Complex Exponentials
The most important signal is complex-valued, the complex
exponential.
st=Aⅇⅈ2π
f
0
t+φ=Aⅇⅈφⅇⅈ2π
f
0
t
s
t
A
2
f
0
t
φ
A
φ
2
f
0
t
(2)
Here,
ⅈ denotes
-1
-1
(Mathematicians use the symbol
ii
for
-1
-1
).
For electrical engineers, history led to a different symbol.
Ampère
used the symbol
ii to denote
current (intensité de current).
Euler first used
ii for
imaginary numbers but that notation did not take hold until
roughly Ampère's time. It wasn't until the twentieth
century that the importance of complex numbers to circuit
theory became evident. By then, using
ii for current was entrenched and
electrical engineers chose
ⅈ
for writing complex numbers.
Aⅇⅈφ
A
φ
is known as the signal's
complex amplitude.
Considering the complex amplitude as a complex number
in polar form, its magnitude is the amplitude
AA and its angle the signal
phase. The complex amplitude is also known as a
phasor. The complex exponential cannot be further
decomposed into more elemental signals, and is the
most important signal in electrical
engineering! Mathematical manipulations at first
appear to be more difficult because complex-valued numbers are
introduced. In fact, early in the twentieth century,
mathematicians thought engineers would not be sufficiently
sophisticated to handle complex exponentials even though they
greatly simplified solving circuit problems.
Steinmetz
introduced complex exponentials to electrical engineering, and
demonstrated that "mere" engineers could use them to good
effect and even obtain right answers! See
Complex Numbers for a
review of complex numbers and complex arithmetic.
The complex exponential defines the notion of frequency: it is
the
only signal that contains only one
frequency component. The sinusoid consists of two frequency
components: one at the frequency
+f0
f0
and the other at
-f0
f0
.
Euler relation:
This decomposition of the sinusoid can be traced to Euler's
relation.
cos2πft=ⅇⅈ2πft+ⅇ-ⅈ2πft2
2
f
t
2
f
t
2
f
t
2
(3)
sin2πft=ⅇⅈ2πft-ⅇ-ⅈ2πft2ⅈ
2
f
t
2
f
t
2
f
t
2
(4)
ⅇⅈ2πft=cos2πft+ⅈsin2πft
2
f
t
2
f
t
2
f
t
(5)
Decomposition:
The complex exponential signal can thus be written in terms of
its real and imaginary parts using Euler's relation. Thus,
sinusoidal signals can be expressed as either the real or the
imaginary part of a complex exponential signal, the choice
depending on whether cosine or sine phase is needed, or as the
sum of two complex exponentials. These two decompositions are
mathematically equivalent to each other.
Acos2πft+φ=ℜAⅇⅈφⅇⅈ2πft
A
2
f
t
φ
A
φ
2
f
t
(6)
Asin2πft+φ=ℑAⅇⅈφⅇⅈ2πft
A
2
f
t
φ
A
φ
2
f
t
(7)
Using the complex plane, we can envision the complex
exponential's temporal variations as seen in the above figure
(
Figure 1). The magnitude of
the complex exponential is
AA,
and the initial value of the complex exponential at
t=0
t
0
has an angle of
φφ.
As time increases, the locus of points traced by the complex
exponential is a circle (it has constant magnitude of
AA). The number of times per
second we go around the circle equals the frequency
ff. The time taken for the
complex exponential to go around the circle once is known as
its
period TT, and
equals
1f
1
f
. The projections onto the real and imaginary axes
of the rotating vector representing the complex exponential
signal are the cosine and sine signal of Euler's relation
(
Equation 3).
Real Exponentials
As opposed to complex exponentials which oscillate,
real exponentials decay.
st=ⅇ-tτ
s
t
t
τ
(8)
The quantity
ττ is known as
the exponential's
time constant, and corresponds
to the time required for the exponential to decrease by a
factor of
1ⅇ
1
, which approximately equals
0.3680.368.
A decaying complex exponential is the product of a real and
a complex exponential.
st=Aⅇⅈφⅇ-tτⅇⅈ2πft=Aⅇⅈφⅇ-1τ+ⅈ2πft
s
t
A
φ
t
τ
2
f
t
A
φ
1
τ
2
f
t
(9)
In the complex plane, this signal corresponds to an
exponential spiral. For such signals, we can define
complex frequency as the quantity multiplying
tt.
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