Assume that $A=A^T$ and consider the following scalar function,
its differential, and its subsequent integral.
$$\eqalign{
\phi(x) &= \frac{1}{2}x^TAx \\
d\phi &= dx^T(Ax) \\
\int_0^a dx^T(Ax) = \int_{\phi(0)}^{\phi(a)} d\phi
&= \Big[\phi(a)-\phi(0)\Big]
= \frac{a^2}{2}\big({\tt 1}^TA{\tt 1}\big) \\
}$$
This might be the answer to your question, but only if $A$ is symmetric and if the repetition of the $i$-index was meant to imply the Einstein summation convention.
NB: The above uses $(x)$ instead of $(t)$ as the independent variable.
Update
Based on your comment, it sounds like you have the following problem in mind.
For $i=1$, write the vector as $x={\tt [}\;t\;u\;v\;\ldots\;{\tt ]}^T$ and write the integral as
$$\eqalign{
\Phi_1
&= \int_0^a dt\; e_1^TAx \cr
&= e_1^TA\;\int_0^a dt\,x \cr
&= e_1^TA\;{\tt [}\;\tfrac{1}{2}a^2\quad au\quad av\;\ldots\;{\tt ]}^T \cr
&= e_1^TA\Big(\tfrac{1}{2}a^2e_1 + a(I-e_1e_1^T)x\Big) \cr
&= \frac{a^2}{2}\big(e_1^TAe_1\big) + a(e_1^TAx) - a(e_1^TAe_1)(e_1^Tx) \cr
}$$
The calculation is the same for any other value of $i$, just replace the $e_1$ basis vectors with $e_i$.