How rough can differential form, manifold and chain be for Stokes theorem to hold? When I first learned Stokes theorem, everything is assumed to be smooth to prevent any strange things happen. But to apply to more cases, I may need to use a version of Stokes theorem that holds for rougher forms, chains and manifolds. For instance, when I learned Cauchy integral theorem, the paths and the analytic functions are only assumed to be $C^1$.
Does Stokes theorem hold for merely $C^1$ forms, chains and manifolds? I think so because we only exterior differentiate once in the equation of Stokes theorem, and the pullback by the chain (parametrisation of surfaces) only uses the first derivative, while the continuity of first derivative is added to ensure the exterior derivative ($d\omega$) and the pullback form ($(\partial c)^*\omega$) is integrable.
Edit: I see that Stokes theorem holds for manifolds with corners. I suppose these are equivalent to piecewise smooth surfaces, lines, etc. However, it is not all of what I am asking about. I am asking whether Stokes theorem holds when the differential form, manifold and chain are simply assumed to be $C^1$.

Stokes' theorem holds for manifolds with corners. The following is Theorem $16.25$ on page $419$ in John M. Lee's book $\textit{Introduction to Smooth Manifolds}$. 
$\textbf{Theorem}$ (Theorem $16.25$, [Lee]). Let $M$ be an oriented smooth $n$-manifold with corners, and let $\omega$ be a compactly supported smooth $(n-1)$-form on $M$. Then 
$$
\int_M d\omega = \int_{\partial M}\omega. 
$$
The author proves the above theorem in the book. Furthermore, Lee also discusses and proves Stokes' theorem for surface integrals (see Theorem $16.34$ on page $427$).
$\textbf{Theorem}$ (Theorem $16.34$, [Lee]). Let $M$ be an oriented Riemannian $3$-manifold with or without boundary, and let $S$ be a compact oriented $2$-dimensional smooth submanifold with boundary in $M$. For any smooth vector field $X$ on $M$, 
$$
\int_S \langle \text{curl } X,N \rangle_g \:dA = \int_{\partial S}\langle X,T\rangle_g \: ds, 
$$
where $N$ is the smooth unit normal vector field along $S$ that determines its orientation, $ds$ is the Riemannian volume form for $\partial S$ (with respect to the metric and orientation induced from $S$), and $T$ is the unique positively oriented unit tangent vector field on $\partial S$. 
