DSBSC Demodulators

The process of extracting an original message signal from DSBSC wave is known as detection or demodulation of DSBSC. The following demodulators (detectors) are used for demodulating DSBSC wave.

Coherent Detector

Costas Loop

Coherent Detector

Here, the same carrier signal (which is used for generating DSBSC signal) is used to detect the message signal. Hence, this process of detection is called as coherent or synchronous detection. Following is the block diagram of the coherent detector.

In this process, the message signal can be extracted from DSBSC wave by multiplying it with a carrier, having the same frequency and the phase of the carrier used in DSBSC modulation. The resulting signal is then passed through a Low Pass Filter. Output of this filter is the desired message signal.

Let the DSBSC wave be

$$sleft ( t ight )= A_c cosleft ( 2 pi f_ct ight )m left ( t ight )$$

The output of the local oscillator is

$$cleft ( t ight )= A_c cosleft ( 2 pi f_ct+ phi ight )$$

Where, $phi$ is the phase difference between the local oscillator signal and the carrier signal, which is used for DSBSC modulation.

From the figure, we can write the output of product modulator as

$$vleft ( t ight )=sleft ( t ight )cleft ( t ight )$$

Substitute, $sleft ( t ight )$ and $cleft ( t ight )$ values in the above equation.

$$Rightarrow vleft ( t ight )=A_c cos left ( 2 pi f_ct ight )mleft ( t ight )A_c cos left ( 2 pi f_ct + phi ight )$$

$={A_{c}}^{2} cos left ( 2 pi f_ct ight ) cos left ( 2 pi f_ct + phi ight )mleft ( t ight )$

$=frac{{A_{c}}^{2}}{2}left [ cosleft ( 4 pi f_ct+ phi ight )+ cos phi ight ]mleft ( t ight )$

$$vleft ( t ight )=frac{{A_{c}}^{2}}{2} cosphi mleft ( t ight )+frac{{A_{c}}^{2}}{2} cos left ( 4 pi f_ct+ phi ight )mleft ( t ight )$$

In the above equation, the first term is the scaled version of the message signal. It can be extracted by passing the above signal through a low pass filter.

Therefore, the output of low pass filter is

$$v_0t=frac{{A_{c}}^{2}}{2} cos phi m left ( t ight )$$

The demodulated signal ampptude will be maximum, when $phi=0^0$. That’s why the local oscillator signal and the carrier signal should be in phase, i.e., there should not be any phase difference between these two signals.

The demodulated signal ampptude will be zero, when $phi=pm 90^0$. This effect is called as quadrature null effect.

Costas Loop

Costas loop is used to make both the carrier signal (used for DSBSC modulation) and the locally generated signal in phase. Following is the block diagram of Costas loop.

Costas loop consists of two product modulators with common input $sleft ( t ight )$, which is DSBSC wave. The other input for both product modulators is taken from Voltage Controlled Oscillator (VCO) with $-90^0$ phase shift to one of the product modulator as shown in figure.

We know that the equation of DSBSC wave is

$$sleft ( t ight )=A_c cosleft ( 2 pi f_ct ight )mleft ( t ight )$$

Let the output of VCO be

$$c_1left ( t ight )=cosleft ( 2 pi f_ct + phi ight )$$

This output of VCO is appped as the carrier input of the upper product modulator.

Hence, the output of the upper product modulator is

$$v_1left ( t ight )=sleft ( t ight )c_1left ( t ight )$$

Substitute, $sleft ( t ight )$ and $c_1left ( t ight )$ values in the above equation.

$$Rightarrow v_1left ( t ight )=A_c cos left ( 2 pi f_ct ight )mleft ( t ight ) cosleft ( 2 pi f_ct + phi ight )$$

After simppfying, we will get $v_1left ( t ight )$ as

$$v_1left ( t ight )=frac{A_c}{2} cos phi mleft ( t ight )+frac{A_c}{2} cosleft ( 4 pi f_ct + phi ight )mleft ( t ight )$$

This signal is appped as an input of the upper low pass filter. The output of this low pass filter is

$$v_{01}left ( t ight )=frac{A_c}{2} cos phi mleft ( t ight )$$

Therefore, the output of this low pass filter is the scaled version of the modulating signal.

The output of $-90^0$ phase shifter is

$$c_2left ( t ight )=cosleft ( 2 pi f_ct + phi-90^0 ight )= sinleft ( 2 pi f_ct + phi ight )$$

This signal is appped as the carrier input of the lower product modulator.

The output of the lower product modulator is

$$v_2left ( t ight )=sleft ( t ight )c_2left ( t ight )$$

Substitute, $sleft ( t ight )$ and $c_2left ( t ight )$ values in the above equation.

$$Rightarrow v_2left ( t ight )=A_c cosleft ( 2 pi f_ct ight )mleft ( t ight ) sin left ( 2 pi f_ct + phi ight )$$

After simppfying, we will get $v_2left ( t ight )$ as

$$v_2left ( t ight )=frac{A_c}{2} sin phi mleft ( t ight )+frac{A_c}{2} sin left ( 4 pi f_ct+ phi ight )mleft ( t ight )$$

This signal is appped as an input of the lower low pass filter. The output of this low pass filter is

$$v_{02}left ( t ight )=frac{A_c}{2} sin phi mleft ( t ight )$$

The output of this Low pass filter has $-90^0$ phase difference with the output of the upper low pass filter.

The outputs of these two low pass filters are appped as inputs of the phase discriminator. Based on the phase difference between these two signals, the phase discriminator produces a DC control signal.

This signal is appped as an input of VCO to correct the phase error in VCO output. Therefore, the carrier signal (used for DSBSC modulation) and the locally generated signal (VCO output) are in phase.