To solve in the time domain, first re-arrange equation 2 in the form
\$ \frac{di}{dt} + \frac{R}{L}\,i= \frac{V}{L} \$
This is a linear first order differential equation. This class of equations can be solved by multiplying through by an integrating factor. In this case the integrating factor is
\$ e^{\small\frac{^R}{L}\normalsize t} \$
Multiplying through we get
\$ e^{\small\frac{^R}{L}\normalsize t}\, \frac{di}{dt} + \frac{R}{L} \, e^{\small\frac{^R}{L}\normalsize t} \,i = \frac{V}{L} \, e^{\small\frac{^R}{L}\normalsize t} \$
By the product rule, the left side becomes
\$ \frac{d}{dt} \left( e^{\small\frac{^R}{L}\normalsize t}\,i \right) = \frac{V}{L}
\, e^{\small\frac{^R}{L}\normalsize t} \$
Integrate both sides with respect to t
\$ \int\frac{d}{dt}\left(e^{\small\frac{^R}{L}\normalsize t}\,i \right)\,dt = \frac{V}{L}\int e^{\small\frac{^R}{L}\normalsize t} \, dt \$
and we get
\$ e^{\small\frac{^R}{L}\normalsize t}\,i = \frac{V}{L}\,\frac{L}{R} \,e^{\small\frac{^R}{L}\normalsize t} + c\$, where c is a constant. Dividing through by \$ \,e^{\small\frac{^R}{L}\normalsize t} \$ we get
\$ i = \frac{V}{R} \, + ce^{-\small\frac{^R}{L}\normalsize t}\$
Solve for \$c\$ by setting initial conditions \$t=0\$ and \$\, i
_{(t=0)} = 0\$ to obtain
\$c = - \frac{V}{R}\$
Substitute for c to obtain the solution
\$ i = \frac{V}{R} \,\left(1 - e^{-\small\frac{^R}{L} \normalsize t} \right)\$