but the page itself only proves that the words occur in the processed Steinmetz text.

AliasHits
field3583
displacement224
pressure114
fields111
medium108
tension80
ether66
field of force40
strain37
stress29
SourceHitsSections
Theoretical Elements of Electrical Engineering68479
Theory and Calculation of Electric Apparatus65120
Theory and Calculation of Transient Electric Phenomena and Oscillations47831
Theory and Calculation of Alternating Current Phenomena40228
General Lectures on Electrical Engineering30914
Four Lectures on Relativity and Space2923
Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients27810
Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients27210
Theory and Calculation of Alternating Current Phenomena25922
Theory and Calculation of Electric Circuits23415
Theory and Calculation of Alternating Current Phenomena21919
Radiation, Light and Illumination14910
Engineering Mathematics: A Series of Lectures Delivered at Union College576
Investigation of Some Trouble in the Generating System of the Commonwealth Edison Co.374
America and the New Epoch3112
SectionSourceHitsTop matched aliasesWorkbenchLocation
Chapter 20: Single-Phase Commutator MotorsTheory and Calculation of Electric Apparatus306field (297), displacement (6), medium (3)Workbenchlines 23906-30087
Lecture 4: Single-Energy Transients In Alternating Current CircuitsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients137field (134), fields (3)Workbenchlines 2485-3386
Lecture 2: Conclusions From The Relativity TheoryFour Lectures on Relativity and Space134field (78), ether (52), field of force (7), fields (2), medium (1)Workbenchlines 736-2388
Lecture 4: Single-Energy Transients In Alternating Current CircuitsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients133field (130), fields (3)Workbenchlines 2162-2971
Lecture 14: Alternating Current Railway MotorGeneral Lectures on Electrical Engineering129field (129)Workbenchlines 8649-9342
Lecture 3: Gravitation And The Gravitational FleldFour Lectures on Relativity and Space102field (99), field of force (2), fields (2), ether (1)Workbenchlines 2389-3594
Chapter 22: Armature Reactions Of AlternatorsTheory and Calculation of Alternating Current Phenomena91field (91)Workbenchlines 23971-25134
Chapter 13: Reactance Of Synchronous MachinesTheory and Calculation of Electric Circuits77field (76), fields (1)Workbenchlines 23466-24022
Chapter 14: Short-Circuit Currents Of AlternatorsTheory and Calculation of Transient Electric Phenomena and Oscillations72field (72)Workbenchlines 14549-15353
Chapter 10: Mutual InductanceTheory and Calculation of Transient Electric Phenomena and Oscillations66field (65), tension (1)Workbenchlines 10475-12216
Theory Section 19: Fields of ForceTheoretical Elements of Electrical Engineering65field (54), fields (10), field of force (7), medium (1)Workbenchlines 7737-7990
Lecture 2: The Electric FieldElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients61field (58), fields (3)Workbenchlines 1003-1658
Lecture 2: The Electric FieldElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients61field (58), fields (3)Workbenchlines 883-1530
Chapter 8: Velocity Of Propagation Of Electric FieldTheory and Calculation of Transient Electric Phenomena and Oscillations59field (55), fields (4)Workbenchlines 26095-27002
Chapter 1: The Constants Of The Electric CircuitTheory and Calculation of Transient Electric Phenomena and Oscillations58field (50), stress (5), medium (2), fields (1)Workbenchlines 1317-1992
Lecture 4: The Characteristics Of Space A. The Geometry Of The Gravitational FieldFour Lectures on Relativity and Space56field (46), ether (6), fields (3), medium (1)Workbenchlines 3595-6820
Chapter 3: Inductance And Resistance In Continuous Current CircuitsTheory and Calculation of Transient Electric Phenomena and Oscillations56field (55), fields (1)Workbenchlines 2659-3514
Theory Section 1: Magnetism and Electric CurrentTheoretical Elements of Electrical Engineering55field (45), fields (5), medium (5), field of force (1)Workbenchlines 477-909
Chapter 14: Dielectric LossesTheory and Calculation of Alternating Current Phenomena52field (40), displacement (3), fields (3), pressure (3), stress (3)Workbenchlines 14334-15409
Chapter 4: Induction Motor With Secondary ExcitationTheory and Calculation of Electric Apparatus52field (52)Workbenchlines 5555-8554
Chapter 21: Alternating-Current GeneratorTheory and Calculation of Alternating Current Phenomena48field (46), displacement (2)Workbenchlines 22302-23970
Chapter 17: Inductor MachinesTheory and Calculation of Electric Apparatus47field (47)Workbenchlines 20294-20974
Chapter 21: Regulating Pole ConvertersTheory and Calculation of Electric Apparatus47field (45), displacement (2)Workbenchlines 30088-31715
Chapter 17: Alternating-Current GeneratorTheory and Calculation of Alternating Current Phenomena45field (43), displacement (2)Workbenchlines 16362-17596
Lecture 17: Arc LightingGeneral Lectures on Electrical Engineering43field (22), pressure (12), stress (4), medium (3), ether (1)Workbenchlines 9920-12795
Chapter 24: Synchronous MotorTheory and Calculation of Alternating Current Phenomena42field (22), displacement (20)Workbenchlines 25682-29374
Chapter 19: Commutatob MotobsTheory and Calculation of Alternating Current Phenomena41field (38), displacement (3)Workbenchlines 21339-22387
Chapter 20: Commutator MotorsTheory and Calculation of Alternating Current Phenomena41field (38), displacement (3)Workbenchlines 19458-20501
Chapter 16: Aiitebnatingh-Current OsnebatorTheory and Calculation of Alternating Current Phenomena37field (35), displacement (2)Workbenchlines 17025-18828
Chapter 11: Phase ControlTheory and Calculation of Alternating Current Phenomena36field (35), fields (1)Workbenchlines 9767-10717
Lecture 6: LuminescenceRadiation, Light and Illumination35pressure (30), field (4), tension (1)Workbenchlines 5077-6608
Chapter 9: Inductive DischargesTheory and Calculation of Transient Electric Phenomena and Oscillations35field (34), pressure (1)Workbenchlines 34897-40349
Apparatus Section 17: Synchronous Machines: Short-circuit Currents of AlternatorsTheoretical Elements of Electrical Engineering34field (34)Workbenchlines 10190-10429
Chapter 2: Potential Series And Exponential FunctionEngineering Mathematics: A Series of Lectures Delivered at Union College33field (30), pressure (3)Workbenchlines 3492-6063
Lecture 13: Electric Railway: Motor CharacteristicsGeneral Lectures on Electrical Engineering33field (33)Workbenchlines 7124-8648
Chapter 16: Reaction MachinesTheory and Calculation of Electric Apparatus33field (31), displacement (1), fields (1)Workbenchlines 19374-20293
Chapter 23: ReviewTheory and Calculation of Electric Apparatus33field (29), fields (2), displacement (1), medium (1)Workbenchlines 32138-32819
Chapter 11: Foucault Or Eddy CurrentsTheory and Calculation of Alternating Current Phenomena32field (28), field of force (3), medium (3), fields (1)Workbenchlines 8384-9380
Apparatus Section 1: Induction Machines: GeneralTheoretical Elements of Electrical Engineering31field (27), fields (3), field of force (2), displacement (1)Workbenchlines 18949-19165
Chapter 11: Fouoault Or Eddy 0Ubbent8Theory and Calculation of Alternating Current Phenomena30field (26), field of force (3), medium (3), fields (1)Workbenchlines 10500-11563
Chapter 3: MagnetismTheory and Calculation of Electric Circuits30field (28), fields (2)Workbenchlines 5445-6941
Chapter 16: Induction MotorTheory and Calculation of Alternating Current Phenomena27field (20), displacement (7)Workbenchlines 13649-16361
Chapter 12: Frequency Converter Or General Alternating Current TransformerTheory and Calculation of Electric Apparatus27field (27), field of force (1)Workbenchlines 14897-17124
Lecture 2: Relation Of Bodies To RadiationRadiation, Light and Illumination26medium (23), ether (1), field (1), pressure (1)Workbenchlines 1549-2365
Apparatus Subsection 79: Direct-current Commutating Machines: C. Commutating Machines 219Theoretical Elements of Electrical Engineering26field (26)Workbenchlines 13019-13119
Chapter 2: Electric Conduction. Gas And VaporTheory and Calculation of Electric Circuits26pressure (26)Workbenchlines 3895-5444
Chapter 7: Shaping Of Waves : GeneralTheory and Calculation of Electric Circuits25field (22), strain (2), stress (1)Workbenchlines 12222-12961
Mathematical Appendix 5: Appendix: Synchronous OperationInvestigation of Some Trouble in the Generating System of the Commonwealth Edison Co.24field (12), displacement (10), fields (1), strain (1)WorkbenchPDF pages 27-68, lines 2165-5013
Lecture 10: Continual And Cumulative OscillationsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients24field (15), fields (4), displacement (3), medium (2)Workbenchlines 6804-8485
Apparatus Section 3: Synchronous Machines: Armature ReactionTheoretical Elements of Electrical Engineering23field (23)Workbenchlines 8741-8906
Chapter 16: IlTheory and Calculation of Alternating Current Phenomena23displacement (17), field (6)Workbenchlines 19346-21338
Chapter 19: Synchronous MotorTheory and Calculation of Alternating Current Phenomena23displacement (17), field (6)Workbenchlines 18053-19457
Lecture 10: Inductance And Capacity Of Round Parallel ConductorsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients22field (15), fields (4), medium (2), displacement (1)Workbenchlines 6089-7274
Apparatus Subsection 63: Direct-current Commutating Machines: C. Commutating Machines 197Theoretical Elements of Electrical Engineering22field (22)Workbenchlines 11795-11863
Chapter 14: Phase Conversion And Single-Phase GenerationTheory and Calculation of Electric Apparatus22field (19), displacement (1), fields (1), medium (1)Workbenchlines 17125-18412
Lecture 8: GenerationGeneral Lectures on Electrical Engineering21field (15), pressure (5), medium (1)Workbenchlines 3781-4217
Apparatus Section 6: Synchronous Converters: Reactive Currents and CompoundingTheoretical Elements of Electrical Engineering21field (20), fields (1)Workbenchlines 15476-15585
Chapter 25: Distortion Of Wave-Shape And Its CausesTheory and Calculation of Alternating Current Phenomena21field (16), displacement (4), strain (1)Workbenchlines 29375-32539
Lecture 8: Arc Lamps And Arc LightingRadiation, Light and Illumination20field (14), pressure (5), stress (1)Workbenchlines 7141-8510
Chapter 33: Efficiency Of SystemsTheory and Calculation of Alternating Current Phenomena20stress (9), strain (8), displacement (1), medium (1), tension (1)Workbenchlines 36515-37127
Chapter 22: Distortion Of Wave-Shape And Its CausesTheory and Calculation of Alternating Current Phenomena19field (16), displacement (3)Workbenchlines 21190-21982
Chapter 4: MagnetismTheory and Calculation of Electric Circuits19medium (10), field (6), fields (3)Workbenchlines 6942-9061
Chapter 7: Power And Energy Of The Complex CircuitTheory and Calculation of Transient Electric Phenomena and Oscillations19field (19)Workbenchlines 33528-34202
Lecture 9: Hunting Of Synchronous MachinesGeneral Lectures on Electrical Engineering18field (17), displacement (1)Workbenchlines 4218-4594
Lecture 1: Nature And Different Forms Of RadiationRadiation, Light and Illumination18field (6), ether (5), medium (5), fields (1), tension (1)Workbenchlines 608-1548
Apparatus Section 5: Synchronous Converters: Armature ReactionTheoretical Elements of Electrical Engineering18field (18)Workbenchlines 15161-15475
Lecture 5: Temperature RadiationRadiation, Light and Illumination17tension (16), pressure (1)Workbenchlines 3946-5076
Chapter 20: Beactiox MachinesTheory and Calculation of Alternating Current Phenomena17field (14), displacement (1), fields (1), tension (1)Workbenchlines 22388-23273
Chapter 21: Reaction MachinesTheory and Calculation of Alternating Current Phenomena16field (14), displacement (1), fields (1)Workbenchlines 20502-21189
Apparatus Section 9: Synchronous Machines: Magnetic Characteristic or Saturation CurveTheoretical Elements of Electrical Engineering15field (15)Workbenchlines 9554-9650
Apparatus Section 7: Synchronous Converters: Variable Ratio Converters (“split Pole” Converters)Theoretical Elements of Electrical Engineering15field (15)Workbenchlines 15586-15734
Chapter 13: Transient Term Of The Rotating FieldTheory and Calculation of Transient Electric Phenomena and Oscillations15field (13), displacement (2)Workbenchlines 13936-14548
Apparatus Section 13: Synchronous Machines: Parallel OperationTheoretical Elements of Electrical Engineering14field (14)Workbenchlines 9821-9878
Chapter 13: Foucault Or Eddy CurrentsTheory and Calculation of Alternating Current Phenomena14field (13), field of force (1), fields (1)Workbenchlines 13484-14333
Chapter 37: Quarter-Phase SystemTheory and Calculation of Alternating Current Phenomena14field (11), displacement (3)Workbenchlines 38393-40115
Chapter 21: Dibtobtiox Of Wavs-Shafe And Its CausesTheory and Calculation of Alternating Current Phenomena14field (11), displacement (3)Workbenchlines 23274-24559
Chapter 18: Surging Of Synchronous MotorsTheory and Calculation of Electric Apparatus14field (14)Workbenchlines 20975-21712
Chapter 7: Distribution Of Alternating-Current Density In ConductorTheory and Calculation of Transient Electric Phenomena and Oscillations14field (12), fields (1), tension (1)Workbenchlines 24981-26094
Lecture 3: Single-Energy Transients In Continuous Current CircuitsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients13field (11), fields (1), medium (1)Workbenchlines 1659-2484
Lecture 3: Single-Energy Transients In Continuous Current CircuitsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients13field (11), fields (1), medium (1)Workbenchlines 1531-2161
Lecture 6: Higher Harmonics Of The Generator WaveGeneral Lectures on Electrical Engineering13field (10), strain (1), stress (1), tension (1)Workbenchlines 3133-3507
Chapter 5: MagnetismTheory and Calculation of Electric Circuits13field (8), fields (4), medium (1)Workbenchlines 9062-11050
Lecture 1: General ReviewGeneral Lectures on Electrical Engineering12tension (11), field (1)Workbenchlines 154-565
Lecture 12: Illumination And Illuminating EngineeringRadiation, Light and Illumination12field (10), strain (2)Workbenchlines 16485-17445
Apparatus Introduction 21: IntroductionTheoretical Elements of Electrical Engineering12field (12)Workbenchlines 8292-8517
Apparatus Subsection 54: Direct-current Commutating Machines: C. Commutating Machines 187Theoretical Elements of Electrical Engineering12field (12)Workbenchlines 11214-11300
Chapter 9: High-Frequency ConductorsTheory and Calculation of Transient Electric Phenomena and Oscillations12field (12)Workbenchlines 27003-27760
Lecture 8: Traveling WavesElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients11tension (9), field (1), medium (1)Workbenchlines 5279-6124
Lecture 8: Traveling WavesElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients11tension (9), field (1), medium (1)Workbenchlines 4745-5520
Theory Section 6: Self-inductance of Continuous-current CircuitsTheoretical Elements of Electrical Engineering11field (11)Workbenchlines 1785-2249
Apparatus Section 4: Induction Machines: Induction GeneratorTheoretical Elements of Electrical Engineering11field (11)Workbenchlines 21158-21588
Apparatus Section 12: Synchronous Machines: Starting of Synchronous MotorsTheoretical Elements of Electrical Engineering11field (11)Workbenchlines 9749-9820
Apparatus Section 8: Direct-current Commutating Machines: Armature ReactionTheoretical Elements of Electrical Engineering11field (11)Workbenchlines 11616-11694
Apparatus Subsection 66: Direct-current Commutating Machines: C. Commutating Machines 201Theoretical Elements of Electrical Engineering11field (11)Workbenchlines 11981-12083
Apparatus Section 11: Synchronous Converters: Double-current GeneratorsTheoretical Elements of Electrical Engineering11field (10), displacement (1)Workbenchlines 15893-15982
Chapter 5: Single-Phase Induction MotorTheory and Calculation of Electric Apparatus11displacement (5), field (4), medium (2)Workbenchlines 8555-10582
Chapter 12: Reactance Of Induction ApparatusTheory and Calculation of Electric Circuits11field (9), fields (2)Workbenchlines 22634-23465
Chapter 12: Magnetic Saturation And Hysteresis In Alternat Ing-Current CircuitsTheory and Calculation of Transient Electric Phenomena and Oscillations11field (11)Workbenchlines 12885-13935
Lecture 1: Nature And Origin Of TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients10field (7), pressure (2), fields (1)Workbenchlines 557-1002
Lecture 1: Nature And Origin Of TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients10field (7), pressure (2), fields (1)Workbenchlines 460-882
Chapter 3: Trigonometric SeriesEngineering Mathematics: A Series of Lectures Delivered at Union College10pressure (5), field (4), fields (1)Workbenchlines 6064-15155
Lecture 10: Regulation And ControlGeneral Lectures on Electrical Engineering10field (10)Workbenchlines 4595-4930
Lecture 3: Physiological Effects Of RadiationRadiation, Light and Illumination10field (4), medium (4), pressure (1), strain (1)Workbenchlines 2366-3638
Theory Section 2: Magnetism and E.m.f.Theoretical Elements of Electrical Engineering10field (10)Workbenchlines 910-1032
Apparatus Subsection 49: Direct-current Commutating Machines: C. Commutating Machines 181Theoretical Elements of Electrical Engineering10field (10)Workbenchlines 10941-11024
Apparatus Subsection 53: Direct-current Commutating Machines: C. Commutating Machines 185Theoretical Elements of Electrical Engineering10field (10)Workbenchlines 11132-11213
Apparatus Section 9: Synchronous Converters: Inverted ConvertersTheoretical Elements of Electrical Engineering10field (9), tension (1)Workbenchlines 15735-15810
Chapter 22: Unipolar MachinesTheory and Calculation of Electric Apparatus10field (9), medium (1)Workbenchlines 31716-32137
Chapter 2: Circuit Control By Periodic Transient PhenomenaTheory and Calculation of Transient Electric Phenomena and Oscillations10field (10)Workbenchlines 15626-15962
Lecture 5: Single-Energy Tra.Nsient Of Ironclad CircuitElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients9field (7), fields (1), medium (1)Workbenchlines 3387-3720
Lecture 5: Single-Energy Transient Of Ironclad CircuitElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients9field (7), fields (1), medium (1)Workbenchlines 2972-3286
Lecture 11: Lightning ProtectionGeneral Lectures on Electrical Engineering9pressure (7), field (2)Workbenchlines 4931-5294
Apparatus Section 8: Synchronous Machines: Characteristic Curves of Synchronous MotorTheoretical Elements of Electrical Engineering9field (8), displacement (1)Workbenchlines 9399-9553
Apparatus Subsection 48: Direct-current Commutating Machines: C. Commutating MachinesTheoretical Elements of Electrical Engineering9field (9)Workbenchlines 10845-10940
Apparatus Section 4: Synchronous Converters: Armature Current and HeatingTheoretical Elements of Electrical Engineering9displacement (7), field (2)Workbenchlines 13889-15160
Chapter 24: ConclusionTheory and Calculation of Electric Apparatus9field (9)Workbenchlines 32820-33531
Lecture 5: Long Distance TransmissionGeneral Lectures on Electrical Engineering8tension (7), field (1)Workbenchlines 2562-3132
Apparatus Section 4: Synchronous Machines: Self-inductanceTheoretical Elements of Electrical Engineering8field (8)Workbenchlines 8907-9034
Apparatus Subsection 51: Direct-current Commutating Machines: C. Commutating Machines 183Theoretical Elements of Electrical Engineering8field (8)Workbenchlines 11047-11125
Apparatus Subsection 61: Direct-current Commutating Machines: C. Commutating MachinesTheoretical Elements of Electrical Engineering8field (8)Workbenchlines 11711-11773
Apparatus Subsection 70: Direct-current Commutating Machines: C. Commutating MachinesTheoretical Elements of Electrical Engineering8field (8)Workbenchlines 12319-12398
Chapter 18: Polyphase Induction MotorsTheory and Calculation of Alternating Current Phenomena8displacement (4), field (4)Workbenchlines 17717-20445
Chapter 28: Copper Efficiency Of SystemsTheory and Calculation of Alternating Current Phenomena8strain (7), displacement (1)Workbenchlines 26584-27052
Chapter 23: Effects Of Higher HarmonicsTheory and Calculation of Alternating Current Phenomena8displacement (4), field (2), strain (2)Workbenchlines 21983-22448
Chapter 30: Efficiency Of SystemsTheory and Calculation of Alternating Current Phenomena8strain (7), displacement (1)Workbenchlines 25136-25597
Chapter 2: Multiple Squirrel-Cage Induction MotorTheory and Calculation of Electric Apparatus8field (5), medium (2), fields (1)Workbenchlines 3543-5554
Report Record 4: Record of Four TroublesInvestigation of Some Trouble in the Generating System of the Commonwealth Edison Co.7displacement (4), field (3)WorkbenchPDF pages 16-27, lines 1139-2164
Chapter 7: Numerical CalculationsEngineering Mathematics: A Series of Lectures Delivered at Union College7field (7)Workbenchlines 21989-25587
Lecture 13: Physiological Problems Of Illuminating EngineeringRadiation, Light and Illumination7field (7)Workbenchlines 17446-17956
Theory Section 3: Generation of E.m.f.Theoretical Elements of Electrical Engineering7field (7)Workbenchlines 1033-1243
Apparatus Section 3: Induction Machines: Single -phase Induction MotorTheoretical Elements of Electrical Engineering7field (4), displacement (3)Workbenchlines 20428-21157
Apparatus Section 2: Synchronous Machines: Electromotive ForcesTheoretical Elements of Electrical Engineering7field (7)Workbenchlines 8658-8740
Apparatus Section 15: Synchronous Machines: Fluctuating Cross Currents in Parallel OperationTheoretical Elements of Electrical Engineering7displacement (3), field (3), fields (1)Workbenchlines 9918-10123
Apparatus Subsection 55: Direct-current Commutating Machines: C. Commutating Machines 189Theoretical Elements of Electrical Engineering7field (7)Workbenchlines 11301-11386
Apparatus Subsection 80: Direct-current Commutating Machines: C. Commutating Machines 221Theoretical Elements of Electrical Engineering7field (7)Workbenchlines 13120-13188
Chapter 20: Single-Phase Induction MotorsTheory and Calculation of Alternating Current Phenomena7field (5), displacement (2)Workbenchlines 21538-22301
Chapter 26: Effects Of Higher HarmonicsTheory and Calculation of Alternating Current Phenomena7displacement (4), field (2), strain (1)Workbenchlines 32540-33010
Chapter 14: The Osni!Raij Aiitebnatina-Cubbent TbakbfobmsbTheory and Calculation of Alternating Current Phenomena7field (7), field of force (1)Workbenchlines 14089-14918
Chapter 15: Induction MotobTheory and Calculation of Alternating Current Phenomena7field (4), displacement (3)Workbenchlines 14919-17024
Chapter 20: RiTheory and Calculation of Alternating Current Phenomena7displacement (3), field (2), strain (2)Workbenchlines 24560-25119
Chapter 15: The General Alternating-Current Transformer Or Frequency ConverterTheory and Calculation of Alternating Current Phenomena7field (7), field of force (1)Workbenchlines 12683-13648
Chapter 1: Speed Control Of Induction MotorsTheory and Calculation of Electric Apparatus7field (6), medium (1)Workbenchlines 1368-3542
Chapter 10: Hysteresis MotorTheory and Calculation of Electric Apparatus7field (7)Workbenchlines 14551-14761
Lecture 6: Double-Energy TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients6field (4), medium (1), tension (1)Workbenchlines 3721-4369
Lecture 6: Double-Energy TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients6field (4), medium (1), tension (1)Workbenchlines 3287-3955
Apparatus Section 1: Direct-current Commutating Machines: GeneralTheoretical Elements of Electrical Engineering6field (5), fields (1)Workbenchlines 10430-10474
Apparatus Section 1: Synchronous Converters: GeneralTheoretical Elements of Electrical Engineering6field (4), displacement (1), tension (1)Workbenchlines 13189-13795
Chapter 3: Law Of Electromagnetic InductionTheory and Calculation of Alternating Current Phenomena6field (6)Workbenchlines 2012-2148
Chapter 23: Synchronizing AlternatorsTheory and Calculation of Alternating Current Phenomena6field (3), displacement (2), medium (1)Workbenchlines 25135-25681
Chapter 3: Iiaw Of Eucctbo-Maonimc InductionTheory and Calculation of Alternating Current Phenomena6field (6)Workbenchlines 1973-2121
Chapter 3: Law Of Electro-Magnetic InductionTheory and Calculation of Alternating Current Phenomena6field (6)Workbenchlines 1606-1742
Chapter 6: MagnetismTheory and Calculation of Electric Circuits6fields (4), field (2)Workbenchlines 11051-12221
Chapter 14: Constant-Potential Constant-Current Trans FormationTheory and Calculation of Electric Circuits6field (5), displacement (1)Workbenchlines 24023-27995
Chapter 18: Oscillating CurrentsTheory and Calculation of Electric Circuits6field (3), stress (2), displacement (1)Workbenchlines 31657-33200
Report Section 3: Discussion of RecommendationsInvestigation of Some Trouble in the Generating System of the Commonwealth Edison Co.5fields (3), field (2)WorkbenchPDF pages 12-16, lines 721-1138
Lecture 7: Line OscillationsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients5field (2), tension (2), medium (1)Workbenchlines 4370-5278
Lecture 7: Line OscillationsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients5field (2), tension (2), medium (1)Workbenchlines 3956-4744
Chapter 5: Methods Of ApproximationEngineering Mathematics: A Series of Lectures Delivered at Union College5field (5)Workbenchlines 15156-16482
Lecture 3: Light And Power DistributionGeneral Lectures on Electrical Engineering5field (3), medium (1), tension (1)Workbenchlines 983-1526
Theory Section 4: Power and Effective ValuesTheoretical Elements of Electrical Engineering5field (5)Workbenchlines 1244-1572
Apparatus Section 6: Synchronous Machines: Characteristic Curves of Alternating-current GeneratorTheoretical Elements of Electrical Engineering5field (5)Workbenchlines 9170-9291
Apparatus Section 3: Direct-current Commutating Machines: Generated E.m.fs.Theoretical Elements of Electrical Engineering5field (5)Workbenchlines 10778-10835
Apparatus Section 10: Direct-current Commutating Machines: CompoundingTheoretical Elements of Electrical Engineering5field (5)Workbenchlines 11774-11794
Apparatus Section 12: Direct-current Commutating Machines: Efficiency and LossesTheoretical Elements of Electrical Engineering5field (5)Workbenchlines 11864-11904
Chapter 15: Distributed Capacity, Inductance, Resistance, And LeakageTheory and Calculation of Alternating Current Phenomena5field (4), field of force (2), medium (1)Workbenchlines 15410-16076
Chapter 17: Synchbonizino AiitebkatobsTheory and Calculation of Alternating Current Phenomena5displacement (2), field (2), medium (1)Workbenchlines 18829-19345
Chapter 13: Distributed Capacity, Inductance, Resistance, And LeakageTheory and Calculation of Alternating Current Phenomena5field (3), field of force (3), medium (2)Workbenchlines 9741-11604
Chapter 18: Synchronizing AlternatorsTheory and Calculation of Alternating Current Phenomena5displacement (2), field (2), medium (1)Workbenchlines 17597-18052
Chapter 19: Alternating- Current Motors In GeneralTheory and Calculation of Electric Apparatus5displacement (3), field (2)Workbenchlines 21713-23905
Chapter 7: Power And Energy Of The Complex Circuit. 513Theory and Calculation of Transient Electric Phenomena and Oscillations5field (5)Workbenchlines 1228-1261
Chapter 3: Mechanical RectificationTheory and Calculation of Transient Electric Phenomena and Oscillations5field (4), fields (1)Workbenchlines 15963-17754
Chapter 2: Long-Distance Transmission LineTheory and Calculation of Transient Electric Phenomena and Oscillations5field (4), field of force (2), medium (1)Workbenchlines 19339-21720
Chapter 6: Germany in the Individualistic EraAmerica and the New Epoch4field (3), fields (1)Workbenchlines 2776-3206
Chapter 13: Evolution: Industrial GovernmentAmerica and the New Epoch4field (3), medium (1)Workbenchlines 5798-6232
Chapter 16: The Future CorporationAmerica and the New Epoch4field (2), fields (1), pressure (1)Workbenchlines 6975-7567
Lecture 2: General DistributionGeneral Lectures on Electrical Engineering4tension (4)Workbenchlines 566-982
Theory Section 8: Power in Alternating-current CircuitsTheoretical Elements of Electrical Engineering4displacement (4)Workbenchlines 2718-2864
Apparatus Section 7: Synchronous Machines: Synchronous MotorTheoretical Elements of Electrical Engineering4field (4)Workbenchlines 9292-9398
Apparatus Section 10: Synchronous Machines: Efficiency and LossesTheoretical Elements of Electrical Engineering4field (4)Workbenchlines 9651-9718
Apparatus Section 9: Direct-current Commutating Machines: Saturation CurvesTheoretical Elements of Electrical Engineering4field (4)Workbenchlines 11695-11710
Apparatus Subsection 76: Direct-current Commutating Machines: Motors Shunt MotorTheoretical Elements of Electrical Engineering4field (4)Workbenchlines 12780-12928
Chapter 30: Balanced And Unbalanced Polyphase SystemsTheory and Calculation of Alternating Current Phenomena4displacement (4)Workbenchlines 35256-35691
Chapter 35: Balanced Symmetrical Polyphase SystemsTheory and Calculation of Alternating Current Phenomena4field (2), displacement (1), medium (1)Workbenchlines 37453-37957
Chapter 12: Dibtbisnted Capacity, Inductance, Besistance, AndTheory and Calculation of Alternating Current Phenomena4field (2), field of force (2), medium (2)Workbenchlines 11564-12672
Chapter 25: Baiianced And Unbaxiancbd Polyphase SystemaTheory and Calculation of Alternating Current Phenomena4displacement (4)Workbenchlines 25605-26027
Chapter 27: Balanced And Unbalanced Polyphase SystemsTheory and Calculation of Alternating Current Phenomena4displacement (4)Workbenchlines 24054-24488
Chapter 9: Synchronous Induction MotorTheory and Calculation of Electric Apparatus4field (3), displacement (1)Workbenchlines 14466-14550
Chapter 15: Synchronous RectifierTheory and Calculation of Electric Apparatus4field (4)Workbenchlines 18413-19373
Chapter 1: Electric Conduction. Soled And LiquidTheory and Calculation of Electric Circuits4field (2), stress (2)Workbenchlines 959-3894
Chapter 8: Velocity Of Propagation Op Electric Field. 387Theory and Calculation of Transient Electric Phenomena and Oscillations4field (4)Workbenchlines 972-1013
Chapter 3: The Natural Period Of The Transmission LineTheory and Calculation of Transient Electric Phenomena and Oscillations4tension (2), displacement (1), field (1), field of force (1)Workbenchlines 21721-23178
Chapter 3: The Individualistic Era: From Competition to Co-operationAmerica and the New Epoch3field (2), pressure (1)Workbenchlines 874-1745
Chapter 8: America in the PastAmerica and the New Epoch3fields (2), field (1)Workbenchlines 3741-4267
Chapter 17: ConclusionAmerica and the New Epoch3field (1), pressure (1), strain (1)Workbenchlines 7568-8027
Theory Section 5: Self-inductance and Mutual InductanceTheoretical Elements of Electrical Engineering3field (3)Workbenchlines 1573-1784
Apparatus Section 2: Induction Machines: Polyphase Induction MotorTheoretical Elements of Electrical Engineering3field (2), displacement (1)Workbenchlines 19166-20427
Theory Section 17: Impedance and AdmittanceTheoretical Elements of Electrical Engineering3field (3)Workbenchlines 6814-7380
Theory Section 20: NomenclatureTheoretical Elements of Electrical Engineering3field (3)Workbenchlines 7991-8291
Apparatus Section 1: Synchronous Machines: GeneralTheoretical Elements of Electrical Engineering3field (3)Workbenchlines 8518-8657
Apparatus Section 16: Synchronous Machines: Higher Frequency Cross Currents Between Synchronous MachinesTheoretical Elements of Electrical Engineering3field (3)Workbenchlines 10124-10189
Apparatus Subsection 40: Direct-current Commutating Machines: C. Commutating MachinesTheoretical Elements of Electrical Engineering3field (3)Workbenchlines 10475-10519
Apparatus Subsection 73: Direct-current Commutating Machines: C. Commutating MachinesTheoretical Elements of Electrical Engineering3field (3)Workbenchlines 12492-12659
Apparatus Subsection 74: Direct-current Commutating Machines: C. Commutating MachinesTheoretical Elements of Electrical Engineering3field (3)Workbenchlines 12660-12763
Chapter 4: Vector RepresentationTheory and Calculation of Alternating Current Phenomena3displacement (3)Workbenchlines 2149-2759
Chapter 6: Induction-Motor Regulation And StabilityTheory and Calculation of Electric Apparatus3field (3)Workbenchlines 10583-12397
Chapter 11: Instability Of Circuits: Induction And Syn Chronous MotorsTheory and Calculation of Electric Circuits3displacement (2), field (1)Workbenchlines 21382-22633
Chapter 16: Load Balance Of Polyphase SystemsTheory and Calculation of Electric Circuits3field (3)Workbenchlines 29302-30428
Chapter 17: Circuits With Distributed LeakageTheory and Calculation of Electric Circuits3medium (3)Workbenchlines 30429-31656
Chapter 6: Oscillating Currents,Theory and Calculation of Transient Electric Phenomena and Oscillations3pressure (2), field (1)Workbenchlines 5312-6797
Chapter 1: IntroductionTheory and Calculation of Transient Electric Phenomena and Oscillations3field (3)Workbenchlines 15354-15625
Chapter 6: Alternating Magnetic Flux DistributionTheory and Calculation of Transient Electric Phenomena and Oscillations3fields (2), field (1)Workbenchlines 23948-24980
Chapter 1: General EquationsTheory and Calculation of Transient Electric Phenomena and Oscillations3field (2), medium (1)Workbenchlines 27761-28694
Chapter 2: The Epoch of the French RevolutionAmerica and the New Epoch2field (1), fields (1)Workbenchlines 627-873
Chapter 7: The Other European Nations in the Individualistic EraAmerica and the New Epoch2field (1), pressure (1)Workbenchlines 3207-3740
Chapter 9: America in the Individualistic EraAmerica and the New Epoch2field (1), fields (1)Workbenchlines 4268-4715
Chapter 12: Evolution: Political GovernmentAmerica and the New Epoch2field (1), fields (1)Workbenchlines 5328-5797
Lecture 9: Oscillations Of The Compound CircuitElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2tension (2)Workbenchlines 6125-6803
Lecture 9: Oscillations Of The Compound CircuitElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2tension (2)Workbenchlines 5521-6088
Lecture 7: High Frequency Oscillations And SurgesGeneral Lectures on Electrical Engineering2field (2)Workbenchlines 3508-3780
Lecture 12: Electric RailwayGeneral Lectures on Electrical Engineering2field (2)Workbenchlines 5295-7123
Lecture 9: Measurement Of Light And RadiationRadiation, Light and Illumination2pressure (2)Workbenchlines 8511-9388
Lecture 10: Light Flux And DistributionRadiation, Light and Illumination2field (2)Workbenchlines 9389-12573
Apparatus Section 6: Induction Machines: Phase ConverterTheoretical Elements of Electrical Engineering2field (2)Workbenchlines 21647-21812
Theory Section 13: Alternating-current TransformerTheoretical Elements of Electrical Engineering2displacement (2)Workbenchlines 4465-5263
Apparatus Section 7: Direct-current Commutating Machines: Effect of Slots on Magnetic FluxTheoretical Elements of Electrical Engineering2field (2)Workbenchlines 11387-11400
Apparatus Subsection 57: Direct-current Commutating Machines: C. Commutating MachinesTheoretical Elements of Electrical Engineering2field (2)Workbenchlines 11401-11540
Apparatus Section 13: Direct-current Commutating Machines: CommutationTheoretical Elements of Electrical Engineering2field (2)Workbenchlines 11905-11980
Apparatus Subsection 72: Direct-current Commutating Machines: GeneratorsTheoretical Elements of Electrical Engineering2field (2)Workbenchlines 12400-12491
Apparatus Subsection 75: Direct-current Commutating Machines: C. Commutating MachinesTheoretical Elements of Electrical Engineering2field (2)Workbenchlines 12764-12779
Apparatus Subsection 77: Direct-current Commutating Machines: C. Commutating MachinesTheoretical Elements of Electrical Engineering2field (2)Workbenchlines 12929-13007
Apparatus Section 1: Alternating-current Transformer: GeneralTheoretical Elements of Electrical Engineering2medium (2)Workbenchlines 16804-16911
Chapter 1: IntroductionTheory and Calculation of Alternating Current Phenomena2field (2)Workbenchlines 1120-1683
Chapter 12: Effective Resistance And ReactanceTheory and Calculation of Alternating Current Phenomena2field (2)Workbenchlines 10718-13483
Chapter 19: Induction GeneratorsTheory and Calculation of Alternating Current Phenomena2field (2)Workbenchlines 20446-21537
Chapter 27: Symbolic Representation Of General Alternating WavesTheory and Calculation of Alternating Current Phenomena2displacement (2)Workbenchlines 33011-34776
Chapter 1: IntroductionTheory and Calculation of Alternating Current Phenomena2field (2)Workbenchlines 1224-1727
Chapter 4: Graphic BefrisxintationTheory and Calculation of Alternating Current Phenomena2displacement (2)Workbenchlines 2122-2743
Chapter 10: FTheory and Calculation of Alternating Current Phenomena2field (2), field of force (1)Workbenchlines 8269-10499
Chapter 30: Quartbr-Fhase SystemTheory and Calculation of Alternating Current Phenomena2displacement (1), field (1)Workbenchlines 27501-29124
Chapter 1: IntroductionTheory and Calculation of Alternating Current Phenomena2field (2)Workbenchlines 963-1366
Chapter 4: Graphic RepresentationTheory and Calculation of Alternating Current Phenomena2displacement (2)Workbenchlines 1743-2321
Chapter 10: Effective Resistance And ReactanceTheory and Calculation of Alternating Current Phenomena2field (2)Workbenchlines 6957-8383
Chapter 31: Three-Phase SystemTheory and Calculation of Alternating Current Phenomena2displacement (2)Workbenchlines 25598-25903
Chapter 32: Quarter-Phase SystemTheory and Calculation of Alternating Current Phenomena2displacement (1), field (1)Workbenchlines 25904-27405
Chapter 8: Synchronizing Induction MotorsTheory and Calculation of Electric Apparatus2field (2)Workbenchlines 13956-14465
Chapter 8: Shaping Of Waves By Magnetic SaturationTheory and Calculation of Electric Circuits2field (1), fields (1)Workbenchlines 12962-16963
Chapter 7: Resistance, Inductance, And Capacity In Series In Alternating-Current CircuitTheory and Calculation of Transient Electric Phenomena and Oscillations2field (2)Workbenchlines 6798-7825
Chapter 9: Divided CircuitTheory and Calculation of Transient Electric Phenomena and Oscillations2field (2)Workbenchlines 9228-10474
Chapter 1: IntroductionTheory and Calculation of Transient Electric Phenomena and Oscillations2field (2)Workbenchlines 19260-19338
Chapter 2: Discussion Of General EquationsTheory and Calculation of Transient Electric Phenomena and Oscillations2field (2)Workbenchlines 28695-29315
Chapter 3: Standing WavesTheory and Calculation of Transient Electric Phenomena and Oscillations2field (1), medium (1)Workbenchlines 29316-30243
Chapter 5: Free OscillationsTheory and Calculation of Transient Electric Phenomena and Oscillations2field (2)Workbenchlines 31451-32708
Chapter 1: Eras in the World’s HistoryAmerica and the New Epoch1field (1)Workbenchlines 234-626
Chapter 15: The American NationAmerica and the New Epoch1strain (1)Workbenchlines 6598-6974
Report Section 2: RecommendationsInvestigation of Some Trouble in the Generating System of the Commonwealth Edison Co.1fields (1)WorkbenchPDF pages 7-12, lines 145-720
Chapter 1: The General NumberEngineering Mathematics: A Series of Lectures Delivered at Union College1field (1)Workbenchlines 915-3491
Chapter 6: Empirical CurvesEngineering Mathematics: A Series of Lectures Delivered at Union College1field (1)Workbenchlines 16483-21988
Theory Section 7: Inductance in Alternating-current CircuitsTheoretical Elements of Electrical Engineering1field (1)Workbenchlines 2250-2717
Apparatus Section 6: Alternating-current Transformer: Heating and VentilationTheoretical Elements of Electrical Engineering1pressure (1)Workbenchlines 18461-18520
Theory Section 12: Impedance of Transmission LinesTheoretical Elements of Electrical Engineering1displacement (1)Workbenchlines 3761-4464
Theory Section 16: Phase Control of Transmission LinesTheoretical Elements of Electrical Engineering1field (1)Workbenchlines 6222-6813
Theory Section 18: Equivalent Sine WavesTheoretical Elements of Electrical Engineering1displacement (1)Workbenchlines 7381-7736
Apparatus Section 5: Synchronous Machines: Synchronous ReactanceTheoretical Elements of Electrical Engineering1field (1)Workbenchlines 9035-9169
Apparatus Subsection 45: Direct-current Commutating Machines: C. Commutating Machines 177Theoretical Elements of Electrical Engineering1field (1)Workbenchlines 10737-10777
Apparatus Section 4: Direct-current Commutating Machines: Distribution of Magnetic FluxTheoretical Elements of Electrical Engineering1field (1)Workbenchlines 10836-10844
Apparatus Section 6: Direct-current Commutating Machines: Effect of Commutating PolesTheoretical Elements of Electrical Engineering1field (1)Workbenchlines 11126-11131
Apparatus Subsection 67: Direct-current Commutating Machines: C. Commutating MachinesTheoretical Elements of Electrical Engineering1field (1)Workbenchlines 12084-12199
Apparatus Section 10: Synchronous Converters: FrequencyTheoretical Elements of Electrical Engineering1field (1)Workbenchlines 15811-15892
Apparatus Section 13: Synchronous Converters: Direct-current ConverterTheoretical Elements of Electrical Engineering1field (1)Workbenchlines 16065-16540
Chapter 2: Instantaneous Values And Integral ValuesTheory and Calculation of Alternating Current Phenomena1field (1)Workbenchlines 1684-2011
Chapter 6: Topographic MethodTheory and Calculation of Alternating Current Phenomena1displacement (1)Workbenchlines 3267-3618
Chapter 7: Polar Coordinates And Polar DiagramsTheory and Calculation of Alternating Current Phenomena1displacement (1)Workbenchlines 3619-4087
Chapter 10: Resistance And Reactance Of TransmissionTheory and Calculation of Alternating Current Phenomena1field (1)Workbenchlines 6993-9766
Chapter 28: General Polyphase SystemsTheory and Calculation of Alternating Current Phenomena1tension (1)Workbenchlines 34777-34928
Chapter 36: Three-Phase SystemTheory and Calculation of Alternating Current Phenomena1displacement (1)Workbenchlines 37958-38392
Chapter 29: Thbkb-Fhase SystemTheory and Calculation of Alternating Current Phenomena1displacement (1)Workbenchlines 27053-27500
Chapter 6: Topographic MethodTheory and Calculation of Alternating Current Phenomena1displacement (1)Workbenchlines 2774-3131
Chapter 24: Symbolic Representation Of General Alternating WavesTheory and Calculation of Alternating Current Phenomena1displacement (1)Workbenchlines 22449-23642
Chapter 25: General Polyphase SystemsTheory and Calculation of Alternating Current Phenomena1tension (1)Workbenchlines 23643-23780
Chapter 6: Alternating Magnetic Flux Distribution. 355Theory and Calculation of Transient Electric Phenomena and Oscillations1fields (1)Workbenchlines 904-937
Chapter 9: Inductive Discharges. 535Theory and Calculation of Transient Electric Phenomena and Oscillations1field (1)Workbenchlines 1286-1316
Chapter 2: IntroductionTheory and Calculation of Transient Electric Phenomena and Oscillations1field (1)Workbenchlines 1993-2658
Chapter 4: Arc RectificationTheory and Calculation of Transient Electric Phenomena and Oscillations1stress (1)Workbenchlines 17755-19259
Chapter 20: Single-Phase Commutator Motors - 306 hit(s)

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... econom- ical, due to their very low speed, resultant from the low frequency. The direction of rotation of a direct-current motor, whether shunt or series motor, remains the same at a reversal of the im- pressed e.m.f., as in this case the current in the armature circuit and the current in the field circuit and so the field magnetism both reverse. Theoretically, a direct-current motor therefore could be operated on an alternating impressed e.m.f. provided that the magnetic circuit of the motor is laminated, so as to fol- low the alternations of magnetism without serious loss of power, and ...
... ir very low speed, resultant from the low frequency. The direction of rotation of a direct-current motor, whether shunt or series motor, remains the same at a reversal of the im- pressed e.m.f., as in this case the current in the armature circuit and the current in the field circuit and so the field magnetism both reverse. Theoretically, a direct-current motor therefore could be operated on an alternating impressed e.m.f. provided that the magnetic circuit of the motor is laminated, so as to fol- low the alternations of magnetism without serious loss of power, and that precautions are tak ...
Lecture 4: Single-Energy Transients In Alternating Current Circuits - 137 hit(s)

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... the instantaneous values of the resultant currents (shown in drawn line) must be zero at any moment, not only during the permanent condition, but also dur- ing the transition period existing before the permanent condi- tion is reached. It is interesting to apply this to the resultant magnetic field produced by three equal three-phase magnetizing coils placed under equal angles, that is, to the starting of the three-phase rotating magnetic field, or in general any polyphase rotating magnetic field. Fig. 18. — Construction of Starting Transient of Rotating Field. As is well known, thr ...
... dur- ing the transition period existing before the permanent condi- tion is reached. It is interesting to apply this to the resultant magnetic field produced by three equal three-phase magnetizing coils placed under equal angles, that is, to the starting of the three-phase rotating magnetic field, or in general any polyphase rotating magnetic field. Fig. 18. — Construction of Starting Transient of Rotating Field. As is well known, three equal magnetizing coils, placed under equal angles and excited by three-phase currents, produce a result- ant magnetic field which is constant in i ...
Lecture 2: Conclusions From The Relativity Theory - 134 hit(s)

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... e become dependent on the conditions of obser- vation. The law of conservation of matter thus had to be abandoned and mass became a manifestation of energy. The law of gravitation has been recast, and the force of gravitation has become an effect of inertial motion, like centrifugal force. The ether has been abandoned, and the field of force of Faraday and Maxwell has become the fundamental conception of physics. The laws of mechanics ^ have been changed, and time and space have been bound' together in the four-dimensional world space, the dimen- sions of which are neither space nor time, ...
... s of obser- vation. The law of conservation of matter thus had to be abandoned and mass became a manifestation of energy. The law of gravitation has been recast, and the force of gravitation has become an effect of inertial motion, like centrifugal force. The ether has been abandoned, and the field of force of Faraday and Maxwell has become the fundamental conception of physics. The laws of mechanics ^ have been changed, and time and space have been bound' together in the four-dimensional world space, the dimen- sions of which are neither space nor time, but a symmetrical combination of both. W ...
Lecture 4: Single-Energy Transients In Alternating Current Circuits - 133 hit(s)

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... the instantaneous values of the resultant currents (shown in drawn line) must be zero at any moment, not only during the permanent condition, but also dur- ing the transition period existing before the permanent condi- tion is reached. It is interesting to apply this to the resultant magnetic field produced by three equal three-phase magnetizing coils placed under equal angles, that is, to the starting of the three-phase rotating magnetic field, or in general any polyphase rotating magnetic field. Fig. 18. — Construction of Starting Transient of Rotating Field. As is well known, thre ...
... dur- ing the transition period existing before the permanent condi- tion is reached. It is interesting to apply this to the resultant magnetic field produced by three equal three-phase magnetizing coils placed under equal angles, that is, to the starting of the three-phase rotating magnetic field, or in general any polyphase rotating magnetic field. Fig. 18. — Construction of Starting Transient of Rotating Field. As is well known, three equal magnetizing coils, placed under equal angles and excited by three-phase currents, produce a result- ant magnetic field which is constant in in ...
Lecture 14: Alternating Current Railway Motor - 129 hit(s)

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FOURTEENTH LECTURE ALTERNATING CURRENT RAILWAY MOTOR. mN a direct current motor, whether a shunt or a series motor, the motor still revolves in the same direction, if the impressed e. m. f. be reversed, as field and arma- ture both reverse. Since a reversal of voltage does not change the operation of the motor, such a direct current motor there- fore can operate also on alternating current. With an alter- nating voltage supply, the field magnetism of the motor also alternates ; the motor field must th ...
... in the same direction, if the impressed e. m. f. be reversed, as field and arma- ture both reverse. Since a reversal of voltage does not change the operation of the motor, such a direct current motor there- fore can operate also on alternating current. With an alter- nating voltage supply, the field magnetism of the motor also alternates ; the motor field must therefore be laminated, to avoid excessive energy losses and heating by eddy currents (cur- rents produced in the field iron by the alternation of the mag- netism) just as in the direct current motor the armature must be laminated. ...
Lecture 3: Gravitation And The Gravitational Fleld - 102 hit(s)

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LECTURE III GRAVITATION AND THE GRAVITATIONAL FLELD A. THE IDENTITY OF GRAVITATIONAL, CENTRIFUGAL AND INERTIAL MASS As seen in the preceding lecture, the conception of the ether as the carrier of radiation had to be abandoned as incompatible with the theory of relativity; the conception of action at a distance is repugnant to our reasoning, and its place is taken by the conception of the field of force, or, more correctly, the energy field. The energy field is a stor ...
... AND INERTIAL MASS As seen in the preceding lecture, the conception of the ether as the carrier of radiation had to be abandoned as incompatible with the theory of relativity; the conception of action at a distance is repugnant to our reasoning, and its place is taken by the conception of the field of force, or, more correctly, the energy field. The energy field is a storage of energy in space, character- ized by the property of exerting a force on any body susceptible to this energy — that is, a magnetic field on a magnetizable body, a gravitational field on a gravitational mass, etc. Light, ...
Chapter 22: Armature Reactions Of Alternators - 91 hit(s)

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CHAPTER XXII ARMATURE REACTIONS OF ALTERNATORS 192. The change of the terminal voltage of an alternating current generator, resulting from a change of load at constant field excitation, is due to the combined effect of armature reaction and armature self-induction. The counter m.m.f. of the armature current, or armature reaction, combines with the impressed m.m.f. or field excitation to the resultant m.m.f., which produces the resultant magnetic field in the field ...
... nal voltage of an alternating current generator, resulting from a change of load at constant field excitation, is due to the combined effect of armature reaction and armature self-induction. The counter m.m.f. of the armature current, or armature reaction, combines with the impressed m.m.f. or field excitation to the resultant m.m.f., which produces the resultant magnetic field in the field poles and generates in the armature an e.m.f. called the "virtual generated e.m.f.," since it has no actual existence, but is merely a mathematical fiction. The counter e.m.f. of self-induction of the ...
Chapter 13: Reactance Of Synchronous Machines - 77 hit(s)

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... YNCHRONOUS MACHINES 119. The synchronous machine — ^alternating-current generator, synchronous motor or synchronous condenser — consists of an armature containing one or more electric circuits traversed by alternating currents and synchronously revolving relative to a unidirectional magnetic field, excited by direct current. The armature circuit, like every electric circuit, has a resistance, r, in which power is being dissipated by the current, /, and an in- ductance, L, or reactance, a; = 2 irfL^ which represents the mag- netic flux produced by the current in the armature circuit, and ...
... ng dissipated by the current, /, and an in- ductance, L, or reactance, a; = 2 irfL^ which represents the mag- netic flux produced by the current in the armature circuit, and interlinked with this circuit. Thus, if ^^ = voltage induced in the armature circuit by its rotation through the magnetic field — or, as now more usually the case, the rotation of the magnetic field through the armature circuit — the terminal voltage of the armature circuit is ^ = ^o-(r+jx)/. In Fig. 110 is shown diagrammatically the path of the field flux, in two different positions, A with an armature slot standin ...
Chapter 14: Short-Circuit Currents Of Alternators - 72 hit(s)

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... CURRENTS OF ALTERNATORS. 112. The short-circuit current of an alternator is limited by armature reaction and armature self-inductance; that is, the current in the armature represents a m.m.f. which with lagging current, as at short circuit, is demagnetizing or opposing the impressed m.m.f. of field excitation, and by combining therewith to a resultant m.m.f. reduces the magnetic flux from that corre- sponding to the field excitation to that corresponding to the resultant of field excitation and armature reaction, and thus reduces the generated e.m.f. from the nominal generated e.m.f., eO ...
... ductance; that is, the current in the armature represents a m.m.f. which with lagging current, as at short circuit, is demagnetizing or opposing the impressed m.m.f. of field excitation, and by combining therewith to a resultant m.m.f. reduces the magnetic flux from that corre- sponding to the field excitation to that corresponding to the resultant of field excitation and armature reaction, and thus reduces the generated e.m.f. from the nominal generated e.m.f., eOJ to the virtual generated e.m.f., er The armature current also produces a local magnetic flux in the armature iron and pole- ...
Chapter 10: Mutual Inductance - 66 hit(s)

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... vely related to each other symmetrically, or reduced thereto; that is, where the mutual inductance is due to coils enclosed in the first circuit, interlinked magnetically with coils enclosed in the second circuit, as the primary and the secondary coils of a transformer, or a shunt and a series field winding of a generator, 144 TRANSIENT PHENOMENA the two coils are assumed as of the same number of turns, or reduced thereto. ri, No. turns second circuit If a = — = — =rr— — - -- : - r— , the currents in the nA No. turns first circuit second circuit are multiplied, the e.m.fs. divided ...
... uation of voltage, actually an appreciable time must elapse. A 600-kw. 8-pole direct-current generator overcompounds from 500 volts at no load to 600 volts at terminals at full load of 1000 amperes. The circuit constants are: resistance of armature winding, r0 = 0.01 ohm; resistance of series field winding, r2' = 0.003 ohm; number of turns per pole in shunt field winding, n1= 1000, and magnetic flux per pole at 500 volts, 4> = 10 megalines. At 600 volts full load terminal voltage (or voltage from brush to brush) the generated e.m.f. is e + irQ = 610 volts. From the saturation curve or ...
Theory Section 19: Fields of Force - 65 hit(s)

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19. FIELDS OF FORCE 89. When an electric current flows through a conductor, power is consumed and heat produced inside of the conductor. In the space outside and surrounding the conductor, a change has taken place also, and this space is not neutral and inert any ...
... s in chains; a magnetic needle is moved and places itself in a definite direction. Due to the passage of the current in the conductor, there are therefore in the spaces outside of the con- ductor — where the current does not flow — forces exerted, and FIELDS OF FORCE 113 this space then is not neutral space, but has become a field of force, and the cause of the field, in this case the electric current in the conductor, is its "motive force." As in this case the actions exerted in the field of force are ...
Lecture 2: The Electric Field - 61 hit(s)

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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 su ...
... 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 EL ...
Lecture 2: The Electric Field - 61 hit(s)

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LECTURE II. THE ELECTRIC FIELD. 7. Let, in Fig. 7, a generator G transmit electric power over line A into a receiving circuit L. While power flows through the conductors A, power is con- sumed in these conductors by conversion into heat, repre- sented by i?r. This, however, Fig. 7. is not all, but in the space surr ...
... r flows through the conductors A, power is con- sumed in these conductors by conversion into heat, repre- sented by i?r. 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 <J>. 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 E ...
Chapter 8: Velocity Of Propagation Of Electric Field - 59 hit(s)

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CHAPTER VIII. VELOCITY OF PROPAGATION OF ELECTRIC FIELD. 67. In the theoretical investigation of electric circuits the velocity of propagation of the electric field through space is usually not considered, but the electric field assumed as instan- taneous throughout space; that is, the electromagnetic com- ponent of the field is considered as in p ...
CHAPTER VIII. VELOCITY OF PROPAGATION OF ELECTRIC FIELD. 67. In the theoretical investigation of electric circuits the velocity of propagation of the electric field through space is usually not considered, but the electric field assumed as instan- taneous throughout space; that is, the electromagnetic com- ponent of the field is considered as in phase with the current, the electrostatic component as in phase with the voltage. In reality, however, the elec ...
Chapter 1: The Constants Of The Electric Circuit - 58 hit(s)

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... uctive receiver circuit, the flow of energy always decreases from generating to receiving circuit, and the power gradient therefore is characteristic of the direc- tion of the flow of energy.) In the space outside of the conductor, during the flow of energy through the circuit, a condition of stress exists which is called the electric field of the conductor. That is, the surrounding space is not uniform, but has different electric and magnetic properties in different directions. No power is required to maintain the electric field, but energy 3 4 TRANSIENT PHENOMENA is required to p ...
... always decreases from generating to receiving circuit, and the power gradient therefore is characteristic of the direc- tion of the flow of energy.) In the space outside of the conductor, during the flow of energy through the circuit, a condition of stress exists which is called the electric field of the conductor. That is, the surrounding space is not uniform, but has different electric and magnetic properties in different directions. No power is required to maintain the electric field, but energy 3 4 TRANSIENT PHENOMENA is required to produce the electric field, and this energy ...
Lecture 4: The Characteristics Of Space A. The Geometry Of The Gravitational Field - 56 hit(s)

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LECTURE IV THE CHARACTERISTICS OF SPACE A. THE GEOMETRY OF THE GRAVITATIONAL FIELD The starting point of the relativity theory is that the laws of nature, including the velocity of light in empty space, are the same everywhere and with regard to any system to which they may be referred — whether on the revolving platform of the earth or in the speeding railway train or in ...
... een the fixed stars. From this it follows that the length of a body is not a fixed property of it, but is relative, depending on the conditions of obser- vation— the relative velocity of the observer with regard to the body. It also is shown that the laws of motion of bodies in a gravitational field are identical with the laws of inertial motion with regard to an accelerating system (as exemplified by the billiard ball in the speeding railway train, Lecture I). From these two conclusions it follows that in the gravitational field the circumference of a circle is not equal to tt times its ...
Chapter 3: Inductance And Resistance In Continuous Current Circuits - 56 hit(s)

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... circuits to reduce the inductance than in alternating-current circuits, where the inductance usually causes a drop of voltage, and direct-current circuits as a rule have higher inductance, especially if the circuit is used for producing magnetic flux, as in solenoids, electro- magnets, machine-fields. Any change of the condition of a continuous-current circuit, as a change of e.m.f., of resistance, etc., which leads to a change of current from one value i0 to another value iv results in the appearance of a transient term connecting the current values i0 and iv and into the equation of the ...
... it. That is, an inductive circuit cannot be opened instantly, but the arc following the break maintains the circuit for some time, and the voltage generated in opening an inductive circuit is the higher the quicker the break. Hence in a highly inductive circuit, as an electromagnet or a machine field, the insulation may be punctured by excessive generated e.m.f. when quickly opening the circuit. As example, some typical circuits may be considered. CONTINUOUS-CURRENT CIRCUITS 27 21. Starting of a continuous-current lighting circuit, or non-in- ductive load. Let e0 = 125 volts = impre ...
Theory Section 1: Magnetism and Electric Current - 55 hit(s)

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1. MAGNETISM AND ELECTRIC CURRENT 1. A magnet pole attracting (or repelling) another magnet pole of equal strength at unit distance with unit force1 is called a unit magnet pole. The space surrounding a magnet pole is called a magnetic field of force, or magnetic field. The magnetic field at unit distance from a unit magnet pole is called a unit magnetic field, and is represented by one line of magnetic force (or shortly "one line") per square centimeter, and from a unit magnet pole thus issue a to ...
... SM AND ELECTRIC CURRENT 1. A magnet pole attracting (or repelling) another magnet pole of equal strength at unit distance with unit force1 is called a unit magnet pole. The space surrounding a magnet pole is called a magnetic field of force, or magnetic field. The magnetic field at unit distance from a unit magnet pole is called a unit magnetic field, and is represented by one line of magnetic force (or shortly "one line") per square centimeter, and from a unit magnet pole thus issue a total of 4 TT lines ...
Chapter 14: Dielectric Losses - 52 hit(s)

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... tive reactance, as "effective resistance," so the energy losses in the dielectric lead to a power component in the condensive reactance, which may be repre- sented by an "effective resistance of dielectric losses" or an "effective conductance of dielectric losses." In the alternating magnetic field, power is consumed by mag- netic hysteresis. This is proportional to the frequency, and to the 1.6*'' power of the magnetic density, and is considerable, amounting in a closed magnetic circuit to 40 to 60 per cent, of the total volt-amperes. In the dielectric field, the energy losses usually ...
... In the alternating magnetic field, power is consumed by mag- netic hysteresis. This is proportional to the frequency, and to the 1.6*'' power of the magnetic density, and is considerable, amounting in a closed magnetic circuit to 40 to 60 per cent, of the total volt-amperes. In the dielectric field, the energy losses usually are very much smaller, rarely amounting to more than a few per cent., though they may at high temperature in cables rise as high as 40 to 60 per cent. The foremost such losses are: leakage, that is, ih loss of the current passing by conduction (as "dynamic current") ...
Chapter 4: Induction Motor With Secondary Excitation - 52 hit(s)

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CHAPTER IV INDUCTION MOTOR WITH SECONDARY EXCITATION 38. While in the typical synchronous machine and eommu- tating machine the magnetic field is excited by a direct current, characteristic of the induction machine is, that the magnetic field is excited by an alternating current derived from the alter- nating supply voltage, just as in the alternating-current trans- former. As the alternating magnetizing current is a wattless reactiv ...
CHAPTER IV INDUCTION MOTOR WITH SECONDARY EXCITATION 38. While in the typical synchronous machine and eommu- tating machine the magnetic field is excited by a direct current, characteristic of the induction machine is, that the magnetic field is excited by an alternating current derived from the alter- nating supply voltage, just as in the alternating-current trans- former. As the alternating magnetizing current is a wattless reactive current, the result is, that the alternating-current input into the induction motor is always laggi ...
Chapter 21: Alternating-Current Generator - 48 hit(s)

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CHAPTER XXI ALTERNATING-CURRENT GENERATOR 185. In the alternating-current generator, e.m.f. is generated in the armature conductors by their relative motion through a constant or approximately constant magnetic field. When yielding current, two distinctly different m.m.fs. are acting upon the alternator armature — the m.m.f. of the field due to the field-exciting spools, and the m.m.f. of the armature current. The former is constant, or approximately so, while the latter is alternating, and in synchronous ...
... 185. In the alternating-current generator, e.m.f. is generated in the armature conductors by their relative motion through a constant or approximately constant magnetic field. When yielding current, two distinctly different m.m.fs. are acting upon the alternator armature — the m.m.f. of the field due to the field-exciting spools, and the m.m.f. of the armature current. The former is constant, or approximately so, while the latter is alternating, and in synchronous motion relatively to the former; hence fixed in space relative to the field m.m.f., or uni- FiG. 129. directional; but ...
Chapter 17: Inductor Machines - 47 hit(s)

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CHAPTER XVII INDUCTOR MACHINES Inductor Alternators, Etc. 156. Synchronous machines may be built with stationary field and revolving armature, as shown diagrammatically in Fig. 134, or with revolving field and stationary armature, Fig. 135, or with stationary field and stationary armature, but revolving magnetic circuit. The revolving-armature type was the most frequent in the early days, but has practically ...
CHAPTER XVII INDUCTOR MACHINES Inductor Alternators, Etc. 156. Synchronous machines may be built with stationary field and revolving armature, as shown diagrammatically in Fig. 134, or with revolving field and stationary armature, Fig. 135, or with stationary field and stationary armature, but revolving magnetic circuit. The revolving-armature type was the most frequent in the early days, but has practically gone out of use except for special Fia. 134. — Revolving armature alternator Fig. ...
Chapter 21: Regulating Pole Converters - 47 hit(s)

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... constant impressed alternating voltage, is in- 424 EL ECTRIC A L A PPA RA T f '8 dependent of the wave shape, and thus run be produced whether the alternating voltage is a sine wave or any other wave. It is obvious that, instead of shifting the brushes on the com- mutator, the magnetic field poles may \k< shifted, in the opposite direction, by the same angle, as shown in Fig. 198, A, B, C. Instead of mechanically shifting the field poles, they can bt shifted electrically, by having each field pole consist of a numUr of sections, and successively reversing the polarity of these sec ...
... ether the alternating voltage is a sine wave or any other wave. It is obvious that, instead of shifting the brushes on the com- mutator, the magnetic field poles may \k< shifted, in the opposite direction, by the same angle, as shown in Fig. 198, A, B, C. Instead of mechanically shifting the field poles, they can bt shifted electrically, by having each field pole consist of a numUr of sections, and successively reversing the polarity of these sec- tions, as shown in Fig. 199, A, B, C, D. by mechanically shifting llie poles. Instead of having a large number of field pole sections, ob ...
Chapter 17: Alternating-Current Generator - 45 hit(s)

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CHAPTER XVII. ALTERNATING-CURRENT GENERATOR. 182. In the alternating-current generator, E.M.F. is induced in the armature conductors by their relative motion through a constant or approximately constant magnetic field. When yielding current, two distinctly different M.M.Fs. are acting upon the alternator armature — the M.M.F. of the field due to the field-exciting 'spools, and the M.M.F. of the armature current. The former is constant, or approx- imately so, while the latter is alternating, and in synchro- ...
... 182. In the alternating-current generator, E.M.F. is induced in the armature conductors by their relative motion through a constant or approximately constant magnetic field. When yielding current, two distinctly different M.M.Fs. are acting upon the alternator armature — the M.M.F. of the field due to the field-exciting 'spools, and the M.M.F. of the armature current. The former is constant, or approx- imately so, while the latter is alternating, and in synchro- nous motion relatively to the former ; hence, fixed in space relative to the field M.M.F., or uni-directional, but pulsating ...
Lecture 17: Arc Lighting - 43 hit(s)

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... either direct current or alternating current. For direct current constant current supply, separate arc light machines have been built, and are still largely used. In these machines, inherent regulation for constant current is produced by using a very high armature reaction and relatively weak field excitation; that is, the armature ampere turns are nearly equal and opposite to the field ampere turns, and thus both very large compared with the difference, the resultant ampere turns, which produce the magnetic field. A moderate increase of current and consequent increase of armature ampere ...
... separate arc light machines have been built, and are still largely used. In these machines, inherent regulation for constant current is produced by using a very high armature reaction and relatively weak field excitation; that is, the armature ampere turns are nearly equal and opposite to the field ampere turns, and thus both very large compared with the difference, the resultant ampere turns, which produce the magnetic field. A moderate increase of current and consequent increase of armature ampere turns therefore greatly reduces the resultant ampere turns and ARC LIGHTING 221 so th ...
Chapter 24: Synchronous Motor - 42 hit(s)

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... ion that loading the motor reduces, unloading increases, the current within the range between 1 and 12. The condition of maximum output is 3, current in phase with impressed e.m.f. Since at constant current the loss is constant, this is at the same time the condition of maximum efficiency; no displacement of phase of the impressed e.m.f., or self-induction of the circuit compensated by the effect of the lead of the motor current. This condition of maximum efficiency of a circuit we have found already in Chapter XL 216. B. £"0 and Ei constant, I variable. Obviously Eq lies again on the circle ...
... ^ = impedance of the circuit of (equivalent) resistance, r, and (equivalent) reactance, x = 2 irfL, containing the impressed e.m.f., eo and the counter e.m.f., d, of the syn- chronous motor ^; that is, the e.m.f. generated in the motor arma- ture by its rotation through the (resultant) magnetic field. Let i = current in the circuit (effective values). The mechanical power delivered by the synchronous motor (including friction and core loss) is the electric power consumed by the counter e.m.f., ei; hence ■p = iei cos {i, 6]); (1) thus, cos (t, ei) = -^> lei sin a, eO = ^1 - (|-j ...
Chapter 19: Commutatob Motobs - 41 hit(s)

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... sence of commu- tators. The main subdivisions of commutator motors are the repulsion motor, the series motor, and the shunt motor. REPULSION MOTOR. 193. The repulsion motor is an induction motor or transformer motor ; that is, a motor in which the main current enters the primary member or field only, while in the secondary member, or armature, a current is in- duced, and thus the action is due to the repulsive thrust between induced current and inducing magnetism. As stated under the heading of induction motors, a multiple circuit armature is required for the purpose of having alwa ...
... pulsive thrust between induced current and inducing magnetism. As stated under the heading of induction motors, a multiple circuit armature is required for the purpose of having always secondary circuits in inductive relation to the primary circuit during the rotation. If with a single- coil field, these secondary circuits are constantly closed upon themselves as in the induction motor, the primary circuit will not exert a rotary effect upon the armature while at rest, since in half of the armature coils the cur- rent is induced so as to give a rotary effort in the one direction, and in ...
Chapter 20: Commutator Motors - 41 hit(s)

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... ence of commu- tators. The main subdivisions of commutator motcrs are the repulsion motor, the series motor, and the shunt motor. REPULSION MOTOR. 214. The repulsion motor -is an induction motor or transformer motor ; that is, a motor in which the main current enters the primary member or field only, while in the secondary member, or armature, a current is in- duced, arid thus the action is due to the repulsive thrust between induced current and inducing magnetism. As stated under the heading of induction motors, a multiple circuit armature is required for the purpose of having alw ...
... pulsive thrust between induced current and inducing magnetism. As stated under the heading of induction motors, a multiple circuit armature is required for the purpose of having always secondary circuits in inductive relation to the primary circuit during the rotation. If with a single- coil field, these secondary circuits are constantly closed upon themselves as in the induction motor, the primary circuit will not exert a rotary effect upon the armature while at rest, since in half of the armature coils the cur- rent is induced so as to give a rotary effort in the one direction, and in ...
Chapter 16: Aiitebnatingh-Current Osnebator - 37 hit(s)

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CHAPTER XVI. AIiTEBNATINGh-CURRENT OSNEBATOR. 159. In the alternating-current generator, E.M.F. is induced in the armature conductors by their relative motion through a constant or approximately constant magnetic field. When yielding current, two distinctly different M.M.Fs. are acting upon the alternator armature — the M.M.F. of the field due to the field-exciting spools, and the M.M.F. of the armature current. The former is constant, or approx- imately so, while the latter is alternating, and in synchro- ...
... 159. In the alternating-current generator, E.M.F. is induced in the armature conductors by their relative motion through a constant or approximately constant magnetic field. When yielding current, two distinctly different M.M.Fs. are acting upon the alternator armature — the M.M.F. of the field due to the field-exciting spools, and the M.M.F. of the armature current. The former is constant, or approx- imately so, while the latter is alternating, and in synchro- nous motion relatively to the former ; hence, fixed in space relative to the field M.M.F., or uni-directional, but pulsating ...
Chapter 11: Phase Control - 36 hit(s)

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... t requires a receiving circuit in which, independent of the load, a lagging or leading component of current can be produced at will. Such is the case in synchronous motors or converters: in a synchronous motor a lagging current can be produced by decreasing, a leading current by increasing, the field excitation. 81. If in a direct-current motor, at constant impressed voltage, the field excitation and therefore the field magnetism is decreased, the motor speed increases, as the armature has to revolve faster to consume the impressed e.m.f., and if the field excitation is increased, the mot ...
... mponent of current can be produced at will. Such is the case in synchronous motors or converters: in a synchronous motor a lagging current can be produced by decreasing, a leading current by increasing, the field excitation. 81. If in a direct-current motor, at constant impressed voltage, the field excitation and therefore the field magnetism is decreased, the motor speed increases, as the armature has to revolve faster to consume the impressed e.m.f., and if the field excitation is increased, the motor slows down. A synchronous motor, however, cannot vary in speed, since it must keep in ...