Richard P. answered 03/30/20
PhD in Physics with 10+ years tutoring experience in STEM subjects
This problem is strongly analogous to the damped harmonic oscillator. The correspondences are
m → 1/C
b → R
m → L
Since R2 >> L/C for this case, the circuit is strongly over damped. That is to say, the inductor plays only a tiny role.
There will be one very short time constant and one which is (to a very good approximation) the usual RC time constant . For this case RC = .36 s.
Assuming that, in the charging the capacitor to 10 V in 2 seconds, no high frequency source was used, and the capacitor charged up slowly with the .36 s time constant. , the relevant equations are those of the RC type circuit.
V(3) / V(2) = V(3)/10 = ( 1- exp(-3/.36) ) /( 1 -exp(-2/.36) )
which works out to v(3) = 10.0364 V