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harmonska analiza

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10<br />

Polvalna simetrija signala<br />

Polvalna simetričnost ni ne liha ne soda (slika 1.4). Zanjo velja:<br />

x(t) = −x(t ± T 0 /2) (1.9)<br />

in<br />

Slika 1.4<br />

Primer polvalno simetričnega signala.<br />

a 0 = 0<br />

a 2k+1 = 4 ∫<br />

T 0<br />

b 2k+1 = 4 T 0<br />

∫<br />

T 0 /2<br />

T 0 /2<br />

cos(2k + 1)ω 0 t dt<br />

Četrtvalna simetrija sodega signala<br />

(1.10a)<br />

(1.10b)<br />

sin(2k + 1)ω 0 t dt , k = 0,1,2,... (1.10c)<br />

x( t)<br />

A<br />

t<br />

T 0 /2 T 0 /2 T 0 3T 0 /2<br />

Signal ima četrtvalno sodo simetrijo, če velja (slika 1.5):<br />

T 0<br />

A<br />

osnutek<br />

x(t) = x(−t) in x(t) = x(t + T 0 /2) . (1.11)<br />

V tem primeru Fourierove koeficiente lahko izračunamo z:<br />

a 0 = 0<br />

a 2k+1 = 8 ∫<br />

T 0<br />

T 0 /4<br />

(1.12a)<br />

x(t)cos(2k + 1)ω 0 t dt , k = 0,1,2,... (1.12b)<br />

b n = 0 . (1.12c)<br />

Četrtvalna simetrija lihega signala<br />

Signal ima četrtvalno liho simetrijo, če velja (slika 1.6):<br />

x(t) = x(−t) in x(t) = x(t + T 0 /2) . (1.13)

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