The frozen function get's it's name because it can be thought of by taking the sample point and then freezing in all directions except for along the -th component of the input for
we will show that , we know that and thus it is a constant funtion, this implies tha directional derivative is 0
Therefore we can se that
Thus is not a number in general. It is a linear map that takes a small displacement and returns the best linear approximation to the change .
- If is constant, then .
- If is linear, then .
- If , then is differentiable at if and only if each component is differentiable at , and .
- If are differentiable at , then .
- If are differentiable at , then .
- If , then
First suppose is continuously differentiable on . Then is differentiable at every , so exists. The -th partial derivative of the -th component function is the -entry of the Jacobian matrix: Since the matrix-valued function is continuous, each entry function is continuous. Thus all partial derivatives exist and are continuous on .
Conversely, suppose all partial derivatives exist and are continuous on . Fix . Since is open, choose a small rectangle around contained in . Define a linear transformation by We show that is the derivative of at .
Write , and for , set For each component , telescope the change from to : Each summand changes only the -th coordinate. By the one-variable mean value theorem applied along that coordinate segment, if , there is a point on the segment from to such that If , the same formula holds with any point on the segment.
Therefore Since each is continuous at , the differences go to as . Hence By the definition of differentiability, is differentiable at , with .
Since was arbitrary, is differentiable on . The matrix of is exactly so The entries of this matrix are continuous functions of , so the Jacobian matrix varies continuously on . Thus is continuously differentiable on .
By the Jacobian entries are partial derivatives corollary, the Jacobian matrix of at , with input coordinates ordered as , is
Applying this matrix to the displacement givesIn the normalized case, continuity of the Jacobian matrix gives a closed rectangle with in its interior such that stays close to on . Applying the mean value inequality to , after shrinking if needed, gives for all . Therefore so is one-to-one on .
The boundary of is compact, and is not in the image of that boundary. Hence there is an open ball around such that every is closer to than to any value with on the boundary of .
Fix , and define on . Since is a compact closed rectangle and is continuous, the extreme value theorem gives a point where is minimized. The choice of prevents this minimum from occurring on the boundary, so the minimum occurs at an interior point .
By the interior extremum theorem, all partial derivatives of vanish at . Written in matrix form, this says Since is close to , it is invertible. Therefore , so . This proves that every has a preimage in the interior of . Together with injectivity, this gives a local inverse , where .
The estimate implies so is continuous.
Let . Since is differentiable at , Using the continuity estimate for , this remainder identity implies Since the Jacobian matrix of is continuous and matrix inversion is continuous on invertible matrices, is continuously differentiable. If is , repeated differentiation of shows inductively that is .
The derivative matrix of at , written in the -variables followed by the -variables, has block form where is the matrix of partial derivatives of with respect to the -variables. This block matrix is invertible, with inverse Indeed, by block matrix multiplication, and the product in the opposite order is also the identity matrix.
By the inverse function theorem, after restricting to open neighborhoods, has a continuously differentiable inverse. Write this inverse as The first component must be , because the first component of is .
Define Then so .
Conversely, if for in the chosen neighborhood, then Since is one-to-one on that neighborhood, . Hence , proving uniqueness.
Since is obtained from the continuously differentiable inverse , it is continuously differentiable. If is , then is , so is by the smooth part of the inverse function theorem. Therefore is .