Differential equation - not sure where to start

[marka]

Homework Statement

I need to solve for the voltage across a capacitor in a resistor-capacitor charging equation (eg. http://sub.allaboutcircuits.com/images/05175.png" ), except that the resistance varies inversely with the voltage across the capacitor. With a constant R, I'm happy solving the first order differential equation, but when R(t)=1/(a+b(Vc(t))), I don't know where to start.

Homework Equations

V_{in} = V_{r} + V_{c}

V_{in} = i(t).R(t) + \frac{1}{C}\int_{0}^{t}i(\tau)d\tau

R(t) = \frac{1}{a+bV_{c}(t)}

The Attempt at a Solution

V_{in} = \frac{i(t)}{a+bV_{c}(t)} + \frac{1}{C}\int_{0}^{t}i(\tau)d\tau

V_{in} = \frac{i(t)}{a+\frac{b}{C}\int_{0}^{t}i(\tau)d\tau} + \frac{1}{C}\int_{0}^{t}i(\tau)d\tau

V_{in}.a + \frac{b.V_{in}}{C}\int_{0}^{t}i(\tau)d\tau = i(t) + (\frac{1}{C}\int_{0}^{t}i(\tau)d\tau)^{2}

(differentiate wrt t, use chain rule for the last term)

0 + \frac{b.V_{in}}{C}i(t) = \frac{di(t)}{dt} + \frac{2.i(t)}{C}\int_{0}^{t}i(\tau)d\tau)I'm a bit stuck with where to go here - I'm not sure how to get rid of the integral in the last term, or even whether I've done the right thing so far. Any hints would be greatly appreciated,

Mark

 

[Defennder]

It looks easier if you are to work in terms of q(t) instead of i(t) since you won't have to deal with the integral of i(t). If you write everything out in terms of q and throw the dq/dt to one side and everything else on the left, the DE is recognisable as a Riccati differential equation.

On the other hand you could make use of the Laplace transform to work with i(t) but the term in R(t) looks pretty complicated to transform.