For $x$ close to $0$,
$$\frac{\sqrt x}{\sin (x)}=\frac{1}{\sqrt{x}}+\frac{x^{3/2}}{6}+O\left(x^{7/2}\right)$$ so no problem.
But close to $x=\pi$
$$\frac{\sqrt x}{\sin (x)}=-\frac{\sqrt{\pi }}{x-\pi }-\frac{1}{2 \sqrt{\pi }}+\frac{\left(3-4 \pi ^2\right)
}{24 \pi ^{3/2}} (x-\pi )+O\left((x-\pi )^2\right)$$ and, here, there is a major issue.
Amazingly, the problem could have been solved $\color{red}{1,400}$ years ago using
$$\sin(x) \simeq \frac{16 (\pi -x) x}{5 \pi ^2-4 (\pi -x) x}\qquad (0\leq x\leq\pi)$$ was proposed by Mahabhaskariya of Bhaskara I, a seventh-century Indian mathematician.
This would give
$$I(a)=\int_{0}^{a}\frac{\sqrt x}{\sin (x)}dx\simeq \int_{0}^{a} \frac{5 \pi ^2-4 (\pi -x) x}{16 (\pi -x) \sqrt{x}} dx$$
$$I(a)=\frac{5 \pi ^{3/2}}{8} \tanh ^{-1}\left(\frac{\sqrt{a}}{\sqrt{\pi
}}\right)-\frac{a^{3/2}}{6}$$ and, as shown below, it is a decent approximation
$$\left(
\begin{array}{ccc}
a & \text{approximation} & \text{exact} \\
0.25 & 0.98828 & 1.00209 \\
0.50 & 1.41108 & 1.42619 \\
0.75 & 1.75095 & 1.76576 \\
1.00 & 2.05704 & 2.07133 \\
1.25 & 2.35188 & 2.36586 \\
1.50 & 2.65145 & 2.66535 \\
1.75 & 2.97141 & 2.98529 \\
2.00 & 3.33164 & 3.34531 \\
2.25 & 3.76309 & 3.77615 \\
2.50 & 4.32461 & 4.33677 \\
2.75 & 5.16168 & 5.17417 \\
3.00 & 6.89988 & 6.92410
\end{array}
\right)$$