Let :
f (t) be the information signal :
\omega_{R} be the angular RF, :
\omega_{I} be the angular IF and :
\omega_{s} be the angular subcarrier frequency. In direct modulation transmitter the information signal modulates the RF carrier. If the type of modulation is conventional
amplitude modulation the RF output is, : \mbox{RF}=(1+f(t))\cdot \sin(\omega_{R} t) Likewise in superheterodyne transmitter the modulated IF is; : \mbox{IF}=(1+f(t))\cdot \sin(\omega_{I} t) This signal is applied to a frequency mixer. The other input to the mixer is a high frequency subcarrier signal. :
\mbox{SC}= \sin( \omega_{s} t) The two signals are multiplied to give; : \mbox{IF}\cdot \mbox{SC}=(1+f(t))\cdot \sin(\omega_{I} t)\cdot \sin(\omega_{s} t) Applying well known rules of
trigonometry; :\mbox{IF}\cdot \mbox{SC}= \frac{1}{2}(1+f(t))\cdot (\cos(\omega_{s} t-\omega_{I} t)-\cos(\omega_{s}t +\omega_{I} t)) A filter at the output of the mixer filters out one of the terms at the right (usually the summation) leaving RF : \mbox{RF}= \frac{1}{2}(1+f(t)) \cdot \cos(\omega_{s} t-\omega_{I} t) Here
\omega_{s}-\omega_{I} is the required angular RF; i.e.,
\omega_R= \omega_{s}-\omega_{I} After phase and amplitude equalization, : \mbox{RF}=(1+f(t))\cdot \sin(\omega_{R} t) == Advantages of superheterodyne ==