Differentiability is the existence of a derivative at a point. For maps between finite-dimensional normed vector spaces, the existence of a Fréchet derivative requires a single linear map approximating the increment with error . Merely having partial derivatives need not provide this approximation; continuous partial derivatives on a neighbourhood do suffice.
Set . The difference quotient has Euclidean norm , so . For , differentiation gives . Thus this differentiable curve has a derivative discontinuous at zero, despite each scalar component satisfying the usual one-dimensional derivative properties.
The function for , extended by , is differentiable everywhere. At zero its derivative is zero by the difference quotient, while away from zero is unbounded near zero. Differentiability of a function is therefore weaker than continuity of its derivative.
If all partial derivatives exist near a point and are continuous there, successive coordinate increments and the one-variable mean value theorem express as with . Subtracting the displayed linear map leaves , proving Fréchet differentiability. In two dimensions the absolute remainder is at most for small enough increments.
At a point with , factor the difference of squares and divide by to show that differentiability of is equivalent to that of . At a zero of , its square has a local minimum; if differentiable, its derivative must vanish. The difference quotient then vanishes exactly when , equivalently . For example, with is not differentiable at zero, but its square is.
For , differentiability at means that the difference quotient has a finite two-sided limit of a function. For , require derivatives through order throughout some open neighbourhood of , and require the final difference quotient
to exist as a finite real number. The last derivative need not exist elsewhere or be continuous at . In particular, existence of by itself does not justify taking a second derivative: the function must first be defined in a neighbourhood of .

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