Title: Frequency Domain Analysis
1Frequency Domain Analysis
Review of Complex Numbers
z is complex, a and b are real, j is THE
imaginary number
a is the real part of z b is the imaginary
part z is the sum of its real and imaginary parts
2Complex Numbers
A complex number may be represented by plotting
it in rectangular coordinates
b
a
Or, in polar coordinates
3Complex Numbers
From this, It's obvious that
b
a
4Complex Numbers
Titans Formula
Eulers Formula
Oilers Formula
So, multiplying by the magnitude of z
So another way of writing the complex number z is
5Complex Arithmetic
For addition of complex numbers, use the
rectangular form
For multiplication, you can still use the
rectangular form
But polar form is often more convenient
6Complex Arithmetic
Every complex number
has its complex conjugate
In polar form
7Complex Arithmetic
Again, for division, the polar form is often more
convenient
But, the rectangular form can be used
8Complex Functions
Suppose z is a complex-valued function of a real
valued variable f
Its real and imaginary parts are real-valued
functions of f, as are its magnitude and phase
9Frequency Response
The response of a BIBO stable, LSI system to a
sinusoidal input is of particular interest,
because any periodic signal may be described as a
sum of sinusoids (Fourier series) and any
aperiodic signal can be described as an integral
of a continuum of sinusoids. The response of
such a system to a single sinusoid is a sinusoid
of the same frequency. The amplitude and phase
of the steady-state response are functions of the
frequency, and comprise the systems Frequency
Response.
10Frequency Response
Consider a sinusoidal signal
This can be represented as a phasor
We can find the response of a system H(s) to V
11Frequency Response
Remember our old friend, the RC lowpass filter?
12Frequency Response
Substituting j2pf for s
H(f) is a complex-valued function of the
real-valued variable, f. It has a real part and
an imaginary part, as well as a magnitude and
phase angle. The magnitude is the systems
Amplitude Response, and the phase angle is its
Phase Response.
13Frequency Response
For a frequency f, we can find the output phasor
Or, in the time domain,
14Frequency Response
For our RC circuit,
So
15Frequency Response
If our filter is normalized, that is, has a
corner frequency such that
16Frequency Response
Wed probably like to see plots of the frequency
response
17Frequency Response
18Negative Frequency
What???
This is nice. The real part is fine, but what
does an imaginary sinusoid look like on an
oscilloscope? What does it sound like? It would
be nice if we could just get rid of it.
19Negative Frequency
Adding these
Which can be rewritten
20Negative Frequency
So the real sinusoid can be thought of as a sum
of two complex exponentials, one of positive
frequency and one of negative frequency. Any
real-world signal, whether it is a
single-frequency sinusoid or not, may also be
treated as having a positive frequency component
and a negative frequency component. This is
often referred to as a Mathematical Fiction.
21Negative Frequency
We use this fiction because it is convenient.
Suppose we have a system H(f) driven by a complex
exponential
Then we can solve for the output signal by simply
multiplying the complex exponential input by H(f)
22Negative Frequency
23Negative Frequency
Recall that a real sinusoid can be written as a
sum of two complex exponentials, one of positive
frequency and one of negative frequency
Or
Where
24Negative Frequency
So y(t) is an increasing function of t,
increasing at a constant rate f (or w).
Therefore, cos(t) can be represented by two
counterrotating vector, rotating at rates of w
and w.
25Negative Frequency
26Frequency Response and Impulse Response
If a system whose impulse response is h(t) is
driven by a signal x(t), where
Then the output signal can be found by
convolution
27Frequency Response and Impulse Response
So,
The bracketed term is obviously the systems
frequency response, but on closer inspection it
is also the Fourier transform of the impulse
response.
28Frequency Response
For example, take our old friend the RC lowpass
filter. We previously found its impulse response
to be
Lets plug this into the Fourier Transform
integral
29Frequency Response
30Frequency Response
This is the same result we got earlier, by
circuit analysis. The system frequency response
is the same as the Fourier transform of the
system impulse response.
31Periodic Signals
Any periodic signal can be represented as a
Fourier series, or sum of sinusoids (or complex
exponentials).
Since were concerned only with linear systems,
the response to a sum of signals is the sum of
the responses to each individual signal
32Periodic Signals
Note that this is the steady-state response, the
output that would be observed if the driving
signal had been present for a long time (strictly
speaking, since the Big Bang). In real life, the
response would also contain a component called
the Natural Response which would account for the
finite duration of the input.