It's easily to show gauge-integrability using one math trick.
All the folowing will be done in assumption that gauge-integral is Henstock-Kurzweil integral. (H.-K. integral).
We know that if $f$ and $g$ are H.-K. integrable then $f+g$ also H.-K. integrable.
So, let's rewrite your function as
$$
\sin(x) + (x-\sin(x))1_{[0,1]\cap\mathbb{Q}}
$$
First part, $f = \sin(x)$ is Riemann integrable (and consequently H.-K. integrable with gauge $\delta_1(x)$ equals some constant value, depending on $\varepsilon$).
Second part, $g = (x-sin(x))1_{[0,1]\cap\mathbb{Q}}$ is H.-K. integrable with gauge $$\delta_2(x) = \bigg(\frac{\varepsilon}{2^{k+1}}\bigg)1_{[0,1]\cap\mathbb{Q}} + 1_{[0,1]\setminus\mathbb{Q}}$$
where $k$ means number of rational number.
For any $\tau=\{\xi_i,\Delta_i\}_{i=1}^n$ - $\delta_2$-partition of $[0,1]$ sum $$\bigg|\sum_{i=1}^n g(\xi_i)|\Delta_i|\bigg| \leq \sum_{k=1}^\infty g(r_k)2\delta(r_k) < \sum_{k=1}^\infty \frac{2\varepsilon}{2^{k+1}} = \varepsilon$$
where $r_k$ means $k$-th rational number. That's why $\int_{[0,1]}g(x)dx = 0$
So, your function is integrable as sum of integrable functions. If you want an explicit formula for gauge, you can try to construct it from $\delta_1$ and $\delta_2$.