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We define differentiability in two dimensions as follows. A function of two variables is differentiable at argument if the surface it defines in space looks like a plane for arguments near .
(Given any positive numerical criterion, there is a circle around within which its graph differs from the plane by less than that criterion.)
Recall that a plane in variables and is defined by a linear equation that can be put in the form
(A)
The plane that resembles here is called the tangent plane to at and the function it represents is called the linear approximation to defined at .
The quantities and are called the partial derivatives of with respect to and with respect to , and written as follows
Here is the directional derivative of in the direction of the axis, , while is the directional derivative of in the direction of the axis, .
The linear approximation to at arguments and which describes the tangent plane to at therefore takes the form
where the vector , called the gradient vector to at , is the vector whose components are the partial derivatives of in the and directions at the point
We generally do not write out the cumbersome subscripts that indicate the point at which the gradient and linear approximation are defined, because they are so cumbersome, and simply write
Notice that we can write as or with the symbol , called "del" representing the combination: .
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