Here is a portion of the text that the original poster wants us to go find:
The load current for mode 1 can be found from
. . . . .\(\displaystyle V_s\, =\, Ri_1\, +\, L\dfrac{di_1}{dt}\, +\, E\)
which with the initial load current i1 (t = 0) = I1 gives the load current as
. . . . .\(\displaystyle i_1\, =\, I_1 e^{\left(-tR\,/\,L\right)}\, +\, \dfrac{V_s\, -\, E}{R}\, \left(1\, -\, e^{\left(-tR\,/\,L\right)}\right)\)
The poster's work is displayed in a small fuzzy graphic. I think the poster's steps are as follows:
\(\displaystyle V_s\, =\, R_{i_1}\, +\, L\, \dfrac{di_1}{dt}\, +\, E\)
In laplace
\(\displaystyle V_s\, =\, RI(S)\, +\, E\, + \, L\left[SI(S)\, -\, I_1\right]\)
\(\displaystyle V_s\, =\, RI(S)\, +\, LSI(S)\, +\, E\, -\, -\, LI_1\)
\(\displaystyle I(S)\left[R\, +\, LS\right]\, =\, V_S\, -\, E\, +\, LI_1\)
\(\displaystyle LIS\, \left[S\, +\, \dfrac{R}{L}\right]\)
\(\displaystyle LIS\, =\, \dfrac{V_S\, -\, E}{\left(S\, +\, \dfrac{R}{L}\right)}\, +\, \dfrac{LI_1}{\left(S\, +\, \dfrac{R}{L}\right)}\)
\(\displaystyle I(S)\, =\, \dfrac{V_S\, -\, E}{L \left(S\, +\, \dfrac{R}{L}\right)}\, +\, \dfrac{LI_1}{L \left(S\, +\, \dfrac{R}{L}\right)}\)
\(\displaystyle i(t)\, =\, \left(\dfrac{V_S\, -\, E}{L}\right)\, e^{(-R/L)t}\)