The given expression describes a piecewise function of voltage u(t) across a circuit element with respect to time and is defined over four intervals:
$$ u(t)= \begin{cases} V_{0} \frac{t}{(2T)} &\text{for \(0 \leq t \leq 2T)\)}\\ V_{0} &\text{for \(2T \leq t \leq 3T)\)}\\ -V_{0} &\text{for \(3T \leq t \leq 4T)\)}\\ \frac{V_{0}}{2}(\frac{t}{T}-6) &\text{for \(4T \leq t \leq 8T)\)} \end{cases} $$
for $$0 < t \leq 2T$$
The expression $$i(t)=i(0)+\frac{1}{L} \int_{0}^{t} V_{0}\frac{t}{2T}dt$$ is a relationship between the current i(t) and the voltage V_0 over time for an inductor with inductance L.
Doing the math (if I am correct) I take:
\begin{align*} \frac{1}{L} &* \int_{0}^{t} V_{0}\frac{t}{2T}dt\\ &=\frac{V_{0}}{L} \int_{0}^{t} \frac{t}{2T}dt\\ &=\frac{V_{0}}{L}\dfrac{t^2}{4T}\\ &=\frac{V_{0}}{L}(\dfrac{t}{2T})^2 \end{align*}
the book that I am reading gives the result $$i(t) =\frac{V_{0}T}{L}(\dfrac{t}{2T})^2 $$.
2 questions :
1) First of all the i(0) = ?
2) where the T in the numerator came from in the resulted expression ?