The group of equations below describe the relationship of variables from a circuit(C stands for capicator, L is for inductor etc.). And the equation at the bottom shows how the transfer function is defined.
My question is how can the transfer function be determined from the group of equations above. And can you enunciate on that? A step by step enunciation would be really appreciated.
\begin{equation} \left\{ \begin{aligned} &V_A=V_{IN}\cdot \frac{\left(\frac{1}{j\omega C_A}\mid\mid\left(R_{A1}+R_{A2}\right)\right)}{\left(\frac{1}{j\omega C_A}\mid\mid\left(R_{A1}+R_{A2}\right)\right) + R_A + j\omega L_A}\cdot\frac{R_{A2}}{R_{A1}+R_{A2}}\\ &V_B=V_{IN}\cdot \frac{\left(\frac{1}{j(\omega+\pi) C_B}\mid\mid\left(R_{B1}+R_{B2}\right)\right)}{\left(\frac{1}{j(\omega+\pi) C_B}\mid\mid\left(R_{B1}+R_{B2}\right)\right) + R_B + j(\omega+\pi) L_B}\cdot\frac{R_{B2}}{R_{B1}+R_{B2}}\\ &V_{IN}=\left[V_{DC}-\left(V_A+V_B\right)\right]\cdot\frac{\Re_A\mid\mid\Re_B}{R_s+\left(\Re_A\mid\mid\Re_B\right)}\\ &\Re_A=\frac{1}{j\omega C_A}\mid\mid\left(R_{A1}+R_{A2}\right) + R_A + j\omega L_A\\ &\Re_B=\frac{1}{j\omega C_B}\mid\mid\left(R_{B1}+R_{B2}\right) + R_B + j\omega L_B\\ \end{aligned} \right. \end{equation}
\begin{equation} G(\omega)=\frac{V_A-V_B}{V_{DC}} \end{equation}
P.S. In the fig above, double slanted bar stands for parallel connection in a circuit, i.e. $R_A\mid\mid R_B=\frac{R_AR_B}{R_A+R_B}$