I wan to solve the following ODE's:- $$L_1 q''(t)+R_1q'(t)+\frac 1C_1 q(t)-Mq_2''(t)=V\sin(\omega t)$$ $$L_2 q_2''(t)+R_2q_2'(t)+\frac 1C_2 q_2(t)-Mq''(t)=V\sin(\omega t)$$ $L,C,R,V>0$, I already know how to solve linear non-homogenous and non-coupled ODE, using the homogenous solution plus the particular solution found by using a trial function.
How can I reduce the given equations to non=coupled form so as to apply similar methodologies to solve them?
I just know the basic methods to solve simple ODE's.
I am comfortable with solving simple coupled ODE such as
$$y_1'(t)=Ay_2(t)\text{ and } y_2'(t)=B+Cy_1(t)$$
by simple substitution.
(The physics tag is added because these equations describe the behaviour of coupled RLC circuit with an application in metal detectors)
From the first equation, we get $$q_2''=Aq''+Bq'+Cq+D\sin(\omega t)\tag1$$ for some constants $A,B,C,D$. Then also $$q_2'''=Aq'''+Bq''+Cq'+D\omega\cos(\omega t)\tag2$$ and $$q_2''''=Aq''''+Bq'''+Cq''-D\omega^2\sin(\omega t)\tag3$$
Differentiating the second equation twice gives $$Eq_2''''+Fq_2'''+Gq_2''+Hq''''=I\omega^2\sin(\omega t)\tag4$$ for some constants $E,F,G,H,I$. Now replace $q_2''$, $q_2'''$, and $q_2''''$ in (4) by using (1), (2), and (3), respectively, and voila! equations uncoupled.