DSP OHT 1 Cheat Sheet PDF

Title DSP OHT 1 Cheat Sheet
Author Syed Shaharyaar Hussain
Course Signals and systems
Institution National University of Sciences and Technology
Pages 2
File Size 478.8 KB
File Type PDF
Total Downloads 49
Total Views 141

Summary

This is formula sheet compilation by my batch mates Usama Mirza and Hamza Chippa for the course of Digital Signal Processing....


Description



If ROC contains unit circle then the system is stable If ROC contains infinity then the system is causal ROC cannot contain any poles ROC must be a connected region

x[n] = ∑ x[k]δ[n − k] k=− ∞ ∞

u[n] = ∑ δ[n − k] k=0

δ [n] = u[n] − u[n − 1] N = 2πk ω I deal delay system : y [n] = x [n − nd ] 1 M1 +M2 +1

M oving Average System : y [n] =

Sampling ∞

s(t) = ∑ δ (t − nT s )

M2

n=− ∞

∑ x [n − k ]





xs (t) = xc (t)s(t) = ∑ xc(t)δ(t − nT s) = ∑ xc(nT s)δ(t − nT s)

k=− M 1

n=− ∞

n=− ∞

n

Accumulator System : y[n] = ∑ x[k]

S (jΩ) =

k=− ∞

2π Ts

C ompressor System : y [n] = x[Mn]



∑ δ(Ω − kΩ s), Ω s = 2π /T

s

k=− ∞ ∞

X s (jΩ) =

1 X (jΩ) 2π c

Finite Impulse Response (FIR) Infinite Impulse Response (IIR)

1 * S(jΩ) = T s ∑ X c(j(Ω − kΩ s)) k=− ∞

Memoryless: Depends only on present value on n h[n] = 0, for n =/ 0 Causal: Doesn’t depend on future values of n h[n] = 0, for n < 0

Ωs ≥ 2Ω N , Ω N is the greatest frequency in x c(t)

Stable: Finite output for finite input ∞

∑ ∣h[n] ∣ has to be finite

n=− ∞

Aliasing if Nyquist’s criteria not satisfied

Linear System: A x1 [n] + B x2 [n] → Ay 1 [n] + By 2[n] Time Invariant: x[n − no ] → y [n − no ]

Convolution:

Original signal can be recovered using a low pass filter



x[n] * h[n] = ∑ x [k]h[n − k ] k= −∞

x[n] * δ[n] = x[n], x[n] * δ[n − k] = x[n − k] Complex exponentials are eigenfunctions of LTI Systems H(ej⍵ ) is the eigenvalue of an LTI System ∞

Fourier Transform: X (ejω ) = ∑ x[n]e − jωn (Periodic with period = 2𝜋) n= −∞

Synthesis Equation: x[n] =

1 2π

∫ X(e j ω)e j ωndω 2π

Fourier Series

Fourier exists if x[n] is absolutely summable

ak =



Z-Transform: X (z) = ∑ x[n]z −n n= −∞

Synthesis Equation: x[n] =

Finite signal

Right sided signal

Left sided signal

Double sided signal

1 N

∑ x[n]e −jkω on Periodic with Period N n=

x[n] = ∑ ak ejkωo n 1 2πj

k=

∮ X (z )z n −1 dz C

Entire z plane except possibly z=0 or z=∞

Table 5: Properties of the Discrete-Time Fourier Transform 1 Z X(ejω ) ej ωndω x [n] = 2π 2π +∞ X x [n]e−jωn X(ejω ) =

Table 2: Properties of the Discrete-Time Fourier Series X X ak ejk (2π/N )n x [n ] = ak ejkω0 n = k=

1 X

ak =

Property

Time Scaling

x [n]e−jkω0 n =

n=

1 X

N

x [n]e−jk (2π/N )n



Fourier series coefficients

ak bk

Periodic with period N and fundamental frequency ω 0 = 2π/N

Ax [n] + By [n] x [n − n0 ] ejM (2π/N)n x [n] x ∗ [n ] x [−n]  x [n/m] if n is a multiple of m x (m) [n] = 0 if n is not a multiple of m



Periodic with period N

Aak + Bbk ak e−jk (2π/N )n 0 ak−M ∗ a−k a−k viewed as 1 ak periodic with m period mN

X

Aperiodic Signal

!

Convolution Multiplication

x [n]y[n]

Differencing in Time

x [r]y[n − r]

Nak bk X

x [n]y[n]

Fourier transform

x [n] y[n] ax [n] + by[n] x [n − n0 ] ej ω0n x [n] x ∗ [n] x [−n]  x [n/k ], if n = multiple of k x (k) [n] = 0, if n 6= multiple of k x [n] ∗ y[n]

Time Expansions

r=hNi

Multiplication

Property

Linearity Time-Shifting Frequency-Shifting Conjugation Time Reversal

(periodic with period mN )

Periodic Convolution

x [n] − x[n − 1] n X x[k]

Accumulation

Running Sum

x [n] − x [n − 1] n  X finite-valued and x[k] periodic only if a = 0 0 k=−∞

Conjugate Symmetry for Real Signals

x [n] real

Real and Even Signals

x [n] real and even

Real and Odd Signals

x [n] real and odd

Even-Odd Decomposition of Real Signals

(1 − e−jk (2π/N ) )ak   1 ak (1 − e−jk (2π/N ) )  ∗ a = a k −k   ℜe{ak } = ℜe{a−k } ℑm{ ak } = −ℑm{ a−k }  | ak | = | a−k |   0) or ∞ (if m < 0)

Differentiation in the z-Domain

Pn

1 1−z −1 X(z)

nx[n]

z) −z dX( dz

k=−∞ x[k]

Initial Value Theorem If x[n] = 0 for n < 0, then x[0] = limz →∞ X(z)

π

+∞ X

π j

+∞ X

Fourier series coefficients (if periodic) ak 2πm = N 1, k = m, m ± N, m ± 2N , . . . 0, otherwise irrational ⇒ The signal is aperiodic ω0 = 2πm N  1 k = ±m, ±m ± N, ±m ± 2N, . . . 2, ak = 0, otherwise ω0 irrational ⇒ The signal is aperiodic 2π ω0 = 2πr  N1 k = r, r ± N, r ± 2N , . . .  2j , 1 − 2j = , k = −r, −r ± N, −r ± 2N, . . .  0, otherwise ω0 irrational ⇒ The signal is aperiodic 2π 1, k = 0, ±N, ±2N , . . . 0, otherwise

(a)

ω0 ak

{δ(ω − ω0 − 2πl) + δ(ω + ω0 − 2πl)} (b) (a) {δ(ω − ω0 − 2πl) − δ(ω + ω0 − 2πl)}

ak

l=−∞

(b) 2π

+∞ X

δ(ω − 2πl)

Periodic  square wave 1, |n| ≤ N1 0, N1 < |n| ≤ N/2 and x[n + N ] = x[n] +∞ X δ[n − kN ] x[n] =



+∞ X

  2πk ak δ ω − N

k=−∞

2π N

k=−∞

ak =

k=−∞



δ ω−

2πk N



1 1 − ae−jω sin[ω (N1 + 1 )] 2 sin(ω/2)  1, 0 ≤ |ω| ≤ W X(ω) = 0, W < |ω| ≤ π X(ω)periodic with period 2π

an u[n], |a| < 1 

1, |n| ≤ N1 0, |n| > N1   sinc Wπn 0 0

9. [cos ω0n]u[n]

1−[cos ω0 ]z−1 1−[2 cos ω0 ]z−1 +z −2

|z| > 1

At least the intersection of R and |z| > 1

10. [sin ω0n]u[n]

[sin ω0 ]z−1 −2 1−[2 cos ω0 ]z−1 +z

|z| > 1

11. [r n cos ω0n]u[n]

1−[r cos ω0 ]z−1 −2 1−[2r cos ω0 ]z −1 +r 2 z

|z| > r

12. [r n sin ω0n]u[n]

[ r sin ω0 ] z 1−[2r cos ω0 ]z −1 +r 2 z−2

|z| > r

R

−1

Useful Infinite Summation Identities (|a| < 1) ∞ X k=0 ∞

X

ak =

1 1−a

kak =

a 2

(1 − a) X 2 k a2 + a k a = (1 − a)3 k=0 k=0 ∞...


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