Directional derivative

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In mathematics, the directional derivative of a multivariate differentiable function along a given vector V at a given point P intuitively represents the instantaneous rate of change of the function, moving through P, in the direction of V. It therefore generalizes the notion of a partial derivative, in which the direction is always taken parallel to one of the coordinate axes.

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[edit] Definition

The directional derivative of a scalar function f(\vec{x}) = f(x_1, x_2, \ldots, x_n) along a vector \vec{v} = (v_1, \ldots, v_n) is the function defined by the limit

D_{\vec{v}}{f}(\vec{x}) = \lim_{h \rightarrow 0}{\frac{f(\vec{x} + h\vec{v}) - f(\vec{x})}{h}}.

If the function f is differentiable at \vec{x}, then the directional derivative exists along any vector \vec{v}, and one has

D_{\vec{v}}{f}(\vec{x}) = \nabla f(\vec{x}) \cdot \vec{v}

where \nabla denotes the gradient and \cdot is the Euclidean inner product. At any point p, the directional derivative of f intuitively represents the rate of change in f along \vec{v} at the point p. Usually directions are taken to be normalized, so \vec{v} is a unit vector, although the definition above works for arbitrary (even zero) vectors.

[edit] In differential geometry

A vector field at a point p naturally gives rise to linear functionals defined on p by evaluating the directional derivative of a differentiable function f along the vector \vec{v} where \vec{v} is the vector of the tangent space at p assigned by the vector field. The value of the functional is then defined as the value of the corresponding directional derivative at p in the direction of \vec{v}.

[edit] Normal derivative

A normal derivative is a directional derivative taken in the direction normal (that is, orthogonal) to some surface in space, or more generally along a normal vector field orthogonal to some hypersurface. See for example Neumann boundary condition.

[edit] See also