Directional Derivate for sums

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I know the directional derivative as $D_uf(x)=\nabla f(x) . u$

But I do not know how this applies here?

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Notice that because the vector $\mathbf{u} = e_2$ is equal to one of the basis vectors this reduces quite nicely. The directional derivative $D_\mathbf{u}$ becomes just $\frac{\partial}{\partial x_2}$ giving

$$\frac{\partial f}{\partial x_2} = x_2 + a_2$$

because any terms involving $x_{i\neq2}$ disappear with the differentiation.