In our analysis of dc networks we
found it is necessary to find the algebraic sum of voltages and currents. Since
the same will also be true for ac networks, the question arises: How do we
determine the algebraic sum of two or more voltages (or currents) that are
varying sinusoidally? Although one solution would be to find the algebraic sum
on a point-to-point basis, this would be a long and tedious process in which
accuracy would be directly related to the scale employed.
It is the purpose of this chapter
to introduce a system of complex numbers which, when related to the
sinusoidal ac waveform, will result in a technique for finding the algebraic
sum of sinusoidal waveforms that is quick, direct, and accurate. In the
following chapters the technique will be extended to permit the analysis of
sinusoidal ac networks in a manner very similar to that applied to dc networks.
The methods and theorems as described for dc networks can then be applied to
sinusoidal ac networks with little difficulty.
For reasons that will be obvious
later, the real axis is sometimes called the resistance axis, and the
imaginary axis, the reactance axis.
Every number from 0 to ± ∞ can be represented by some point along
the real axis. Prior to the development of this system of complex numbers, it
was believed that any number not on the real axis would not exist-hence the
term imaginary for the vertical axis.
In the complex plane, the
horizontal or real axis represents all positive numbers to the right of the
imaginary axis and all negative numbers to the left of the imaginary axis. All
positive imaginary numbers are represented above the real axis, and all
negative imaginary numbers, below the real axis. The symbol) (or sometimes i)
is used to denote an imaginary number.
No comments:
Post a Comment