Inactive Tutor answered 07/11/13
A differential equation with initial conditions is equivalent to a second (Volterra) type of integral equation with the variable upper limit of integration, that is
y = 2∫0t t(1+y)dt = 2∫0t tydt + t2
In order to use successive approximations you have to start with the first one (y1) which can be found by putting into the equation your zero approximation, y(0) = 0. It gives you y1 = t2.
The second approximation (y2) can be found by plugging y1 into the equation. Thus, we have
y2 = 2∫0 t ty1dt + t2 = t4/2 + t2
The same way the next (3rd) approximation
y3 = 2∫0 t ty2dt + t2 = 2∫0 t t(t4/2 + t2)dt +t2 = t6/6 + t4/2 + t2
If you continue the same way to get your next approximation you wil see this is a Tylor expansion of the function
y(t) = exp(t2) - 1
This is a solution of your equation