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Double-sideband suppressed-carrier transmission
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===Distortion and attenuation=== For demodulation, the demodulation oscillator's frequency and phase must be exactly the same as the modulation oscillator's, otherwise, distortion and/or attenuation will occur. To see this effect, take the following conditions: *Message signal to be transmitted: <math>f(t)</math> *Modulation (carrier) signal: <math>V_c\cos(\omega_c t)</math> *Demodulation signal (with small frequency and phase deviations from the modulation signal): <math>V'_c\cos\left[(\omega_c+\Delta\omega)t + \theta\right]</math> The resultant signal can then be given by :<math>f(t) \times V_c\cos(\omega_c t) \times V'_c\cos\left[(\omega_c+\Delta\omega)t + \theta\right]</math> ::<math>=\frac{1}{2}V_c V'_c f(t) \cos\left(\Delta\omega\cdot t+\theta\right) + \frac{1}{2}V_c V'_c f(t) \cos\left[(2\omega_c+\Delta\omega)t+\theta\right]</math> ::<math>\xrightarrow{\text{After low pass filter}} \frac{1}{2}V_c V'_c f(t) \cos\left(\Delta\omega\cdot t+\theta\right)</math> The <math>\cos\left(\Delta\omega\cdot t+\theta\right)</math> terms results in distortion and attenuation of the original message signal. In particular, if the frequencies are correct, but the phase is wrong, contribution from <math>\theta</math> is a constant attenuation factor, also <math>\Delta\omega\cdot t</math> represents a cyclic inversion of the recovered signal, which is a serious form of distortion. [[File:Demodulation distortion diagram.png]]
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