# Certainly_ all electrical engineers know of linear systems theory

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```					1/22/2007                  EECS 723 intro                        2/3

Certainly, all electrical engineers know of linear systems
theory. But, it is helpful to first review these concepts to
make sure that we all understand what this theory is, why it
works, and how it is useful.

First, we must carefully define a linear-time invariant system.

HO: THE LINEAR, TIME-INVARIANT SYSTEM

Linear systems theory is useful for microwave engineers
because most microwave devices and systems are linear (at
least approximately).

HO: LINEAR CIRCUIT ELEMENTS

The most powerful tool for analyzing linear systems is its
eigen function.

HO: THE EIGEN FUNCTION OF LINEAR SYSTEMS

Complex votages and currents at times cause much head
scratching; let’s make sure we know what these complex
values and functions physically mean.

HO: A COMPLEX REPRESENTATION OF SINUSOIDAL FUNCTIONS

Signals may not have the explicit form of an eigen function,
but our linear systems theory allows us to (relatively) easily
analyze this case as well.

Jim Stiles                The Univ. of Kansas             Dept. of EECS
1/22/2007                  EECS 723 intro                        3/3

HO: ANALYSIS OF CIRCUITS DRIVEN BY ARBITRARY FUNCTIONS

If our linear system is a linear circuit, we can apply basic
circuit analysis to determine all its eigen values!

HO: THE EIGEN SPECTRUM OF LINEAR CIRCUITS

Jim Stiles                The Univ. of Kansas              Dept. of EECS
1/21/2007                  The Linear Time Invariant System.doc                     1/13

The Linear, Time-
Invariant System
Most of the microwave devices and networks that we will
study in this course are both linear and time invariant (or
approximately so).

Let’s make sure that we understand what these terms
mean, as linear, time-invariant systems allow us to
apply a large and helpful mathematical toolbox!

LINEARITY
LINEARITY

Mathematicians often speak of operators,
which is “mathspeak” for any mathematical
operation that can be applied to a single
element (e.g., value, variable, vector, matrix, or
function).

...operators, operators, operators!!

For example, a function f ( x ) describes an operation on
variable x (i.e., f ( x ) is operator on x ). E.G.:

f (y ) = y 2 − 3           g (t ) = 2t               y (x ) = x

Jim Stiles                         The Univ. of Kansas                         Dept. of EECS
1/21/2007                      The Linear Time Invariant System.doc                     2/13

Moreover, we find that functions can likewise be operated on!
For example, integration and differentiation are likewise
mathematical operations—operators that operate on
functions. E.G.,:

d g (t )              ∞

∫ f ( y ) dy                dt                  ∫
−∞
y ( x ) dx

A special and very important class of operators are
linear operators.

Linear operators are denoted as L [ y ] , where:

* L symbolically denotes the mathematical operation;

* And y denotes the element (e.g., function, variable,
vector) being operated on.

A linear operator is any operator that satisfies the following
two statements for any and all y :

1. L [ y1 + y2 ] = L [ y1 ] + L [ y2 ]

2. L ⎡a y ⎤ = a L [ y ] , where a is any constant.
⎣ ⎦

Jim Stiles                             The Univ. of Kansas                         Dept. of EECS
1/21/2007              The Linear Time Invariant System.doc          3/13

From these two statements we can likewise conclude that a
linear operator has the property:

L ⎡a y1 + b y2 ⎤ = a L [ y1 ] + b L [ y2 ]
⎣            ⎦

where both a and b are constants.

Essentially, a linear operator has the property that
any weighted sum of solutions is also a solution!

For example, consider the function:

L [t ] = g (t ) = 2t

At t = 1 :
g (t = 1 ) = 2 (1 ) = 2

and at t = 2 :
g (t = 2 ) = 2 (2 ) = 4

Now at t = 1 + 2 = 3 we find:

g (1 + 2 ) = 2 ( 3 )
=6
=2+4
= g (1 ) + g ( 2 )

Jim Stiles                      The Univ. of Kansas             Dept. of EECS
1/21/2007          The Linear Time Invariant System.doc        4/13

More generally, we find that:

g (t1 + t2 ) = 2 (t1 + t2 )
= 2t1 + 2t2
= g (t1 ) + g (t2 )
and
g (a t ) = 2 a t
= a 2t
= a g (t )

Thus, we conclude that the function g (t ) = 2t is indeed a
linear function!

Now consider this function:

y (x ) = m x + b

Q: But that’s the equation of a line! That
must be a linear function, right?

A: I’m not sure—let’s find out!

We find that:
y ( a x ) = m ( ax ) + b
= a mx + b

but:
a y ( x ) = a (m x + b )
= a mx + a b

Jim Stiles                 The Univ. of Kansas            Dept. of EECS
1/21/2007              The Linear Time Invariant System.doc                5/13

therefore:
y ( a x ) ≠ a y ( x ) !!!

Likewise:
y ( x1 + x 2 ) = m ( x1 + x 2 ) + b
= m x1 + m x 2 + b
but:
y ( x1 ) + y ( x 2 ) = ( m x 1 + b ) + ( m x 2 + b )
= m x1 + m x2 + 2b

therefore:
y ( x1 + x2 ) ≠ y ( x1 ) + y ( x2 ) !!!

The equation of a line is not a linear function!

Moreover, you can show that the functions:

f (y ) = y 2 − 3                     y (x ) = x

are likewise non-linear.

Remember, linear operators need not be
functions. Consider the derivative
operator, which operates on functions.
d
d f (x )
dx                                              dx
f (x )

Jim Stiles                      The Univ. of Kansas                   Dept. of EECS
1/21/2007           The Linear Time Invariant System.doc            6/13

Note that:

d                        d f (x ) d g (x )
⎡f ( x ) + g ( x )⎤ =         +
dx ⎣                 ⎦     dx       dx

and also:

d                  d f (x )
⎡a f ( x )⎤ = a
dx ⎣         ⎦       dx

We thus can conclude that the derivative operation is a linear
operator on function f ( x ) :

d f (x )
= L ⎡f ( x )⎤
⎣       ⎦
dx

You can likewise show that the integration operation is
likewise a linear operator:

∫ f ( y ) dy     = L ⎡f ( y ) ⎤
⎣        ⎦

But, you will find that operations such as:

d g 2 (t )                  ∞

∫    y ( x ) dx
dt                        −∞

are not linear operators (i.e., they are non-linear operators).

Jim Stiles                    The Univ. of Kansas              Dept. of EECS
1/21/2007          The Linear Time Invariant System.doc          7/13

We find that most mathematical operations are in fact non-
linear! Linear operators are thus form a small subset of all
possible mathematical operations.

Q: Yikes! If linear operators are so rare, we are we wasting

A: Two reasons!

Reason 1: In electrical engineering, the behavior of most of
our fundamental circuit elements are described by linear
operators—linear operations are prevalent in circuit analysis!

Reason 2: To our great relief, the two characteristics of
linear operators allow us to perform these mathematical
operations with relative ease!

Q: How is performing a linear operation easier than
performing a non-linear one??

A: The “secret” lies is the result:

L ⎡a y1 + b y2 ⎤ = a L [ y1 ] + b L [ y2 ]
⎣            ⎦

Note here that the linear operation performed on a relatively
complex element a y1 + b y2 can be determined immediately
from the result of operating on the “simple” elements y1 and
y2 .

Jim Stiles                 The Univ. of Kansas              Dept. of EECS
1/21/2007                  The Linear Time Invariant System.doc                     8/13

To see how this might work, let’s consider some arbitrary
function of time v (t ) , a function that exists over some finite
amount of time T (i.e., v (t ) = 0 for t < 0 and t >T ).

Say we wish to perform some linear operation on this
function:
L ⎡v (t )⎤ = ??
⎣      ⎦

Depending on the difficulty of the
operation L , and/or the complexity of the
function v (t ) , directly performing this
operation could be very painful (i.e.,
approaching impossible).

Instead, we find that we can often expand a very complex and
stressful function in the following way:

∞
v (t ) = a0 ψ 0 (t ) + a1 ψ 1 (t ) + a2 ψ 2 (t ) +        =
n
∑ an ψ n (t )
=−∞

where the values an are constants (i.e.,
coefficients), and the functions ψ n (t ) are known
as basis functions.

For example, we could choose the basis functions:

ψ n (t ) = t n    for         n ≥0

Resulting in a polynomial of variable t:

Jim Stiles                          The Univ. of Kansas                        Dept. of EECS
1/21/2007                  The Linear Time Invariant System.doc                9/13

∞
v (t ) = a0 + a1 t + a2 t + a3 t +
2         3
= ∑ an t n
n =0

This signal expansion is of course know as the Taylor Series
expansion. However, there are many other useful expansions
(i.e., many other useful basis ψ n (t ) ).

* The key thing is that the basis functions ψ n (t ) are
independent of the function v (t ) . That is to say, the
basis functions are selected by the engineer (i.e., you)
doing the analysis.

* The set of selected basis functions form what’s known as
a basis. With this basis we can analyze the function
v (t ) .

* The result of this analysis provides the coefficients an
of the signal expansion. Thus, the coefficients are
directly dependent on the form of function v (t ) (as well
as the basis used for the analysis). As a result, the set
of coefficients {a1 , a2 , a3 , } completely describe the
function v (t ) !

Q: I don’t see why this “expansion” of function of v (t ) is
helpful, it just looks like a lot more work to me.

A: Consider what happens when we wish to perform a linear
operation on this function:

Jim Stiles                         The Univ. of Kansas                    Dept. of EECS
1/21/2007               The Linear Time Invariant System.doc            10/13

⎡ ∞             ⎤   ∞
L ⎡v (t )⎤ = L ⎢ ∑ an ψ n (t ) ⎥ = ∑ an L ⎡ψ n (t )⎤
⎣      ⎦                                ⎣        ⎦
⎣n =−∞          ⎦ n =−∞

Look what happened! Instead of performing the linear
operation on the arbitrary and difficult function v (t ) , we can
apply the operation to each of the individual basis functions
ψ n (t ) .

Q: And that’s supposed to be easier??

A: It depends on the linear operation and on the basis
functions ψ n (t ) . Hopefully, the operation L [ψ n (t )] is simple
and straightforward. Ideally, the solution to L [ψ n (t )] is

Q: Oh yeah, like I’m going to get so lucky.
I’m sure in all my circuit analysis problems
evaluating L [ψ n (t )] will be long, frustrating,
and painful.

A: Remember, you get to choose the basis over which the
function v (t ) is analyzed. A smart engineer will choose a
basis for which the operations L [ψ n (t )] are simple and
straightforward!

Q: But I’m still confused. How do I choose what basis ψ n (t )
to use, and how do I analyze the function v (t ) to determine
the coefficients an ??

Jim Stiles                      The Univ. of Kansas                 Dept. of EECS
1/21/2007                       The Linear Time Invariant System.doc                             11/13

A: Perhaps an example would help.

Among the most popular basis is this one:

⎧ j ⎛ 2T n ⎞ t
⎜
π
⎟
⎪e ⎝ ⎠                      0 ≤ t ≤T
⎪
ψn = ⎨
⎪0                      t ≤ 0,t ≥T
⎪
⎩
and:
T                                T              ⎛ 2π n ⎞
1                                1               −j ⎜      ⎟t
an =       ∫v (t ) ψ n (t ) dt
∗
=       ∫v (t ) e      ⎝ T ⎠
dt
T   0
T   0

So therefore:

∞           ⎛ 2π n ⎞
j⎜      ⎟t
v (t ) =
n
∑ an e
=−∞
⎝ T ⎠
for 0 ≤ t ≤T

The astute among you will recognize this signal
expansion as the Fourier Series!

Q: Yes, just why is Fourier analysis so
prevalent?

A: The answer reveals itself when we apply a linear operator
to the signal expansion:

⎛ 2π n ⎞
⎡ ∞      −j ⎜      ⎟t ⎤
∞      ⎡ − j ⎜ 2T n ⎟ t ⎤
⎛ π ⎞

L ⎡v (t )⎤ = L ⎢ ∑ an e
⎣      ⎦
⎝ T ⎠
⎥ = ∑ an L ⎢e    ⎝      ⎠
⎥
⎢n =−∞
⎣                     ⎥ n =−∞
⎦          ⎢
⎣                ⎥
⎦

Jim Stiles                              The Univ. of Kansas                                  Dept. of EECS
1/21/2007          The Linear Time Invariant System.doc       12/13

Note then that we must simply evaluate:

⎡ − j ⎛ 2T n ⎞ t ⎤
⎜
π
⎟
L ⎢e    ⎝      ⎠
⎥
⎢
⎣                ⎥
⎦
for all n.

We will find that performing almost any
linear operation L on basis functions of
this type to be exceeding simple (more on
this later)!

TIME INVARIANCE
TIME INVARIANCE

Q: That’s right! You said that most of the microwave devices
that we will study are (approximately) linear, time-invariant
devices. What does time invariance mean?

A: From the standpoint of a linear operator, it means that
that the operation is independent of time—the result does
not depend on when the operation is applied. I.E., if:

L ⎣x (t )⎤ = y (t )
⎡      ⎦
then:

L ⎡x (t − τ )⎤ = y (t − τ )
⎣          ⎦

where τ is a delay of any value.

Jim Stiles                 The Univ. of Kansas            Dept. of EECS
1/21/2007    The Linear Time Invariant System.doc       13/13

The devices and networks that you are
about to study in EECS 723 are in fact
fixed and unchanging with respect to time
(or at least approximately so).

As a result, the mathematical operations
that describe most (but not all!) of our
circuit devices are both linear and time-
invariant operators. We therefore refer
to these devices and networks as linear,
time-invariant systems.

Jim Stiles           The Univ. of Kansas            Dept. of EECS
1/21/2007                      Linear Circuit Elements.doc                             1/6

Linear Circuit Elements
Most microwave devices can be described or modeled in terms
of the three standard circuit elements:

1. RESISTANCE (R)

2. INDUCTANCE (L)

3. CAPACITANCE (C)

For the purposes of circuit analysis, each of these three
elements are defined in terms of the mathematical
relationship between the difference in electric potential v (t )
between the two terminals of the device (i.e., the voltage
across the device), and the current i (t ) flowing through the
device.

We find that for these three circuit elements, the
relationship between v (t ) and i (t ) can be expressed as a
linear operator!
iR (t )

+
vR (t )
LR ⎡vR (t )⎤ = iR (t ) =
Y⎣        ⎦                 R
vR (t )             R

LR ⎡iR (t )⎤ = vR (t ) = R iR (t )
Z⎣        ⎦
−

Jim Stiles                         The Univ. of Kansas                           Dept. of EECS
1/21/2007                             Linear Circuit Elements.doc                               2/6

iC (t )

d vC (t )              +
LC ⎡vC (t )⎤ = iC (t ) = C
Y⎣        ⎦                         dt
vC (t )                  C
t
1
LZ ⎡iC (t )⎤ = vC (t ) =            ∫ iC (t ′) dt ′
C
⎣       ⎦                   C                          −
−∞

iL (t )
t
+                                                     1
LY ⎡v L (t )⎤ = iL (t ) =     ∫ vL(t ′) dt ′
L
⎣        ⎦               L   −∞

v L (t )             L
d iL (t )
LZ ⎡iL (t )⎤ = v L (t ) = L
L
⎣       ⎦                      dt
−

Since the circuit behavior of these devices can be expressed
with linear operators, these devices are referred to as linear
circuit elements.

Q: Well, that’s simple enough, but what about an element
formed from a composite of these fundamental elements?

For example, for example, how are v (t ) and i (t ) related in
the circuit below??

Jim Stiles                                 The Univ. of Kansas                            Dept. of EECS
1/21/2007                      Linear Circuit Elements.doc                           3/6

i (t )
C
+

LZ ⎡i (t )⎤ = v (t ) = ???
⎣      ⎦                                                               L      R
v (t )

−

A: It turns out that any circuit constructed entirely with
linear circuit elements is likewise a linear system (i.e., a linear
circuit).

As a result, we know that that there must be some linear
operator that relates v (t ) and i (t ) in your example!

LZ ⎡i (t )⎤ = v (t )
⎣      ⎦

The circuit above provides a good example of a single-port
(a.k.a. one-port) network.

We can of course construct networks with two or more ports;
an example of a two-port network is shown below:

i1(t )                                     i2(t )
C
+                                                       +

v1(t )                           L                R    v2(t )

−                                                       −

Jim Stiles                        The Univ. of Kansas                          Dept. of EECS
1/21/2007                 Linear Circuit Elements.doc                    4/6

Since this circuit is linear, the relationship between all
voltages and currents can likewise be expressed as linear
operators, e.g.:
L21 ⎡v1 (t )⎤ = v2 (t )
⎣       ⎦

LZ 21 ⎡i1 (t )⎤ = v2 (t )
⎣       ⎦

LZ 22 ⎡i2 (t )⎤ = v2 (t )
⎣       ⎦

Q: Yikes! What would these linear operators for this circuit
be? How can we determine them?

A: It turns out that linear operators for all linear circuits
can all be expressed in precisely the same form! For example,
the linear operators of a single-port network are:

t
v (t ) = LZ ⎡i (t )⎤ =
⎣      ⎦     ∫ g (t − t ′) i (t ′) dt ′
−∞
Z

t
i (t ) = LY ⎡v (t )⎤ =
⎣      ⎦     ∫ g (t − t ′) v (t ′) dt ′
−∞
Y

In other words, the linear operator of linear circuits can
always be expressed as a convolution integral—a
convolution with a circuit impulse function g (t ) .

Q: But just what is this “circuit impulse response”??

Jim Stiles                   The Univ. of Kansas                   Dept. of EECS
1/21/2007                      Linear Circuit Elements.doc           5/6

A: An impulse response is simply the response of one circuit
function (i.e., i (t ) or v (t ) ) due to a specific stimulus by
another.

That specific stimulus is the impulse function δ (t ) .

The impulse function can be defined as:

πt ⎞
sin ⎛
⎜    ⎟
1       ⎝ τ ⎠
δ (t ) = lim
τ →0   τ     ⎛πt ⎞
⎜    ⎟
⎝ τ ⎠

Such that is has the following two properties:

1.    δ (t ) = 0     for t ≠ 0

∞
2.    ∫ δ (t ) dt
−∞
= 1.0

The impulse responses of the one-port example are
therefore defined as:

gZ (t ) v (t ) i (t ) =δ (t )
and:

gY (t ) i (t ) v (t ) =δ (t )

Jim Stiles                         The Univ. of Kansas         Dept. of EECS
1/21/2007                 Linear Circuit Elements.doc                     6/6

Meaning simply that gZ (t ) is equal to the
voltage function v (t ) when the circuit is
“thumped” with a impulse current (i.e.,
i (t ) = δ (t ) ), and gY (t ) is equal to the
current i (t ) when the circuit is “thumped”
with a impulse voltage (i.e., v (t ) = δ (t ) ).

Similarly, the relationship between the input and the output
of a two-port network can be expressed as:

t
v2(t ) = L21 ⎡v1(t )⎤ =
⎣      ⎦     ∫ g (t − t ′) v (t ′) dt ′
−∞
1

where:

g (t ) v2(t ) v (t ) =δ (t )
1

Note that the circuit impulse response must be causal
(nothing can occur at the output until something occurs at the
input), so that:

g (t ) = 0      for       t <0

Q: Yikes! I recall evaluating convolution integrals to be
messy, difficult and stressful. Surely there is an easier way
to describe linear circuits!?!

A: Nope! The convolution integral is all there is. However,
we can use our linear systems theory toolbox to greatly
simplify the evaluation of a convolution integral!

Jim Stiles                   The Univ. of Kansas                    Dept. of EECS
1/22/2007            The Eigen Function of Linear Systems                   1/7

The Eigen Function of
Linear,Time-Invariant
Systems
Recall that that we can express (expand) a time-limited signal
with a weighted summation of basis functions:

v (t ) = ∑ an ψ n (t )
n

where v (t ) = 0 for t < 0 and t >T .

Say now that we convolve this signal with some system impulse
function g (t ) :
t
L ⎡v (t )⎤ =
⎣      ⎦     ∫ g (t − t ′) v (t ′) dt ′
−∞
t
=    ∫ g (t − t ′) ∑ an ψ n (t ′) dt ′
−∞            n
t
= ∑ an         ∫ g (t − t ′) ψ n (t ′) dt ′
n        −∞

Look what happened!

Instead of convolving the general function v (t ) , we now find
that we must simply convolve with the set of basis functions
ψ n (t ) .

Jim Stiles                       The Univ. of Kansas                  Dept. of EECS
1/22/2007             The Eigen Function of Linear Systems                     2/7

Q: Huh? You say we must “simply” convolve the set of basis
functions ψ n (t ) . Why would this be any simpler?

A: Remember, you get to choose the basis ψ n (t ) . If you’re
smart, you’ll choose a set that makes the convolution integral
“simple” to perform!

Q: But don’t I first need to know the explicit form of g (t )
before I intelligently choose ψ n (t ) ??

A: Not necessarily!

The key here is that the convolution integral:

t
L ⎡ψ n (t )⎤ =
⎣        ⎦     ∫ g (t − t ′) ψ n (t ′) dt ′
−∞

is a linear, time-invariant operator. Because of this, there
exists one basis with an astonishing property!

These special basis functions are:

⎧e j ωn t for 0 ≤ t ≤T
⎪                                                           ⎛ 2π ⎞
ψ n (t ) = ⎨                                      where         ωn = n ⎜ ⎟
⎪0 for t < 0,t >T                                           ⎝T ⎠
⎩

Now, inserting this function (get ready, here comes the
astonishing part!) into the convolution integral:

Jim Stiles                    The Univ. of Kansas                        Dept. of EECS
1/22/2007                     The Eigen Function of Linear Systems                                              3/7

t
L ⎡e                    ∫ g (t − t ′) e                          dt ′
j ωn t                                      j ωn t ′
⎣                ⎤=
⎦
−∞

and using the substitution u = t − t ′ , we get:

t                                             t −t

∫    g (t − t ′ ) e   j ωn t
dt ′ =           ∫        g (u ) e j ωn (t −u ) ( −du )
−∞                                          t − ( −∞ )
0
=e     j ωn t
∫    g (u ) e − j ωn u ( −du )
+∞
∞
=e     j ωn t
∫ g (u ) e
− j ωn u
du
0

See! Doesn’t that astonish!

Q: I’m astonished only by how lame you are.
How is this result any more “astonishing” than
any of the other supposedly “useful” things
you’ve been telling us?

A: Note that the integration in this result is not a
convolution—the integral is simply a value that depends on n
(but not time t):
∞
G (ωn )                ∫ g (t ) e − j ωn t dt
0

As a result, convolution with this “special” set of basis
functions can always be expressed as:

Jim Stiles                                  The Univ. of Kansas                                           Dept. of EECS
1/22/2007                    The Eigen Function of Linear Systems                        4/7

t

∫    g (t − t ′ ) e j ωn t ′ dt ′ = L ⎡e j ωn t ⎤ = G (ωn ) e j ωnt
⎣         ⎦
−∞

operation on function ψ n (t ) = exp [ j ωnt ] results in precisely the
same function of time t (save the complex multiplier G ( ωn ) )!
I.E.:
L ⎡ψ n (t )⎤ = G ( ωn ) ψ n (t )
⎣        ⎦

Convolution with ψ n (t ) = exp [ j ωnt ] is accomplished by
simply multiplying the function by the complex
number G ( ωn ) !

Note this is true regardless of the impulse response g (t )
(the function g (t ) affects the value of G ( ωn ) only)!

Q: Big deal! Aren’t there lots of other functions that would
satisfy the equation above equation?

A: Nope. The only function where this is true is:

ψ n (t ) = e j ωn t

This function is thus very special. We call this function the
eigen function of linear, time-invariant systems.

Q: Are you sure that there are no other eigen functions??

Jim Stiles                            The Univ. of Kansas                          Dept. of EECS
1/22/2007              The Eigen Function of Linear Systems         5/7

A: Well, sort of.

Recall from Euler’s equation that:

e j ωn t = cos ωn t + j sin ωn t

It can be shown that the sinusoidal functions cos ωn t and
sin ωn t are likewise eigen functions of linear, time-invariant
systems.

The real and imaginary components of eigen function
exp [ j ωnt ] are also eigen functions.

Q: What about the set of values G ( ωn ) ?? Do they have any
significance or importance??

A: Absolutely!

Recall the values G ( ωn ) (one for each n) depend on the impulse
response of the system (e.g., circuit) only:

∞
G (ωn )      ∫ g (t ) e − j ωn t dt
0

Thus, the set of values G ( ωn ) completely characterizes a
linear time-invariant circuit over time 0 ≤ t ≤T .

We call the values G ( ωn ) the eigen values of the
linear, time-invariant circuit.

Jim Stiles                     The Univ. of Kansas            Dept. of EECS
1/22/2007              The Eigen Function of Linear Systems           6/7

Q: OK Poindexter, all eigen stuff this
might be interesting if you’re a
mathematician, but is it at all useful
to us electrical engineers?

A: It is unfathomably useful to us
electrical engineers!

Say a linear, time-invariant circuit is excited (only) by a
sinusoidal source (e.g., v s (t ) = cos ωot ). Since the source
function is the eigen function of the circuit, we will find that
at every point in the circuit, both the current and voltage will
have the same functional form.

That is, every current and voltage in the circuit will
likewise be a perfect sinusoid with frequency ωo !!

Of course, the magnitude of the sinusoidal
oscillation will be different at different
points within the circuit, as will the relative
phase. But we know that every current and
voltage in the circuit can be precisely
expressed as a function of this form:

A cos (ωot + ϕ )

Q: Isn’t this pretty obvious?

Jim Stiles                     The Univ. of Kansas            Dept. of EECS
1/22/2007              The Eigen Function of Linear Systems         7/7

A: Why should it be? Say our source function was instead a
square wave, or triangle wave, or a sawtooth wave. We would
find that (generally speaking) nowhere in the circuit would we
find another current or voltage that was a perfect square
wave (etc.)!
In fact, we would find that not
only are the current and voltage
functions within the circuit
different than the source
function (e.g. a sawtooth) they
are (generally speaking) all
different from each other.

We find then that a linear circuit will (generally
speaking) distort any source function—unless that
function is the eigen function (i.e., an sinusoidal
function).

Thus, using an eigen function as circuit source greatly
simplifies our linear circuit analysis problem. All we need to
accomplish this is to determine the magnitude A and relative
phase ϕ of the resulting (and otherwise identical) sinusoidal
function!

Jim Stiles                     The Univ. of Kansas            Dept. of EECS
1/21/2007          A Complex Representation of Sinusoidal Functions.doc            1/8

A Complex Representation
of Sinusoidal Functions
Q: So, you say (for example) if a linear two-port circuit is
driven by a sinusoidal source with arbitrary frequency ωo ,
then the output will be identically sinusoidal, only with a
different magnitude and relative phase.

C
+                                                     +

v1(t ) =Vm 1 cos (ωot + ϕ1 )              L     R         v2(t ) =Vm 2 cos (ωot + ϕ2 )

−                                                     −

How do we determine the unknown magnitude Vm 2 and phase ϕ2
of this output?

A: Say the input and output are related by the impulse
response g (t ) :
t
v2(t ) = L ⎡v1(t )⎤ =
⎣      ⎦      ∫ g (t − t ′) v (t ′) dt ′
−∞
1

We now know that if the input were instead:

v1 (t ) = e j ω t
0

Jim Stiles                         The Univ. of Kansas                       Dept. of EECS
1/21/2007      A Complex Representation of Sinusoidal Functions.doc         2/8

then:
v2(t ) = L ⎡e j ω t ⎤ = G (ω 0 ) e j ω t
⎣        ⎦
0                       0

where:
∞
G (ω 0 )     ∫ g (t ) e
− j ω0 t
dt
0

Thus, we simply multiply the input v1 (t ) = e j ω t by the complex
0

eigen value G (ω 0 ) to determine the complex output v 2 (t ) :

v2(t ) = G (ω 0 ) e j ω t  0

Q: You professors drive me crazy with all this
math involving complex (i.e., real and imaginary)
voltage functions. In the lab I can only generate
and measure real-valued voltages and real-valued
voltage functions. Voltage is a real-valued,
physical parameter!

A: You are quite correct.

Voltage is a real-valued parameter, expressing electric
potential (in Joules) per unit charge (in Coulombs).

Q: So, all your complex formulations and complex eigen
values and complex eigen functions may all be sound
mathematical abstractions, but aren’t they worthless to us
electrical engineers who work in the “real” world (pun
intended)?

Jim Stiles                     The Univ. of Kansas                    Dept. of EECS
1/21/2007          A Complex Representation of Sinusoidal Functions.doc              3/8

A: Absolutely not! Complex analysis actually simplifies our
analysis of real-valued voltages and currents in linear circuits
(but only for linear circuits!).

The key relationship comes from Euler’s Identity:

e j ωt = cos ωt + j sin ωt

Meaning:
Re {e j ωt } = cos ωt

Now, consider a complex value C. We of course can write this
complex number in terms of it real and imaginary parts:

C =a + j b        ∴ a = Re {C }             and     b = Im {C }

But, we can also write it in terms of its magnitude C and
phase ϕ !

C = C e jϕ

where:

C = C C ∗ = a 2 + b2

ϕ = tan −1 ⎡b a ⎤
⎣ ⎦

Thus, the complex function C e j ω t is:      0

Jim Stiles                         The Univ. of Kansas                         Dept. of EECS
1/21/2007         A Complex Representation of Sinusoidal Functions.doc         4/8

C e jω t = C e jϕ e jω t
0                    0

= C e j ω t +ϕ
0

= C cos (ω 0t + ϕ ) + j C sin (ω 0t + ϕ )

Therefore we find:

C cos (ω 0t + ϕ ) = Re {C e j ω t }   0

Now, consider again the real-valued voltage function:

v1(t ) =Vm 1 cos (ωt + ϕ1 )

This function is of course sinusoidal with a magnitude Vm 1 and
phase ϕ1 . Using what we have learned above, we can likewise
express this real function as:

v1(t ) =Vm 1 cos (ωt + ϕ1 )
= Re { 1 e j ωt }
V

where V1 is the complex number:

V1 = Vm 1 e j ϕ 1

Q: I see! A real-valued sinusoid has a magnitude and phase,
just like complex number. A single complex number (V ) can
be used to specify both of the fundamental (real-valued)
parameters of our sinusoid (Vm , ϕ ).

Jim Stiles                           The Univ. of Kansas                 Dept. of EECS
1/21/2007      A Complex Representation of Sinusoidal Functions.doc                     5/8

What I don’t see is how this helps us in our circuit analysis.
After all:
v2(t ) = G (ωo ) (V1 e j ωot )

which means:
v2(t ) ≠ G (ωo ) Re { 1 e j ωot }
V

What then is the real-valued output v2(t ) of our two-port
network when the input v1(t ) is the real-valued sinusoid:

v1(t ) =Vm 1 cos (ωot + ϕ1 )
???
= Re { 1 e
V       j ωot
}
A: Let’s go back to our original convolution integral:

t
v2(t ) =    ∫ g (t − t ′) v (t ′) dt ′
−∞
1

If:
v1(t ) =Vm 1 cos (ωot + ϕ1 )
= Re { 1 e j ωot }
V
then:
t
v2(t ) =   ∫ g (t − t ′) Re {V e                          }dt ′
j ωot ′
1
−∞

Now, since the impulse function g (t ) is real-valued (this is
really important!) it can be shown that:

Jim Stiles                       The Univ. of Kansas                              Dept. of EECS
1/21/2007     A Complex Representation of Sinusoidal Functions.doc           6/8

t
v2(t ) =   ∫ g (t − t ′) Re {V e                }dt ′
j ωot ′
1
−∞

⎧t                             ⎫
= Re ⎨ ∫ g (t − t ′ )V1 e j ωot dt ′⎬
′

⎩ −∞                           ⎭

Now, applying what we have previously learned;

⎧t                              ⎫
v2(t ) = Re ⎨ ∫ g (t − t ′ )V1 e j ωot ′dt ′⎬
⎩ −∞                            ⎭
⎧ t                            ⎫
= Re ⎨ 1 ∫ g (t − t ′ ) e j ωot dt ′⎬
V                        ′

⎩ −∞                           ⎭
= Re { 1 G (ω0 ) e j ωot }
V

Thus, we finally can conclude the real-valued output v2(t ) due
to the real-valued input:

v1(t ) =Vm 1 cos (ωot + ϕ1 )
= Re { 1 e j ωot }
V
is:

v2(t ) = Re { 2 e j ωot }
V
=Vm 2 cos (ωot + ϕ2 )
where:

V2 = G (ωo )V1

The really important result here is the last one!

Jim Stiles                     The Univ. of Kansas                     Dept. of EECS
1/21/2007         A Complex Representation of Sinusoidal Functions.doc             7/8

C
+                                                   +

v1(t ) =Vm 1 cos (ωot + ϕ1 )              L     R        v2(t ) = Re {G (ωo )V1 e j ωot }

−                                                   −

The magnitude and phase of the output sinusoid (expressed as
complex value V2 ) is related to the magnitude and phase of the
input sinusoid (expressed as complex value V1 ) by the system
eigen value G (ωo ) :
V2
= G (ωo )
V1

Therefore we find that really often in electrical engineering,
we:

1. Use sinusoidal (i.e., eigen function) sources.

2. Express the voltages and currents created by these
sources as complex values (i.e., not as real functions of
time)!

For example, we might say “ V3 = 2.0 ”, meaning:

V3 = 2.0 = 2.0 e j 0                            {                 }
⇒ v3 (t ) = Re 2.0 e j 0e j ωot = 2.0 cos ωot

Jim Stiles                        The Univ. of Kansas                        Dept. of EECS
1/21/2007           A Complex Representation of Sinusoidal Functions.doc                8/8

Or “ I L = −3.0 ”, meaning:

I L = −2.0 = 3.0 e j π      ⇒      iL (t ) = Re {3.0 e j π e j ωot } = 3.0 cos (ωot + π )

Or “Vs = j ”, meaning:

Vs = j = 1.0 e
( )
j π2
⇒ v s (t ) = Re 1.0 e {          ( ) j ωot
j π2
e     }             (
= 1.0 cos ωot + π 2      )
* Remember, if a linear circuit is excited by a sinusoid (e.g.,
eigen function exp ⎡ j ω 0t ⎤), then the only unknowns are
⎣        ⎦
the magnitude and phase of the sinusoidal currents and
voltages associated with each element of the circuit.

* These unknowns are completely described by complex
values, as complex values likewise have a magnitude and
phase.

* We can always “recover” the real-valued voltage or
current function by multiplying the complex value by
exp ⎡ j ω 0t ⎤ and then taking the real part, but typically we
⎣        ⎦
don’t—after all, no new or unknown information is
revealed by this operation!

+                C                                     +

V1                             L       R            V2 = G (ωo )V1

−                                                      −

Jim Stiles                          The Univ. of Kansas                           Dept. of EECS
1/21/2007       Analysis of Circuits Driven by Arbitrary Functions.doc         1/6

Analysis of Circuits Driven
by Arbitrary Functions
Q: What happens if a linear circuit is excited by some
function that is not an “eigen function”? Isn’t limiting our
analysis to sinusoids too restrictive?

A:     Not as restrictive as you might think.

Because sinusoidal functions are the eigen-functions of linear,
time-invariant systems, they have become fundamental to
much of our electrical engineering infrastructure—particularly
with regard to communications.

For example, every radio and TV station is assigned its very
own eigen function (i.e., its own frequency ω )!

It is very important that we use eigen functions for
electromagnetic communication, otherwise the received signal
might look very different from the one that was transmitted!

ψ n (t ) ≠ e j ωnt

Jim Stiles                       The Univ. of Kansas                     Dept. of EECS
1/21/2007           Analysis of Circuits Driven by Arbitrary Functions.doc               2/6

With sinusoidal functions (being eigen functions and all), we
know that receive function will have precisely the same form
as the one transmitted (albeit quite a bit smaller).

Thus, our assumption that a linear circuit is excited
by a sinusoidal function is often a very accurate and
practical one!

Q: Still, we often find a circuit that is not driven by a
sinusoidal source. How would we analyze this circuit?

A: Recall the property of linear operators:

L ⎡a y1 + b y2 ⎤ = a L [ y1 ] + b L [ y2 ]
⎣            ⎦

We now know that we can expand the function:

∞
v (t ) = a0 ψ 0 (t ) + a1 ψ 1 (t ) + a2 ψ 2 (t ) +        =
n
∑ an ψ n (t )
=−∞

and we found that:

⎡ ∞             ⎤   ∞
L ⎡v (t )⎤ = L ⎢ ∑ an ψ n (t ) ⎥ = ∑ an L ⎡ψ n (t )⎤
⎣      ⎦                                ⎣        ⎦
⎣n =−∞          ⎦ n =−∞

Finally, we found that any linear operation L [ψ n (t )] is greatly
simplified if we choose as our basis function the eigen
function of linear systems:

Jim Stiles                           The Univ. of Kansas                           Dept. of EECS
1/21/2007               Analysis of Circuits Driven by Arbitrary Functions.doc                                   3/6

⎧e j ωn t for 0 ≤ t ≤T
⎪                                                                                             ⎛ 2π ⎞
ψ n (t ) = ⎨                                                               where           ωn = n ⎜           ⎟
⎪0 for t < 0,t >T                                                                             ⎝T ⎠
⎩

so that:
L ⎡ψ n (t )⎤ = G (ωn ) e j ωnt
⎣        ⎦

Thus, for the example:
C
+                                                                  +

v1(t )                                       L    R               v2(t )

−                                                                  −

1. Expand the input function v1 (t ) using the basis functions
ψ n (t ) = exp [ j ωnt ] :

∞
v1 (t ) =V01 e   j ω 0t
+V11 e      j ω1t
+V21 e   j ω2t
+   =
n
∑ Vn
=−∞
1   e j ωnt

where:
T
1
Vn 1 =         ∫ v1 (t ) e − j ωnt dt
T     0

Jim Stiles                                      The Univ. of Kansas                                        Dept. of EECS
1/21/2007                Analysis of Circuits Driven by Arbitrary Functions.doc                        4/6

2. Evaluate the eigen values of the linear system:

∞
G (ωn ) = ∫ g (t ) e − j ωn t dt
0

3. Perform the linear operaton (the convolution integral)
that relates v2 (t ) to v1 (t ) :

v2 (t ) = L ⎡v1 (t )⎤
⎣       ⎦
⎡ ∞              ⎤
= L ⎢ ∑ Vn 1 e j ωnt ⎥
⎣n =−∞           ⎦
∞
=
n
∑ Vn
=−∞
1   L ⎡e j ωnt ⎤
⎣        ⎦
∞
=
n
∑ Vn
=−∞
1   G (ωn ) e j ωnt

Summarizing:
∞
v2 (t ) =
n
∑ Vn
=−∞
2   e j ωnt

where:
Vn 2 = G (ωn )Vn 1

and:

T
1
∞
Vn 1 =       ∫v   1   (t ) e   − j ωnt
dt               G (ωn ) = ∫ g (t ) e − j ωn t dt
T   0                                                            0

Jim Stiles                                        The Univ. of Kansas                            Dept. of EECS
1/21/2007                 Analysis of Circuits Driven by Arbitrary Functions.doc                                   5/6

C
+                                                                           +

∞                                                                         ∞
v1(t ) =     ∑ Vn 1 e   j ωnt
L        R            v2(t ) =
n
∑ G (ωn )Vn
=−∞
1             1   e j ωnt
n =−∞

−                                                                           −

As stated earlier, the signal expansion used here is the
Fourier Series.

Say that the timewidth T of the signal v1 (t ) becomes infinite.
In this case we find our analysis becomes:

1
+∞
v2 (t ) =              ∫V   2   (ω ) e j ω t d ω
2π           −∞

where:
V2 (ω ) = G (ω )V1 (ω )

and:

+∞                                                  +∞
V1 (ω ) = ∫ v1 (t ) e        − j ωt
dt                 G (ω ) =    ∫ g (t ) e
− jω t
dt
−∞                                                  −∞

The signal expansion in this case is the Fourier Transform.

We find that as T → ∞ the number of discrete system eigen
values G (ωn ) become so numerous that they form a
continuum—G (ω ) is a continuous function of frequencyω .

Jim Stiles                                    The Univ. of Kansas                                          Dept. of EECS
1/21/2007          Analysis of Circuits Driven by Arbitrary Functions.doc                   6/6

We thus call the function G (ω ) the eigen spectrum or
frequency response of the circuit.

Q: You claim that all this fancy mathematics (e.g., eigen
functions and eigen values) make analysis of linear systems
and circuits much easier, yet to apply these techniques, we
must determine the eigen values or eigen spectrum:

∞                                            +∞
G (ωn ) = ∫ g (t ) e   − j ωn t
dt        G (ω ) =   ∫ g (t ) e
− jω t
dt
0                                            −∞

Neither of these operations look at all easy. And in addition
to performing the integration, we must somehow determine
the impulse function g (t ) of the linear system as well !

Just how are we supposed to do that?

A: An insightful question! Determining the impulse response
g (t ) and then the frequency response G (ω ) does appear to be
exceedingly difficult—and for many linear systems it indeed
is!

However, much to our great relief, we can determine
the eigen spectrum G (ω ) of linear circuits without
having to perform a difficult integration. In fact, we
don’t even need to know the impulse response g (t ) !

Jim Stiles                            The Univ. of Kansas                             Dept. of EECS
1/21/2007                     The Eigen Spectrum.doc                       1/12

The Eigen Spectrum
of Linear Circuits
Recall the linear operators that define a capacitor:

d vC (t )
LC ⎡vC (t )⎤ = iC (t ) = C
Y ⎣       ⎦                     dt

t
1
LZ ⎡iC (t )⎤ = vC (t ) =        ∫ iC (t ′) dt ′
C
⎣       ⎦               C   −∞

We now know that the eigen function of these linear, time-
invariant operators—like all linear, time-invariant
operartors—is exp [ j ω t ] .

The question now is, what is the eigen spectrum of each of
these operators? It is this spectrum that defines the
physical behavior of a given capacitor!

For vC (t ) = exp [ j ω t ] , we find:

iC (t ) = LC ⎡vC (t )⎤
Y ⎣       ⎦
d e j ωt
=C
dt
= ( j ωC ) e j ωt

Jim Stiles                      The Univ. of Kansas                   Dept. of EECS
1/21/2007                   The Eigen Spectrum.doc                      2/12

Just as we expected, the eigen function exp [ j ωt ] “survives”
the linear operation unscathed—the current function i (t ) has
precisely the same form as the voltage function
v (t ) = exp [ j ωt ] .

The only difference between the current and voltage is the
multiplication of the eigen spectrum, denoted as GY (ω ) .
C

i (t ) = LC ⎡v (t ) = e j ωt ⎤ = GY (ω ) e j ωt
Y ⎣                ⎦
C

Since we just determined that for this case:

i (t ) = ( j ωC ) e j ωt

it is evident that the eigen spectrum of the linear operation:

d v (t )
i (t ) = LC ⎡v (t )⎤ = C
Y ⎣      ⎦             dt
is:
jπ 2
GY (ω ) = j ω C = ω C e
C
!!!

So for example, if:

v (t ) = Vm cos (ωot + ϕ )

{(
= Re Vm e
jϕ
)e }j ωot

we will find that:

Jim Stiles                    The Univ. of Kansas                  Dept. of EECS
1/21/2007                       The Eigen Spectrum.doc                                               3/12

LC ⎡(Vm e j ϕ ) e j ωot ⎤ = GY (ωo ) (Vm e j ϕ ) e j ωot
Y ⎣                    ⎦
C

(
= ωC e
jπ 2
) (V e m
jϕ
)e   j ωot

(
= ωC Vm e
(
j π 2 +ϕ
)
) e j ωot

Therefore:

{
iC (t ) = Re ωC Vme
(
j ϕ +π 2    ) j ωot
e         }
(
= ωC Vm cos ωot + ϕ + π
2   )
= −ωC Vm sin ( ωot + ϕ )

Hopefully, this example again emphasizes that these real-
valued sinusoidal functions can be completely expressed in
terms of complex values. For example, the complex value:

VC = Vme j ϕ

means that the magnitude of the sinusoidal voltage is VC =Vm ,
and its relative phase is ∠VC = ϕ .

The complex value:

IC = GY (ω )VC
C

(
= ωC e
jπ 2
)V  C

likewise means that the magnitude of the sinusoidal current
is:

Jim Stiles                        The Univ. of Kansas                                           Dept. of EECS
1/21/2007                         The Eigen Spectrum.doc                            4/12

IC = GY (ω )VC
C

= GY (ω ) VC
C

= ωC Vm

And the relative phase of the sinusoidal current is:

∠IC = ∠GY (ω ) + ∠VC
C

=π 2+ϕ

We can thus summarize the behavior of a capacitor with the
simple complex equation:
IC = ( j ωC )VC

+
IC = ( j ωC )VC
VC                 C
(
= ωC e
jπ2
)V   C

−

that describe a capacitor:

t
1
vC (t ) = LZ ⎡iC (t )⎤ =           ∫ iC (t ′) dt ′
C
⎣       ⎦        C    −∞

Now, if the capacitor current is the eigen function
iC (t ) = exp [ j ωt ] , we find:

Jim Stiles                             The Univ. of Kansas                     Dept. of EECS
1/21/2007                   The Eigen Spectrum.doc                                      5/12

t
1
LZ ⎡e
C
⎣
j ωt
⎤=
⎦ C         ∫e
j ωt ′
dt ′
−∞

⎛ 1 ⎞ j ωt
=⎜      ⎟e
⎝ j ωC ⎠

where we assume i (t = −∞ ) = 0 .

Thus, we can conclude that:

⎛ 1 ⎞ j ωt
LC ⎡e j ωt ⎤ = GZ (ω ) e j ωt = ⎜
Z ⎣       ⎦
C
⎟e
⎝ j ωC ⎠

Hopefully, it is evident that the eigen spectrum of this linear
operator is:

1             −j            1           (
j 3π 2   )
GZ (ω ) =
C
=            =          e
jω C             ωC           ωC

And so:
⎛     ⎞ 1
VC = ⎜         ⎟I
⎝ jωC ⎠ C

Q: Wait a second! Isn’t this essentially the same result as
the one derived for operator LC ??
Y

A: It’s precisely the same! For both operators we find:

VC   1
=
IC j ω C

Jim Stiles                    The Univ. of Kansas                                  Dept. of EECS
1/21/2007                 The Eigen Spectrum.doc                          6/12

This should not be surprising, as both operators LC and LC
Y      Z

relate the current through and voltage across the same
device (a capacitor).

The ratio of complex voltage to complex current is of course
referred to as the complex device impedance Z.

V
Z
I

An impedance can be determined for any linear, time-invariant
one-port network—but only for linear, time-invariant one-port
networks!

Generally speaking, impedance is a function of frequency. In
fact, the impedance of a one-port network is simply the eigen
spectrum GZ (ω ) of the linear operator LZ :

+ I
LZ ⎡i (t )⎤ = v (t )
⎣      ⎦
V =Z I        V                Z
Z = GZ (ω )
−

Note that impedance is a complex value that provides us with
two things:

Jim Stiles                  The Univ. of Kansas                      Dept. of EECS
1/21/2007                  The Eigen Spectrum.doc                  7/12

1. The ratio of the magnitudes of the sinusoidal voltage and
current:
V
Z =
I

2. The difference in phase between the sinusoidal voltage
and current:
∠Z = ∠ V − ∠ I

Q: What about the linear operator:

LY ⎣v (t )⎤ = i (t ) ??
⎡      ⎦

A: Hopefully it is now evident to you that:

1           1
GY (ω ) =                   =
GZ (ω )             Z

The inverse of impedance is admittance Y:

1       I
Y             =
Z           V

Now, returning to the other two linear circuit elements, we
find (and you can verify) that for resistors:

LR ⎡vR (t )⎤ = iR (t )
Y ⎣       ⎦                 ⇒ GY (ω ) = 1 R
R

LR ⎡iR (t )⎤ = vR (t )
Z ⎣       ⎦                 ⇒ GZ (ω ) = R
R

Jim Stiles                   The Univ. of Kansas              Dept. of EECS
1/21/2007                          The Eigen Spectrum.doc                               8/12

and for inductors:

1
LL ⎡v L (t )⎤ = iL (t )
Y ⎣        ⎦              ⇒ GY (ω ) =
L

j ωL

LZ ⎡iL (t )⎤ = v L (t )
L
⎣       ⎦              ⇒ GZ (ω ) = j ω L
L

meaning:

1                                              1                     ( )
j π2
ZR =         = R = R ej0           and          ZL =        = j ωL = ωL e
YR                                             YL

Now, note that the relationship

V
Z =
I

forms a complex “Ohm’s Law” with regard to complex
currents and voltages.

Additionally, ICBST (It Can Be Shown That) Kirchoff’s Laws
are likewise valid for complex currents and voltages:

∑ In
n
=0                  ∑Vn
n
=0

where of course the summation represents complex addition.

Jim Stiles                           The Univ. of Kansas                         Dept. of EECS
1/21/2007                  The Eigen Spectrum.doc                             9/12

As a result, the impedance (i.e., the eigen spectrum) of any
one-port device can be determined by simply applying a basic
knowledge of linear circuit analysis!

Returning to the example:

I                C
+

V         V                                       L     R
Z =
I
−

And thus using out basic circuits knowledge, we find:

Z = ZC + Z R Z L =            1
j ωC   + R j ωL

Thus, the eigen spectrum of the linear operator:

LZ ⎡i (t )⎤ = v (t )
⎣      ⎦

For this one-port network is:

GZ (ω ) =    1
j ωC   + R j ωL

Look what we did! We were able to determine GZ (ω ) without
explicitly determining impulse response gZ (t ) , or having to
perform any integrations!

Jim Stiles                   The Univ. of Kansas                         Dept. of EECS
1/21/2007                        The Eigen Spectrum.doc                            10/12

Now, if we actually need to determine the voltage function
v (t ) created by some arbitrary current function i (t ) , we
integrate:

1
+∞
v (t ) =       ∫G         (ω ) I (ω ) e j ω t d ω
2π
Z
−∞

1
+∞
=
2π     ∫(
−∞
1
j ωC   + R j ω L ) I (ω ) e j ω t d ω

where:
+∞
I (ω ) =          ∫ i (t ) e − j ωt dt
−∞

Otherwise, if our current function is time-harmonic (i.e.,
sinusoidal with frequency ω ), we can simply relate complex
current I and complex voltage V with the equation:

V =Z I
= ( 1 j ωC + R j ω L ) I

Similarly, for our two-port example:

C
+                                                       +

V1                                    L             R   V2

−                                                       −

Jim Stiles                         The Univ. of Kansas                         Dept. of EECS
1/21/2007                  The Eigen Spectrum.doc                   11/12

we can likewise determine from basic circuit theory the eigen
spectrum of linear operator:

L21 ⎡v1 (t )⎤ = v2 (t )
⎣       ⎦
is:

Z L ZR                   j ωL R
G21(ω ) =                =
ZC + Z L Z R           1
+ j ωL R
j ωC

so that:
V2 = G21(ω )V1

or more generally:

1
+∞
v2(t ) =       ∫ G21 (ω )V1(ω ) e j ωt d ω
2π    −∞

where:
+∞
V1(ω ) = ∫ v1(t ) e − j ωt dt
−∞

Finally, a few important definitions involving impedance and

Re {Z }        Resistance R

Im {Z }         Reactance X

Jim Stiles                    The Univ. of Kansas               Dept. of EECS
1/21/2007                    The Eigen Spectrum.doc                12/12

Im {Y }    Susceptance B

Therefore:

Z = R + jX                  Y = G + jB

But be careful!

Although:

1    1
Y = G + jB =              =
R + jX Z

keep in mind that:

1                                 1
G ≠                and              B≠
R                                  X

Jim Stiles                     The Univ. of Kansas             Dept. of EECS

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