a steady state is now equipped with a rectifier and inverter for the purpose of
achieving adjustable-speed control. The induction motor together with its drive is
no longer a linear load. Unfortunately, the previous power definitions under nonsi-
nusoidal currents were dubious, thus leading to misinterpretations in some cases.
Chapter 2 presents a review of some theories dealing with nonsinusoidal conditions.
As pointed out above, the problems related to nonlinear loads have significantly
increased with the proliferation of power electronics equipment. The modern equip-
ment behaves as a nonlinear load drawing a significant amount of harmonic current
from the power network. Hence, power systems in some cases have to be analyzed
under nonsinusoidal conditions. This makes it imperative to establish a consistent
set of power definitions that are also valid during transients and under nonsinu-
soidal conditions.
The power theories presented by Budeanu [3,4] and Fryze [5] had basic concerns
related to the calculation of average power or root-mean-square values (rms values)
of voltage and current. The development of power electronics technology has
brought new boundary conditions to the power theories. Exactly speaking, the new
conditions have not emerged from the research of power electronics engineers.
They have resulted from the proliferation of power converters using power semi-
conductor devices such as diodes, thyristors, insulated-gate bipolar transistors (IG-
BTs), gate-turn-off (GTO) thyristors, and so on. Although these power converters
have a quick response in controlling their voltages or currents, they may draw reac-
tive power as well as harmonic current from power networks. This has made it clear
that conventional power theories based on average or rms values of voltages and
currents are not applicable to the analysis and design of power converters and pow-
er networks. This problem has become more serious and clear during comprehen-
sive analysis and design of active filters intended for reactive-power compensation
as well as harmonic compensation.
From the end of the 1960s to the beginning of the 1970s, Erlicki and Emanuel-
Eigeles [6], Sasaki and Machida [7], and Fukao, Iida, and Miyairi [8] published their
pioneer papers presenting what can be considered as a basic principle of controlled
reactive-power compensation. For instance, Erlicki and Emanuel-Eigeles [6] pre-
sented some basic ideas like “compensation of distortive power is unknown to date.
. . .” They also determined that “a non-linear resistor behaves like a reactive-power
generator while having no energy-storing elements,” and presented the very first ap-
proach to active power-factor control. Fukao, Iida and Miyairi [8] stated that “by con-
necting a reactive-power source in parallel with the load, and by controlling it in such
a way as to supply reactive power to the load, the power network will only supply ac-
tive power to the load. Therefore, ideal power transmission would be possible.”
Gyugyi and Pelly [9] presented the idea that reactive power could be compensat-
ed by a naturally commutated cycloconverter without energy storage elements. This
idea was explained from a physical point of view. However, no specific mathemati-
cal proof was presented. In 1976, Harashima, Inaba, and Tsuboi [10] presented,
probably for the first time, the term “instantaneous reactive power” for a single-
phase circuit. That same year, Gyugyi and Strycula [11] used the term “active ac
power filters” for the first time. A few years later, in 1981, Takahashi, Fujiwara,
1.1. CONCEPTS AND EVOLUTION OF ELECTRIC POWER THEORY 3
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