x(t) = 3 + 4 cos(20nt +30) + 2 sin(60nt) - 4 cos(70nt)

Introductory Circuit Analysis (13th Edition)
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ISBN:9780133923605
Author:Robert L. Boylestad
Publisher:Robert L. Boylestad
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Phasor Signals and Spectra
A useful periodic signal in system analysis is the signal
x(t) = Aej(@ot+0),
Im
wol+0
A cos (@of +0)
Re
-∞<t<∞
MT.
Im
Phase
@of+0
@ol+0
The rotating phasor Ae(+) can be related to a real, sinusoidal signal A cos(@ot+0)
in two ways. The first is by taking its real part,
fo
A cos (wol +0)
x(t) = A cos(@ot + 0) = Rex(1)
= Re Ae/(1+0)
112
-Re
and the second is by taking one-half of the sum of x(1) and its complex conjugate,
A cos(@pt + 0) = x(1) + X* (1)
1
Aej (@₂²+0) + = Ae¯j(1+0)
2
Example:
Sketch the single-sided and double-sided spectra of
Amplitude
Amplitude
A
I hj
A
fo
0
fo
x(t) = 3 + 4 cos(20nt +30) + 2 sin(60nt) - 4 cos(70nt)
cose
fo
A Acose+jAsino
Phase
0
fo
Transcribed Image Text:Phasor Signals and Spectra A useful periodic signal in system analysis is the signal x(t) = Aej(@ot+0), Im wol+0 A cos (@of +0) Re -∞<t<∞ MT. Im Phase @of+0 @ol+0 The rotating phasor Ae(+) can be related to a real, sinusoidal signal A cos(@ot+0) in two ways. The first is by taking its real part, fo A cos (wol +0) x(t) = A cos(@ot + 0) = Rex(1) = Re Ae/(1+0) 112 -Re and the second is by taking one-half of the sum of x(1) and its complex conjugate, A cos(@pt + 0) = x(1) + X* (1) 1 Aej (@₂²+0) + = Ae¯j(1+0) 2 Example: Sketch the single-sided and double-sided spectra of Amplitude Amplitude A I hj A fo 0 fo x(t) = 3 + 4 cos(20nt +30) + 2 sin(60nt) - 4 cos(70nt) cose fo A Acose+jAsino Phase 0 fo
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