complex numbers and complex-valued functions
TRANSCRIPT
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EECE 301
Signals & Systems
Prof. Mark Fowler
Discussion #1
Complex Numbers and Complex-Valued Functions Reading Assignment: Appendix A of Kamen and Heck
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Complex Numbers
Complex numbers arise as roots of polynomials.
1))((
1))((
11 2
=
=
==
jj
jj
jj
Rectangular form of a complex number:
}Im{
}Re{
zb
zajbaz
=
=+=
real numbers
Recall that the solution of
differential equationsinvolves finding roots of the
characteristic polynomial
So
Definition of
imaginary #j
and some
resulting
properties:
)()())((:
)()()()(:
bcadjbdacjdcjbaMultiply
dbjcajdcjbaAdd
++=++
+++=+++
The rules of addition and multiplication are straight-forward:
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Polar Form
jrez =
Polar form an alternate way to express a
complex number
Polar Form
good for multiplication and division
r> 0
Note: you may have learned polar form as r we will NOT use that here!!The advantage of therej is that when it is manipulated using rules of
exponentials and it behaves properly according to the rules of complex #s:
yxyxyxyx
aaaaaa+
== /))((
Dividing Using Polar Form
( )( ))(
2
1
2
1 21
2
1
=j
j
j
err
erer
2
2
222
111 jj ererz==
Multiplying Using Polar Form
( )( ))(
2121 2121 +
=jjj
errerer
( )njnn
jnnnjn
erz
errez
//1/1
=
==
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b
a
z = a + jb
Im
Re
r
Geometry of Complex Numbers
We need to be able convert between Rectangular and Polar Forms this is made
easy and obvious by looking at the geometry (and trigonometry) of complex #s:
r
a
b
cos
sin
ra
rb
=
=
=
+=
a
b
bar
1
22
tan
Conversion Formulas
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Since cos +jsin has the same expansion as e j we can say that:
jej =+ sincos
From Calc II: ...!6!4!2
1cos642
++=
...!7!5!3
sin753
++=
jjjjj
...!4!3!2
1sincos432
+++=+
j
jj
...
!4!3!2
1432
+++++=xxx
xex
Also From Calc II:
...
!4!3!2
1432
+++=
j
jej
Q: Why the formrej for polar form?? Start with trigonometry:
[ ] sincos)sin(cos jrrjrjbaz +=+=+=
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Complex Exponentials vs. Sines and Cosines
Eulers Equations:
(A)
(B)
(C)
(D)
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Summary of Rectangular & Polar Forms
Warning: Your calculatorwill give you the wrong answerwhenever you have a < 0. In other words, forz values that lie in
the II and III quadrants.
You can always fix this by either adding or subtracting .
Use common sense looking at the signs ofa and b will tell
you what quadrantz is in make sure your angle agrees with
that!!!
Summary of Rectangular & Polar Forms
==
+==
=
abz
barz
rrez j
1
22
tan
],(0
Polar Form:
sin}Im{
cos}Re{
rbz
raz
jbaz
==
==+=
Rect Form:
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Conjugate ofZ
jjrezrez
jbazjbaz
==
=+=
*
*
Denoted as
zz or*
Properties ofz*
222*
*
))((.2
}Re{2.1
zbajbajbazz
zzz
=+=+=
=+
U it Ci l
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Unit Circle
Im
Re
1
Unit Circle: A set of complex numbers with
magnitude of 1 (|z| =1)
Allz on the unit circle look like: je1
Re
Im
Four special points on the unitcircle:
2j
ej =
01 je=
2j
ej
=
je=1
=
=
=
=
=
=
=
,...10,6,2,1
,...8,4,0,1
...,11,7,3,
...,9,5,1,
integersallfor1
integereven1,
integerodd,1
2
2
n
n
nj
nj
e
e
n
ne
jn
jn
jn
Know these!!!
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A sinusoid is completely defined by its three parameters:
-AmplitudeA (for EEs typically in volts or amps or other physical unit)
-Frequency in radians per second
-Phase shift in radians
Tis the period of the sinusoid and is related to the frequency
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Phase shift (often just shortened to phase) shows up explicitly in the equation but
shows up in the plot as a time shift (because the plot is a function of time).
Q: What is the relationship between the plot-observed time shift and the equation-
specified phase shift?
A: We can write the time shift of a function by replacing tby t + to (more on this
later, but you should be able to verify that this is true!) Then we get:
)sin())(sin()( ooo ttAttAttf +=+=+
=
So we get that: = to (unit-wise this makes sense!!!)
Frequency can be expressed in two common units:
-Cyclic frequency: f= 1/T in Hz (1 Hz = 1 cycle/second)
-Radian Frequency: = 2/T(in radians/second)
From this we can see that these two frequency units have a simple conversion
factor relationship (like all other unit conversions e.g. feet and meters):
f 2=
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In circuits you used phasors (well call them static phasors here) the point of
using them is to make it EASY to analyze circuits that are driven by a single sinusoid.
Here is an example to refresh your memory!!
Find output voltage of the following circuit:
R = 1
L = 2mH4
1000cos5)( += ttx ?)( =ty
Use phasor and impedance ideas:
45:InputofPhasor
2:InductorofImpedance
j
L
ex
jLjZ
=
==
Use voltage divider to find output:
[ ]46.04 89.0521
2 j
jee
j
jxy
=
+=
Output phasor:
25.145.4 jey =
Output signal: )25.11000cos(45.4)( += tty
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Note that in using static phasors there was no need to carry around the
frequency it gets suppressed in the static phasor
BUT if you have multiple driving sinusoids (each at its own unique frequency)then youll need to keep that frequency in the phasor representation that leads to:
{ } )cos(Re)sin()cos(
oootjj
o
oo
tj
tAeeA
tjte
o
o
+=
+=
system)cos( ooo tA +
input
rotating
phasorModified
system
tjj
ooo eeA
Rotating phasor
output
rotating
phasor
Rotating Phasors
Keeping the frequency part
static phasor part
tjj
o
tj
oooo
oo
oo
eeA
eAtA
=
+ + )()cos(
[ ]
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[ ]
( )
[ ]
{ }
)cos(2
)(~Re22
)(*~)(~
)(*~:isWhat)cos()(
)(~If
oo
tjj
tj
oo
tj
tA
txtxtx
eAe
Ae
txtAtx
Aetx
oo
oo
oo
+=
=+
=
=
+=
=
+
++
Because rotating phasors take the value of a complex number at each
Instant of time they must follow all the rules of complex numbersEspecially: EULERS EQUATIONS!!
Rotating Phasors
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Rotating Phasors
Eulers Equations
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Viewing rotating phasor on the complex plane