The role of the Jacobian in the Implicit Function Theorem

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Discussion Overview

The discussion centers on the role of the Jacobian in the Implicit Function Theorem, exploring its implications in various scenarios involving equations and variables. Participants seek to clarify the conditions under which the theorem applies, particularly regarding the squareness of the Jacobian and its significance in determining the existence of functions defined implicitly.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants express uncertainty about the necessity of the Jacobian being square, particularly in cases where the number of equations is less than the number of variables.
  • There is a discussion about whether a 1x1 Jacobian is valid and if its determinant is simply the single element, with some participants questioning the implications of having a partial derivative equal to zero.
  • One participant explains that if the Jacobian is zero, it indicates no change at that point, which affects the existence of an inverse function.
  • Another participant provides examples illustrating the dimensionality issues when applying the Implicit Function Theorem, emphasizing the importance of the determinant condition for ensuring a unique solution.
  • There is a mention of the need for both partial derivatives to be non-zero in certain contexts to invoke the theorem, while others argue that it may only require one derivative to be non-zero.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the conditions required for the Jacobian in the context of the Implicit Function Theorem. Multiple competing views remain regarding the necessity of the Jacobian being square and the implications of having zero derivatives.

Contextual Notes

Participants highlight limitations related to the dimensionality of the equations and the uniqueness of solutions, as well as the dependence on the definitions of the functions involved. The discussion remains open-ended regarding the implications of the Jacobian's properties.

Who May Find This Useful

This discussion may be useful for students and practitioners in mathematics and related fields who are exploring the Implicit Function Theorem and its applications, particularly those grappling with the role of the Jacobian in various contexts.

Fractal20
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I am trying to understand the role of the Jacobian in the Implicit Function Theorem. However, I have had a hard time finding any discussions that use the Jacobian and are accessible for my level. http://mathworld.wolfram.com/ImplicitFunctionTheorem.html has been the best thing I have found.

More specifically I am unsure about maintaining that the Jacobian be square. So for the theorem to apply book is it true that given m equations with n variables (m < n) the number of dependent variables needs to be equal to the number of equations? If so, then I think I see why the Jacobian will be square (maybe it shows my ignorance to even suggest that something not square could be Jacobian?).

Also, in the case of something like f(x,y) = 0 and we are interested in finding y as a function of x, does the Jacobian still play a role? I want to say the Jacobian is a 1x1: [itex]\frac{\deltad}{\deltay}[/itex]. Is it okay to have 1x1 Jacobians and is the determinant of a 1x1 matrix simply the single element? Furthermore, if in such a case the partial deriv with respect to x is 0, does the theorem still apply? Or does it just mean dy/dx = 0?

Hopefully this wasn't too rambling and unspecific. Any insight would be appreciated! Thanks!
 
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Hey Fractal20.

The Jacobian is basically a way of quantifying the volumetric change at a particular point for a n-dimensional mapping to an n-dimensional mapping.

If the Jacobian is zero, it means that there is no change whatsoever, and this means you get an overall change of zero at that point (with respect to the rate of change with respect to the expansion and contraction with respect to the entire volume).

Since you have no-expansion or contraction at that point it means that you won't get an inverse because an inverse function requires that you are able to use the rate of change of the function to get the rate of change of the inverse.

As a really brief example, consider y = 2 for all x on the real line. dy/dx = 0. Now you can't get an inverse in this instance because there is no dependency between y and x and for an inverse you need a dependency at the minimum before you can even think about getting an inverse.

The other to think about the inverse function is to think about branch cuts when you get turning points. Take for example f(x) = sin(x). You get a max at pi/2 and a minimum at -pi/2 (and all additions of n*pi). So in this case you get a principal branch of -pi/2 to pi/2. But for an inverse function to exist it must be a 1-1 mapping which means you have to look at the parts in-between the points when the derivative is 0.

This isn't a formal argument but it should give some intuition behind the justification of the inverse function theorem.

As for the Jacobian being square, you have to be aware that a transformation must go from one dimension to the same dimension and this ends up in a square matrix.

If you went from a higher dimension to a lower one you would be losing information and it would be not a substitution but a projection and a substitution that preserves the equivalence of the representation preserves the dimension and in terms of a transformation (at least a linear one) this means the matrix is a square one.
 
Great, that clears up things about the squareness. About that bit towards the end of my original post. Are there 1x1 Jacobians, or does that not really apply? Maybe it is translating area to area or just length to length. And lastly, again in the case of a situation like g(x,y) = 0. Do both gx and gy need to not be equal to 0 in order to invoke the implicit function theorem, or is it just that in order to write a variable (let's say u) as a function of another (v) then the derivative g with respect to u must not be 0?
 
Fractal20 said:
I am trying to understand the role of the Jacobian in the Implicit Function Theorem. However, I have had a hard time finding any discussions that use the Jacobian and are accessible for my level. http://mathworld.wolfram.com/ImplicitFunctionTheorem.html has been the best thing I have found.

More specifically I am unsure about maintaining that the Jacobian be square. So for the theorem to apply book is it true that given m equations with n variables (m < n) the number of dependent variables needs to be equal to the number of equations? If so, then I think I see why the Jacobian will be square (maybe it shows my ignorance to even suggest that something not square could be Jacobian?).

If you got too few equations, then you might not have a unique solution.

The goal of the implicit function theorem is to come up with a function [itex]g:\mathbb{R}^n\rightarrow \mathbb{R}^k[/itex]. For example, let's take n=1 and k=2.
Now, the implicit function theorem will come up with a function [itex]g:\mathbb{R}\rightarrow \mathbb{R}^2[/itex] that satisfies some equation f(x,g(x))=0. Now, let's say that [itex]f:\mathbb{R}\times \mathbb{R}^2\rightarrow \mathbb{R}[/itex]. Then the level set f(x,y,z)=0 will have "dimension 2". For example, given [itex]f(x,y,z)=x^2+y^2+z^2-1[/itex], then we have the level set [itex]x^2+y^2+z^2=1[/itex].

Given an element (a,b,c) on the level set, we wish to find [itex]g:U\rightarrow V[/itex] such that g(a)=(b,c) and such that [itex]f(x,g(x))=0[/itex] for all x. But we see that [itex]x^2+y^2+z^2=1[/itex] is the entire sphere. If we want a function such that (for example) g(0)=(0,1), then there are multiple ways to do so. For example, we can pick [itex]g(x)=(0,\sqrt{1-x^2})[/itex], or we can pick [itex]g(x)=(x,\sqrt{1-2x^2})[/itex]. There are an infinite number of g that we can pick under our conditions.

Likewise, if we take the equation [itex]f(x,y,z)=y[/itex], then we will have the level set y=0. If we want g(0)=(0,1), then there are again multiple g that satisfy our equations. For example, everything of the form [itex]g(x)=(0,h(x))[/itex] for [itex]h:\mathbb{R}\rightarrow \mathbb{R}[/itex].

In our first case, we wanted a function from [itex]\mathbb{R}[/itex] to the sphere. This was impossible to do uniquely because the sphere has dimension 2, while the line has dimension 1. In the second case, we want a function from [itex]\mathbb{R}[/itex] to a plane. This is impossible to do uniquely because the plane again has dimension 2, while the line has dimension 1.

Now, what if we intersect our plane and our sphere?? This wil give something of dimension 1. So can we demand a function from [itex]\mathbb{R}[/itex] to the intersection of our plane and our sphere? This comes down to take a function [itex]f:\mathbb{R}\times\mathbb{R}^2\rightarrow \mathbb{R}^2[/itex]. Indeed, we want the function [itex]f(x,y,z)=(x^2+y^2+z^2-1,y)[/itex]. If we want a function now that satisfies g(0)=(0,1), then this is possible to do in a unique way: [itex]g(x)=(0,\sqrt{1-x^2})[/itex].

Now, what if we wanted to be malicious and intersect our sphere with the same sphere. Then we end up with something of dimension 2, which is too large. So the implicit function theorem should break down. So, take [itex]f(x,y,z)=(x^2+y^2+z^2-1,x^2+y^2+z^2-1)[/itex]. It can now be checked that the determinant of our Jacobian is zero, so indeed, the implicit function theorem is not applicable. So, the determinant condition is partly there to ensure us that our dimension is sufficiently reduced.

Also, in the case of something like f(x,y) = 0 and we are interested in finding y as a function of x, does the Jacobian still play a role? I want to say the Jacobian is a 1x1: [itex]\frac{\deltad}{\deltay}[/itex]. Is it okay to have 1x1 Jacobians and is the determinant of a 1x1 matrix simply the single element? Furthermore, if in such a case the partial deriv with respect to x is 0, does the theorem still apply? Or does it just mean dy/dx = 0?

Such a thing can again be solved by the implicit function theorem. For example, given [itex]f:\mathbb{R}\times \mathbb{R}\rightarrow \mathbb{R}:(x,y)\rightarrow x^2+y^2-1[/itex]. Let's say we want a function g(y)=x. The implicit function theorem does not apply directly, but we can make it apply by introducing a function [itex]f:\mathbb{R}\times \mathbb{R}\rightarrow \mathbb{R}:(x,y)\rightarrow f(y,x)[/itex]. The implicit function theorem appied to this, will yield a function such that [itex]f^\prime(x,g(x))=0[/itex]. This is of course the same as [itex]f(g(x),x)[/itex]. So we have found a function going from the second variable to the first.
Of course, the condition for such a function to exist, is now of course that [itex]\frac{\partial f^\prime}{\partial y}\neq 0[/itex]. This is the same as asking that [itex]\frac{\partial f}{\partial x}\neq 0[/itex].
 
Fractal20 said:
Great, that clears up things about the squareness. About that bit towards the end of my original post. Are there 1x1 Jacobians, or does that not really apply? Maybe it is translating area to area or just length to length. And lastly, again in the case of a situation like g(x,y) = 0. Do both gx and gy need to not be equal to 0 in order to invoke the implicit function theorem, or is it just that in order to write a variable (let's say u) as a function of another (v) then the derivative g with respect to u must not be 0?

A 1x1 Jacobian is basically dy/dx or whatever your dependent/independent variables are.

The other thing that will help you is to think of what the Jacobian matrix (not just the determinant) actually is with respect to the derivatives.

Once you have done that, think about what the inverse matrix (i.e. the matrix above but inverted) represents.

This generalization is made very clear in the theory of tensors where you deal with arbitrary co-ordinate systems and you want to go from one system to another and back again. If you can only go one way then it's really pointless when you need to go back.

Then take this all together and consider the transformations as 'co-ordinate systems' in the tensor way and it should start to make a lot more sense.
 

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