The Principles of Electric Power Transmission by Alternating Currents

Front Cover
Wiley, 1928 - Electric lines - 399 pages
 

Contents

Graphical Solution for Mixed Sending and Receivingend Conditions
44
Effect of Transformers
47
CHAPTER IV
51
Nominalπ Method
54
Numerical Example
56
NominalT Solution
57
Ferranti Effect
61
Aluminium
62
Charging Current and Losses in Opencircuited Line
63
Effect of Capacitance on Performance of Loaded Line
64
Limitations of Localisedcapacitance Methods of Solution
66
CHAPTER V
68
Line Constants
71
Introduction of Convergent Series
73
Auxiliary Constants of Circuit
74
Illustration of Convergence of Series
75
Numerical Example
77
Semigraphical Solution for Various Receivingend Conditions
81
Hyperbolic Method of Solution
85
Real and Complex Hyperbolic Angles
86
Line Angle
87
Comparison of Methods
89
Electrical Conditions at Intermediate Points
91
Voltage and Current Distribution along Line
94
Effect of Nonsinusoidal Sendingend Voltage
99
CHAPTER VI
103
Conductivity
104
The Circle Diagram 173
105
Current Distortion Effects
106
Choice of Sendingend Voltage 175 176
107
Introductory
108
Insulation of Cables
109
Conductor Materials
110
Methods of Laying
111
Currentcarrying Capacity
112
Maximum Permissible Temperature for Cables
113
Thermal Resistance
114
Thermal Resistance of the Soil
115
Grouped Cables Laid Direct in the Ground
116
Cables Laid on the Solid System
117
Currentcarrying Capacity of Cables in
118
Cables Drawn into Ducts
119
Arcing Horns and Rings
130
Recent Developments in the Design of Suspensiontype Insulators
138
Testing of Insulators
144
Corona Power Loss
150
CHAPTER VIII
156
Effect on Power Factor
163
178
178
219
200
Comparative Currentcarrying Capacities of Cables Laid under Various Conditions 122 Currentcarrying Capacity of Cables for Emergency Loading
201
Capacitance and Insulation Resistance of Singlecore Cables
202
Inductance and Resistance of Singlecore Cables
204
Electrostatic Stresses in Singlecore Cables
211
Economic Conductor Radius of Singlecore Cable
212
Grading of Cables for Alternating Pressures
213
Practical Difficulties Involved in Grading
218
Effect of Temperature Gradient on Distribution of Electrostatic Stresses in Singlecore Cables 130 Representation of Threecore Cable Capacitances by ...
219
Capacitance of Threecore Cable
221
Electrostatic Stresses in Threecore Cables
222
Special Designs of Threecore Cable
227
Influence of Line Voltage on Cost of Transmission System
253
Other Factors Influencing Electrical Design of System
259
Application of Economic Principles to Underground Lines
262
Choice of Frequency
269
CHAPTER XI
271
Protective Relays
272
Constructional Details of Relay
273
Overload Relays
276
Overload Relays with Series Tripping
277
Time Delays
278
Application of Overload Relays to a Radial Transmission System
279
Protection of Parallel Lines by Overload and Reversepower Relays
281
Protection of Ring System
284
Protection of Parallel Lines by Interlocked Relays
285
Corebalance Leakage Protection
289
Combined Corebalance and Overload Protection
291
Corebalance Protection of Parallel Lines
292
FerrantiHawkins Protection
294
McColl Protection
295
MerzHunter Splitconductor Protection
297
CallenderHunter Fourconductor Protection
299
Ideal Characteristics of Protective Gear
301
Beaver Testsheath Protection
302
Calculation of Shortcircuit Currents
306
Effects of Shortcircuit Currents
311
Currentlimiting Reactors
313
Location of Reactors in System
315
Experimental Methods of Determining Shortcircuit Currents
316
CHAPTER XII
319
Oscillation Frequency of a Line
321
Travelling Waves
325
Reflection of Travelling Waves
326
Origin of Pressure Rises
329
Direct Lightning Stroke
331
Side Stroke of Lightning
332
Electrostaticallyinduced Charges
333
Electrostatic Charging of Line Due to Changes in Altitude or Friction Effects
334
Sudden Opening of Loaded Line
336
Arcing Grounds
343
Pressure Rises in Transformers
344
Attenuation of Travelling Waves
348
CHAPTER XIII
350
Horngap Arrestors
352
Multiplegap Arrestor
358
Lightning Arrestor Spark Gaps
362
Electrolytic Arrestor
367
Oxide Film Arrestor
371
Autovalve Arrestor
372
Arrangement of Lightning Arrestors
374
Condensers
375
Surge Absorbers
378
Arcing Ground Suppressors
379
Petersen Coil
380
Waterjet Earthing Resistances
382
Earthing Choking Coils
383
Modern Tendencies
384
The Potentials of a Threephase Transmission System
385
Earthed versus Isolated Neutrals
388
INDEX
393
253
394

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Page 247 - THE most economical size of the copper conductor for the electric transmission of energy, whether for the electric light or for the performance of mechanical work, would be found by comparing the annual interest of the money value of the copper with the money value of the energy lost in it annually in the heat generated in it by the electric current.
Page 247 - He remarked that (contrary to a very prevalent impression and belief) the gauge to be chosen for the conductor does not depend on the length of it through which the energy is to be transmitted. It depends solely on the strength of the current to be used, supposing the cost of the metal and of a unit of energy to be determined.
Page 214 - ... kV. In a cable of homogeneous insulation, the voltage which may be safely applied is limited by the maximum electric stress at the conductor, but if the dielectric is strong enough at that point it is excessive electrically (and therefore needlessly expensive) further away. If, however, the stress can be so distributed that its value in the outer layers of the dielectric is increased without increasing the stress at the conductor, the insulation thickness, for a given voltage, will be reduced....
Page 212 - A small conductor will allow a greater thickness of insulation, but on the other hand, the smaller radius of curvature tends to increase the stress; the effect of too large a radius of conductor is to cause an increase of stress through reduction of the total thickness of insulation. The maximum stress at the conductor surface is (by formula 1...
Page 309 - This table was prepared after a conference between the leading switchgear manufacturers in America, and was given in a paper, " Rating and Selection of Oil Circuit-breakers ", by EM Hewlett, JN Mahoney, and GA Burnham, read before the American IEE in 1918. The numbers given are factors by which the normal full-load current must be multiplied to get the short-circuit current at any given instant. The percentage reactance figures represent the total reactance in the circuit, including that of the generator,...
Page 39 - This maximum value is equal to O'O or BD. For still greater angles of lag the regulation diminishes again. With leading currents the regulation diminishes as the angle of lead increases, and becomes zero when <£., = / AOF.
Page 124 - To avoid a direct contact between the porcelain and the metal pin, a soft metal (generally lead) thimble is used. An adequate length of leakage path is obtained by providing the insulator with two or three petticoats or rain sheds. These are so designed that even when the outer surface of the insulator is wet due to rain, sufficient leakage resistance is still given by the inner dry surfaces.
Page 7 - ... the power dissipated in the form of heat, in overcoming the ohmic resistance, is proportional to the square of the current. A definite amount of power can therefore be transmitted with less loss when the voltage is high than when it is low; but, on each particular transmission, there is a limit to the pressure beyond which there is nothing to be gained in the matter of economy. This limit is determined by the cost of generating and transforming apparatus (which will be greater for the higher...
Page 20 - JO and the inductance per centimetre length due to the flux inside the conductor is cgs units, . (7) which is the internal inductance of the conductor. The total inductance of each wire per centimetre is therefore...
Page 146 - The corona extends until the increase in the effective diameter of the conductor is sufficient to bring the potential gradient at the edge of the corona down to the disruptive gradient of air, and the corona can then spread no farther at the particular voltage under consideration.

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