Hint. Assume $u(\cdot)$ is continuous over $[0,\infty)$. Then one may differentiate the initial equation twice, using the Leibniz integral rule getting
$$
u''(t)+u(t)=\frac{5}4t, \quad t\geqslant 0,
$$
which can be classically solved using $u(0)=0$ and $u'(0)=\dfrac54$.
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Through Laplace transform the integral equation becomes
$$
4U(s)+\frac{1}{s^2+1}U(s)=\frac{5}{s^2}
$$
that is
$$
U(s)=\frac{5}{s^2}\frac{s^2+1}{4s^2+5}=\frac{1}{s^2}+\frac{1}{4s^2+5}
$$
and then $$
u(t)=t+\frac{1}{2\sqrt{5}}\sin\left(\frac{\sqrt{5}}{2}\;t\right)\qquad t\ge 0
$$
Hint. Assume $u(\cdot)$ is continuous over $[0,\infty)$. Then one may differentiate the initial equation twice, using the Leibniz integral rule getting
which can be classically solved using $u(0)=0$ and $u'(0)=\dfrac54$.