Define w = foo45 as a function of v below.
![[Graphics:../Images/index_gr_904.gif]](../Images/index_gr_904.gif)
![[Graphics:../Images/index_gr_905.gif]](../Images/index_gr_905.gif)
Then consider the inversion v=foo46 as a function of w below.
![[Graphics:../Images/index_gr_907.gif]](../Images/index_gr_907.gif)
The relations between the two sets of the coefficients are given below.
![[Graphics:../Images/index_gr_909.gif]](../Images/index_gr_909.gif)
![[Graphics:../Images/index_gr_910.gif]](../Images/index_gr_910.gif)
![[Graphics:../Images/index_gr_912.gif]](../Images/index_gr_912.gif)
The relation is actually obtained by solving the following coefficients==0.
![[Graphics:../Images/index_gr_914.gif]](../Images/index_gr_914.gif)
Checking if the relation is correct by seeing the identity.
![[Graphics:../Images/index_gr_916.gif]](../Images/index_gr_916.gif)
Consider the following
![[Graphics:../Images/index_gr_919.gif]](../Images/index_gr_919.gif)
Since func48[v] = func48[w] +
, and we can ignore the difference between func48[v] and func48[w]. So, if we redefine w = foo45+func48[v], and v=foo46-func48[w], the inversion relation still holds. We call "v" as the signed distance, and "w" as a modified signed distance characterized by the coefficients cr[r] and br[r].
Jacobian of the transformation from v to w is given below. Here D[func48[w],w] is denoted as
![[Graphics:../Images/index_gr_925.gif]](../Images/index_gr_925.gif)
![[Graphics:../Images/index_gr_927.gif]](../Images/index_gr_927.gif)
We need the log of the Jacobian for later use. logjvw=log .
![[Graphics:../Images/index_gr_930.gif]](../Images/index_gr_930.gif)
Similarly, we write func48[w] as and vinuw is v expressed by u and w.
![[Graphics:../Images/index_gr_933.gif]](../Images/index_gr_933.gif)
![[Graphics:../Images/index_gr_935.gif]](../Images/index_gr_935.gif)
![[Graphics:../Images/index_gr_937.gif]](../Images/index_gr_937.gif)