We define the difference quotient of a function $f$ at $x$ in the direction $l$ as $\triangle^h_l f(x) = \frac{f(x+he_l)-f(x)}{h}$ where $e_l$ is the unit vector in the direction $l$.
The book I am reading claims the following : Let $f \in C^{1,\alpha}(\Omega)$ (a $C^1$ function also in the Hölder space, but I think all the claim is using is $C^1$). Then $\triangle^h_l f(x) = \frac{1}{h}\int_0^1{\frac{d}{dt}f(x+the_l)} = \int_0^1{D_lf(x+the_l)}$ where $D_l$ is the partial with respect to $x_l$. The first equality comes from $C^1$ is easy to see. How did they get the second equality? You need to take a limit for this, and we certainly didn't do that here. Am I missing something obvious?
(The reference being used is Gilbarg-Trudinger p. 110)