Let $f,f'$ be $L^1$ and $$\hat{f}(\xi) = \int_{-\infty}^\infty f(x)e^{-2i \pi \xi x}dx$$ For any $L$ let $$F_L(x)=\sum_n f(x+nL)$$
Then $F_L$ is $L$-periodic and $F_L,F_L'$ are integrable on one period and we have the uniformly convergent Fourier series $$F_L(x)= \sum_k \frac{1}{L}\hat{F}_L(k) e^{2i \pi xk/L}=\sum_k \frac{1}{L}\hat{f}(k/L) e^{2i \pi xk/L}$$
Locally uniformly $$f(x)=\lim_{L \to \infty}F_L(x)$$
And $$f(x)=\lim_{L \to \infty}F_L(x) = \lim_{L \to \infty}\sum_k \frac{1}{L}\hat{f}(k/L) e^{2i \pi xk/L} = \int_{-\infty}^\infty \hat{f}(\xi) e^{2i \pi \xi x}d\xi$$
where the series and the integral converge absolutely.
For the sine transform it is the same starting with $f$ odd, so that grouping the positive and negative frequencies together give series in $\sin$.