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fundamentals of engineering supplied-reference handbook - Ventech!

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DIGITAL SIGNAL PROCESSING<br />

A discrete-time, linear, time-invariant (DTLTI) system with<br />

a single input x[n] and a single output y[n] can be described<br />

by a linear difference equation with constant coefficients <strong>of</strong><br />

the form<br />

y<br />

k<br />

l<br />

[ n]<br />

∑by[ n − i]<br />

= ∑ax[ n − i]<br />

+ i<br />

i<br />

i=<br />

1 i=<br />

0<br />

If all initial conditions are zero, taking a z-transform yields a<br />

transfer function<br />

H<br />

( z)<br />

Y<br />

=<br />

X<br />

∑ a z<br />

i<br />

( z)<br />

i=<br />

0<br />

=<br />

k ( z)<br />

k<br />

z + ∑<br />

l<br />

k −i<br />

k −i<br />

bi<br />

z<br />

i=<br />

1<br />

Two common discrete inputs are the unit-step function u[n]<br />

and the unit impulse function δ[n], where<br />

u<br />

⎧0<br />

⎨<br />

⎩1<br />

n < 0⎫<br />

n ≥ 0<br />

⎬<br />

⎭<br />

[] n =<br />

and δ[]<br />

n<br />

⎧1<br />

= ⎨<br />

⎩0<br />

n = 0 ⎫<br />

n ≠ 0<br />

⎬<br />

⎭<br />

The impulse response h[n] is the response <strong>of</strong> a discrete-time<br />

system to x[n] = δ[n].<br />

A finite impulse response (FIR) filter is one in which the<br />

impulse response h[n] is limited to a finite number <strong>of</strong> points:<br />

h<br />

k<br />

[] n ∑ a δ[<br />

n − i]<br />

= i<br />

i=<br />

0<br />

The corresponding transfer function is given by<br />

H () z<br />

k<br />

∑ a<br />

−i<br />

= i z<br />

i=<br />

0<br />

where k is the order <strong>of</strong> the filter.<br />

An infinite impulse response (IIR) filter is one in which the<br />

impulse response h[n] has an infinite number <strong>of</strong> points:<br />

h<br />

[] n a δ[<br />

n − i]<br />

∑ ∞<br />

= i<br />

i=<br />

0<br />

175<br />

ELECTRICAL AND COMPUTER ENGINEERING (continued)<br />

COMMUNICATION THEORY AND CONCEPTS<br />

The following concepts and definitions are useful for<br />

communications systems analysis.<br />

Functions<br />

Unit step,<br />

u (t)<br />

Rectangular<br />

pulse,<br />

Π(/ t τ )<br />

Triangular pulse,<br />

Λ(/ t τ )<br />

Sinc,<br />

sinc( at )<br />

Unit impulse,<br />

δ () t<br />

The Convolution Integral<br />

In particular,<br />

∫<br />

+∞<br />

⎧⎪<br />

0 t < 0<br />

ut () = ⎨<br />

⎪⎩ 1 t > 0<br />

⎧<br />

1<br />

⎪1<br />

t / τ <<br />

⎪<br />

2<br />

Π(/ t τ ) = ⎨<br />

⎪<br />

1<br />

⎪⎩<br />

0 t / τ ><br />

2<br />

⎧<br />

⎪<br />

1 − t/ τ t/<br />

τ < 1<br />

Λ(/ t τ ) = ⎨<br />

⎪⎩ 0 t / τ > 1<br />

∫<br />

sin( aπt) sinc( at)<br />

=<br />

aπt +∞<br />

−∞<br />

x( t+ t ) δ ( t) dt = x( t )<br />

0 0<br />

for every x(t) defined and<br />

continuous at t = t0. This is<br />

equivalent to<br />

∫<br />

+∞<br />

−∞<br />

xt () ∗ ht () = x( λ) ht ( −λ) dλ<br />

−∞<br />

∫<br />

x() t δ( t − t ) dt = x( t )<br />

+∞<br />

0 0<br />

= ht ( ) ∗ xt ( ) = h( λ) xt ( −λ) dλ<br />

−∞<br />

x() t ∗δ( t − t ) = x( t− t )<br />

0 0<br />

The Fourier Transform and its Inverse<br />

+∞ − j2πft −∞<br />

X( f) = x( t) e dt<br />

∫<br />

∫<br />

+∞ j2πft −∞<br />

x() t = X( f) e df<br />

We say that x(t) and X(f) form a Fourier transform pair:<br />

x() t ↔<br />

X( f)

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