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1. Continuous- and discrete- time signals 1. Complex numbers For any complex number, z∈ , we have
• Cartesian/algebraic form ; 1z x jy j= + = − where
{ }{ }
Re
Im
x z
y z
=
=
• Polar form ; 1jz r e jθ= ⋅ = −
{ } { } argr z z z= = The complex conjugate of a complex number: jz x jy r e∗ − θ= − = ⋅ The absolute value 2 2z x y= + 2z z z∗⋅ = Relation between polar and cartesian coordinates
2 2
cossin
arctg 0 0, 02 =
arctg 0, 0 0, 02
arctg 0, 0
x ry r
r x yy x x yxy x y x yxy x yx
= θ⎧⎨ = θ⎩⎧ = +⎪⎪ ⎧ π⎧>⎪ ⎪ = >⎪⎪ ⎪⎪ θ⎨ ⎨⎪ πθ = + π < ≥⎨⎪ ⎪− = <
⎪⎪⎪ ⎩⎪⎪ − π < <⎪⎪ ⎩⎩
Euler’s relation cos sinje jθ = θ+ θ
cos
2
sin2
j j
j j
e e
e ej
θ − θ
θ − θ
⎧ +θ =⎪
⎪⎨
−⎪ θ =⎪⎩
Modulus argument/phase
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Problems P1. Determine the Cartesian coordinates of the following complex numbers, depending on 0x and 0y , where we have: 0 0 0z x jy= +
a) 01 0
jz r e− θ= ⋅ b) 2 0z r=
c) ( )03 0
jz r e θ +π= ⋅
d) ( )04 0
jz r e θ +π−= ⋅
e) ( )05 0
2jz r e θ + π= ⋅ Sketch 1 2 5, ,...,z z z in the complex plane for the following cases of 0r and 0θ
0 0
0 0
2 4
2 2
r
r
π= θ =
π= θ =
Solution a)
( ) ( )[ ]
01 0 0 0 0
0 0 0
0 0
cos sin
cos sin
jz r e r j
r jx jy
− θ= ⋅ = ⋅ −θ + −θ⎡ ⎤⎣ ⎦= ⋅ θ − θ
= −
b) 2 2
2 0 0 0z r x y= = + c)
( ) ( ) ( )[ ]
03 0 0 0 0
0 0 0 0 0
cos sin
cos sin
jz r e r j
r j x jy
θ +π= ⋅ = ⋅ θ + π + θ + π⎡ ⎤⎣ ⎦= ⋅ − θ − θ = − −
d) ( )0
4 0 0 0jz r e x jyθ +π−= ⋅ = − +
e) ( )0
5 0 0 02jz r e x jyθ + π= ⋅ = +
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P2. Consider z a complex variable with its complex conjugate jz x jy r e∗ − θ= − = ⋅ Prove the following relations are true, where z , 1z and 2z are complex numbers.
a) 2z z r∗⋅ = b) 2 jz ez∗
θ=
c) { }2 Rez z z∗+ = d) { }2 Imz z j z∗− =
e) ( )1 2 1 2z z z z∗ ∗ ∗+ = + f) ( )1 2 1 2az z az z∗ ∗ ∗=
g) 1 1
2 2
z zz z
∗ ∗
∗
⎛ ⎞=⎜ ⎟
⎝ ⎠
Solution a) 2j jz z r e r e r∗ θ − θ⋅ = ⋅ ⋅ ⋅ =
b) 2j
jj
z r e ez r e∗
θθ
− θ⋅
= =⋅
c) { }2 2 Rez z x jy x jy x z∗+ = + + − = =
d) { }2 2 Imz z x jy x jy jy j z∗− = + − + = =
e) ( ) ( ) ( )1 2 1 1 2 2 1 2 1 2 1 2z z x jy x jy x x j y y z z∗ ∗ ∗ ∗+ = + + + = + − + = +
f) ( ) ( ) ( )1 2 1 21 21 2 1 2 1 2 1 2 1 2
jj j j jaz z a re r e ar r e a re r e az z∗∗ ∗ ∗θ +θ−θ θ − θ − θ= ⋅ ⋅ = = ⋅ =
g) 1 1
2 2
z zz z
∗ ∗
∗
⎛ ⎞=⎜ ⎟
⎝ ⎠
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Continuous-time signals Continuous-time unit impulse
( )0
0 0, t
t, t
∞ =⎧δ = ⎨ ≠⎩
Continuous-time unit step
( )1 00 0, t
t, t
≥⎧σ = ⎨ <⎩
Ramp signal
( ) ( )0
0 0t , t
r t t t, t
≥⎧= = σ⎨ <⎩
Even signal ( ) ( ) ( )2e
x t x tx t
+ −=
( ) ( )e ex t x t− =
Odd signal ( ) ( ) ( )2o
x t x tx t
− −=
( ) ( )o ox t x t− = −
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Any given signal x(t) has an odd part and an even part ( ) ( ) ( )e ox t x t x t= + With
( ) ( ) ( )2e
x t x tx t
+ −= and ( ) ( ) ( )
2ox t x t
x t− −
=
• Energy of a continuous-time signal
( ) 2W x t dt
∞
−∞
= ∫
If the signals has the support [ ]1 2,t t , the energy is:
( )2
1
2t
tW x t dt= ∫
Power of the continuous-time signal (again support [ ]1 2,t t )
( )2
1
2
2 1 2 1
1 t
t
WP x t dtt t t t
= =− − ∫
For periodic signals the power is computed over one period!!!
( )0
2
0
1TP x t dt
T= ∫
Problems P3. Consider the signal ( )x t represented below.
Sketch the following signals: a) ( )2x t − e) ( )1x t− − i) ( ) ( )x t t⋅ δ b) ( )2x t + f) ( )2x t j) ( ) ( ) ( )1 2x t t t⋅ ⎡σ − − σ − ⎤⎣ ⎦ c) ( )x t− g) ( )/ 2x t d) ( )3x t− + h) ( )2 4x t − Solution. a) ( )2x t − . The “new origin” is 2t = : 2 0t − = . This is a delayed version of the signal
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b) ( )2x t + . The “new origin” is 2t = − : ( )2 2 0x t t+ ⇒ + =
c) ( )x t− . The signal is reversed or “mirrored” on the time axis
d) ( )3x t− + same as c) with shifting on the time axis. The origin is shifted on 3t =
e) ( 1)
( 1)x t
t− −− +
f) ( )2x t . The support is compressed; this is signal compression in time.
new signal original signal2 t t′= ; for 2 1t t′= = ; on the new time axis we have 1/ 2t = and so on.
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g) ( )/ 2x t . The support is dilated; this is signal dilation in time.
new signal original signal/ 2t t′= ; for / 2 1t t′= = ; on the new time axis we have 2t = and so on.
h) ( )2 4x t − . 2 4 0 2t t− = ⇒ = . The origin is now in 2t = (time compression + shifting)
i) ( ) ( )x t t⋅ δ
j) ( ) ( ) ( )1 2x t t t⋅ ⎡σ − − σ − ⎤⎣ ⎦
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Discrete-time signals Discrete-time unit impulse (Dirac impulse)
[ ] 1 00 0, n
n, n
=⎧δ = ⎨ ≠⎩
Discrete-time unit step
[ ] 1, 00, 0
nn
n≥⎧
σ = ⎨ <⎩
Any given signal x[n] has an odd part and an even part [ ] [ ] [ ]e ox n x n x n= + with
[ ] [ ] [ ]2e
x n x nx n
+ −= and [ ] [ ] [ ]
2ox n x n
x n− −
=
Even signal: [ ] [ ]e ex n x n− = ; Odd signal: [ ] [ ]o ox n x n− = −
• Energy of a discrete-time signal
2[ ]n
W x n∞
=−∞
= ∑
If the signals has the support { }1 1 1 2, ,...,N N N+ , the energy is:
[ ]2
1
2N
n NW x n
== ∑
Power of the discrete-time signal (again support { }1 1 1 2, ,...,N N N+ )
[ ]2
1
2
2 1 2 1
11 1
N
n N
WP x nN N N N =
= =− + − +
∑
For periodic signals the power is computed over one period!!!
[ ] 21
n NP x n
N ∈= ∑
Problems P4. Consider the signal x[n] sketched below.
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Sketch the following signals: a) [ ]2x n − d) [ ]x n− g) [ ] [ ]1 3x n n− ⋅δ − b) [ ]1x n + e) [ ]2x n− c) [ ]2x n f) [ ] [ ]1x n n⋅σ − Solution. a) [ ]2x n − . The new origin is 2; for 2 0n n= − =
b) [ ]1x n + . The new origin is 1; for 1 0n n= − + =
c) [ ]2x n . We have
new original2 n n′= . Number "n" integer => n' even values: ... -2; 0; 2; 4...
d) [ ]x n−
e) [ ] ( )2 2x n x n− = ⎡− − ⎤⎣ ⎦ . The signal is reversed and then shifted or vice versa.
f) [ ] [ ]1x n n⋅σ −
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P5–Homework. Draw the odd and even signals of the x[n] signal represented below:
P6–Homework. Consider the discrete-time signal x[n] represented below.
Sketch the following signals: a) [ ]x n− d) [ ] [ ] [ ]( )2 1 2 2x n n n+ σ + −σ −
b) [ ]1x n + e) [ ] [ ] [ ]( )2 2x n n n+ σ + − σ − c) [ ] [ ]4 2x n n⋅ δ −
P7. a) If the signal [ ]x n is odd, prove that: [ ] [ ]lim 0N
Nn n NS x n x n
∞
→∞=−∞ =−
= = =∑ ∑
b) If [ ]1x n is even and [ ]2x n is odd, show that their product [ ] [ ]1 2x n x n⋅ is odd
c) For a finite energy signal [ ]x n , with the even and odd parts [ ]ex n and [ ]ox n , prove that:
[ ] [ ] [ ]2 2 2e o
n n nx n x n x n
∞ ∞ ∞
=−∞ =−∞ =−∞
= +∑ ∑ ∑
d) Verify by direct computation the relation from c) for the sketched signal.