As it is not clear whether to have the larger or small $\gamma$ expansion of the integral $I(\gamma)= \int^{\pi}_0\frac{\gamma^{10} \theta^2 \sin\theta}{(\gamma^2 \theta^2 + 1)^5} d\theta,$ I will provide both.
For large $\gamma$, we observe that the integral is dominated for $\theta \approx \gamma^{-1}$. That is why can hope that we can expand the $\sin$ function. We will show later that this is really admissible when we see that successive terms are smaller when $\gamma\to\infty$ (the expansion will be an asymptotic expansion). The substitution $x= \gamma\theta$ yields $I(\gamma) = \gamma^{7} \int_0^{\pi \gamma} \frac{x^2 \sin(x/\gamma)}{(1+x^2)^5} dx \sim \gamma^{6} \int_0^\infty \frac{x^3}{(1+x^2)^5} dx + O(\gamma^5).$ Here, we have used that every term in the expansion of $\sin$ gives an additional $\gamma^{-1}$ and that the integral is dominated for $x\approx 1$ such that we could put the integration boundary to $\infty$. The remaining integral is a number which can be evaluated to $1/24$. In total we have $I(\gamma) \sim \frac{\gamma^6}{24}.$
For small $\gamma$, we can obtain a converging series by expanding the integrand in a Taylor series. The first term in the expansion reads $I(\gamma) = \gamma^{10} \int_0^\pi \theta^2 \sin \theta d\theta + O(\gamma^{11}) = (\pi^2 -4) \gamma^{10} + O(\gamma^{11}).$
Knowing the two asymptotics, we (more or less) can draw a plot of the function. It starts off as $(\pi^2 -4) \gamma^{10}$ and then turns over into $\gamma^6/24$. The crossover region is for $\gamma \approx 1$. In this spirit, I expect $I(\gamma) \approx \frac{\gamma^{10}}{(\pi^2-4)^{-1} + 24 \gamma^4}$ to be a reasonable good approximation to the initial integral.