RC oscillator and active bandpass Opamp filter
Hari - here is a much simpler method for deriving the bandpass transfer function:

Without R1 and C the rest of the circuit (at node 1) is nothing else that the classical active inductor circuit based on an GIC block (Generalized Impedance Converter). It is easy to show that the inductive input impedance (node 1) is Zi=sCR²=sL with L=R²C.

Hence, together with the parallel capacitor C you can treat the whole circuit as an ideal tank circuit (L||C) with an input impedance Zt=sL/(1+s²LC). Now, the tank circuit forms - together with R1 - a dynamic voltage divider with a bandpass response (at node 1):

H(s)=Zt/(Zt+R1)=....=sL/[R1(1+s²LC)+sL].  

Introducing the given expression for L you arrive at the desired transfer function (at node 1). More than that, it is easy to show that - for ideal opamps - the output voltage at the opamp outputs is twice the voltage at node 1 (for equal resistors R within the GIC block). Thus, the task for deriving the filters transfer function is solved.

The circuit can be transferred to an oscillator by closing the loop using another resistor R between opamp output and filter input (resp the finite filter input resistance, which is identical to R1 at the oscillation frequency). 

Hence, we have a voltage division ratio (at w=wo): R1/(R1+R).  This ratio must be chosen to be slightly larger than "1/2". In this case (because of the filter gain of "2") we have a loop gain slightly larger than unity at w=wo (safe start of oscillation). For rising amplitudes the diodes will reduce the loop gain to unity - thereby fulfilling the condition for steady-state oscillations.