## The Chain Rule

Since the components of the differential are given by partial derivatives, and partial derivatives (like all single-variable derivatives) are linear, it’s straightforward to see that the differential operator is linear as well. That is, if and are two functions, both of which are differentiable at a point , and and are real constants, then the linear combination is also differentiable at , and the differential is given by

There’s not usually a product for function values in , so there’s not usually any analogue of the product rule and definitely none of the quotient rule, so we can ignore those for now.

But we *do* have a higher-dimensional analogue for the chain rule. If we have a function defined on some open region and another function defined on a region that contains the image , then we can compose them to get a single function defined by . And if is differentiable at a point and is differentiable at the image point , then the composite function is differentiable at .

First of all, what should the differential be? Remember that the differential is a linear transformation that takes displacements from the point and turns them into displacements from the point . Then the differential is a linear transformation that takes displacements from the point and turns them into displacements from the point . Putting these together, we have a composite linear transformation that will start with a linear transformation that takes displacements from the point and turns them into displacements from the point . I assert that this is composite transformation is exactly the differential of the composite function.

Just as a sanity check, what happens when we look at single-variable real-valued functions? In this case, and are both linear transformations from one-dimensional spaces to other one-dimensional spaces. That is, they’re represented as matrices that just multiply by the single real entry. So the composite of the two transformations is given by the matrix whose single entry is the product of the two matrices’ single entries. In other words, in one variable the differentials looks like single real numbers and , and their composite is given by multiplication: . This is exactly the one-variable chain rule. To understand multiple variables we have to move from products of real numbers to compositions of linear transformations, which will be products of real matrices.

Okay, so let’s verify that does indeed act as a differential for . It’s clearly a linear transformation between the appropriate two spaces of displacements. What we need to verify is that it gives a good approximation. That is, for every there is a so that if we have

First of all, since is differentiable at , given there is a so that if we have

Now since is differentiable it satisfies a Lipschitz condition. We showed that this works for real-valued functions, but extending the result is very straightforward. That is, there is some radius and a constant so that if we have the inequality . That is, cannot stretch displacements by more than a factor of as long as the displacements are small enough.

Now may be smaller than already, but just in case let’s shrink it until it is. Then we know that

.

so we can use this difference as a displacement from . We find

Now we’re going to find a constant and a radius so that

whenever . Once this is established, we are done. Given an we can set and let be the smaller of the two resulting radii and . Within this smaller radius, the desired inequality will hold.

To get this result, we choose orthonormal coordinates on the space . We can then use these coordinates to write

But since each of the several is differentiable we can pick our radius so that all of the inequalities

hold for . Then we let be the magnitude of the largest of the component partial derivatives , and we’re done.

Thus when is differentiable at and is differentiable at , then the composite is differentiable at , and the differential of the composite function is given by

the composite of the differentials, considered as linear transformations.

Another crisp, fine exposition. My wife is still annoyed by a time over 20 years ago when we went to a Pasadena restaurant with a younger alumnus friend of mine, whom I’d guided into Mathematical Music Theory (where he got his double degree at UC Santa Cruz and published in IEEE and other venues later), and played in a rock band together. he had a girlfriend with him who, once she found that my wife was a professor, kept interrupting to demand an explanation of the Chain Rule. My wife has taught that, but this was a social event, not a colloquium. Where was I? Oh, right, nicely done! I still think that you should find a coauthor to make this into a textbook.

Comment by Jonathan Vos Post | October 7, 2009 |

The textbook idea has merit, but wouldn’t it have to be rather large? Also the blog format has the advantage that people can ask questions and get answers. Btw John: has anyone come thru with the syntactic reasoners article. If not, send me your email addie and I can provide.

Comment by Avery Andrews | October 8, 2009 |

Charles sent along a copy, thanks.

As for the book, I’m more inclined towards a lay-audience book, at least at first. I’ve thought about the subject, but again I need to find someone with a bit more of a background in the history and philosophy of mathematics to help keep me honest.

I’ll be more comfortable searching for someone once I get more settled in terms of an

actualjob. Unemployment isn’t conducive to the peace of mind I’d need to get that ball rolling.Comment by John Armstrong | October 8, 2009 |

Will your lay-audience book include the category theory you’ve discussed here? I think that could be one of the distinguishing features– there exist plenty of calculus and linear algebra books, but not many lay-audience books talking about category theory.

Actually, a nowhere-dense introduction to category theory by itself would, I think, make the book worthwhile.

Comment by Akhil Mathew | October 10, 2009 |

Probably not. As I’ve mentioned before, the one I’m thinking of seeks to answer the more philosophical question, “What Is A Number?”

Comment by John Armstrong | October 10, 2009 |

Well but it seems to me that categorifying the integers is part of the answer to that. & if a book is ‘nowhere dense’, it is likely to be so heavy that just looking at it will make your wrists hurt

Comment by Avery Andrews | October 11, 2009 |

I mean more like an expansion on the standard content in the first couple days of an advanced calculus class, from Peano axioms through the continuum.

Comment by John Armstrong | October 11, 2009 |

I sometime fantasize about math ebooks that would initially give you a fairly crisp statement of what is true and why, but would then expand to more discursive text when you clicked on a ‘please explain’ icon. Perhaps also some kind of rating/reward system to encourage people to try to figure out as much as possible for themselves.

Comment by Avery Andrews | October 11, 2009 |

A while ago you were nice enough to give props out to my podcast Combinations and Permutations and I am now back(I have been back a few times to read of course but this is my first comment) to let you know that I have a 2nd podcast where I am interviewing mathematicians. The first episode where I interview Gary Chartrand is now up at Strongly Connected Components. Of course I would like you to listen but much more I would love to now have you as a guest on my new podcast. If this is interesting to you please email me at sccmathpodcast@gmail.com

Comment by Combinations and Permutations | October 8, 2009 |

[...] Invariant Rule An immediate corollary of the chain rule is another piece of “syntactic [...]

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Re: philosophical question, “What Is A Number?”

Excerpt from GENE515 (by Jonathan Vos Post)

This partly answers a question asked of me when I was

21 years old, by my doctoral thesis advisor Oliver G.

Selfridge [Father of Machine Perception]. When I say “Man” I am echoing and older

text, and not excluding Woman.

Excerpt from GENE515

What is Man, that he may know Number? What is Number

that it may be known by Man?

As we are mathematicians, we are in the image of our

creator, The Mathematician, who has other attributes

beyond our comprehension, and is Transfinite.

He freely gives us this world, and the cosmos beyond,

and the flora and fauna over which to be stewards, and

our fellow human beings to love, which is in the image

of His love, which is transfinite.

We have free will, and for those of use who choose to

be mathematicians, he gives us the integers as toys,

in which is His book coded.

We play with those toys, some of us in solitude, some

of us playing together. And when we put aside childish

things, behold, we still have the gift of Number, and

they are more than first we knew.

Eureka!, and Aha!, and knowing what Mozart meant when

he said that he did not write music, but it was

already there and he plucked it from thin air as it

blew past. And what Ramanujan said was given him by a

Goddess, And what Gauss could see as a child, and

Riemann in the looking glass of Primes, and Galois by

candlelight in the brief hours before his fatal duel.

Euclid, alone, has looked on beauty bare. But we

mathematicians today are not alone, far from it,

cradled in the same Web woven of Number, binary and

octal and hex, decimal and alphanumeric, vector and

raster, and more in cables, trunks, and as wifi in the

very air about us.

By knowing Number more deeply, we more deeply know

ourselves, and our Creator.

Every word begins and ends with the empty word; the

empty word begins and ends with itself.

Comment by Jonathan Vos Post | October 10, 2009 |

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