Chapter 4 The Derivative

4.2 New Environment: The Bachmann–Landau Notation

4.3 One-Variable Revisionism: The Derivative Redefined

4.3.1.

Let be a linear mapping. Show that for every > 0, the behavior of on determines the behavior of everywhere.

Proof:

Given any , let and . Then , so .

So is determined by .

4.3.2.

Give a geometric interpretation of the derivative when . Give a geometric interpretation of the derivative when and .

Solution:

When , we can think that there are 2 graphs of Figure 4.4. So the derivative is 2 planes.

When and , the derivative is a line.

4.3.3.

Let (where ) have component functions , and let a be an interior point of . Let be a linear mapping with component functions . Using the componentwise nature of the condition, established in Section 4.2, prove the component-wise nature of differentiability: is differentiable at a with derivative if and only if each component is differentiable at a with derivative .

Proof:

4.3.4.

Let . Show that for all . (By the previous problem, you may work component-wise.)

Proof:

First component:

Second component:

4.3.5

Let . Show that for all . (Note that because and because the derivative of the exponential function at 0 is 1, the one-variable characterizing property says that .)

Proof:

4.3.6.

Show that if satisfies for all then is differentiable at .

Proof:

Note . We will show

So .

4.3.7

Show that the function for all is not differentiable at . (First see what and need to be.)

Proof:

First assume exists and it's .

We first check

For to be , we must have . Similarly, we must have .

So if exists, it can only be .

Then we check

This shows cannot be , then we have a contradiction.

So is not differentiable at

4.4 Basic Results and the Chain Rule

4.4.1.

Prove part (2) of Proposition 4.4.1.

Proof: See ch04 notes.

4.4.2.

Prove part (2) of Proposition 4.4.2.

Proof: See ch04 notes.

4.4.3.

Prove part (2) of Lemma 4.4.4.

Define the reciprocal function

Then the derivative of at every nonzero real number a exists and is

Proof:

Since when , .

So it's .

4.4.4

Prove the quotient rule.

Proof:

Consider

So

Then .

Note , so we have

So

4.4.5.

Let . Find for arbitrary . (Hint: is the product , where is the linear function and similarly for and .)

Solution:

4.4.6.

Define on . Find where is a point in the domain of .

Solution:

Define , then we have:

4.4.7

(A generalization of the product rule.) Recall that a function

is called bilinear if for all and all ,

(a) Show that if is bilinear then is .

Proof:

Let

Then

We can find a such that for all . We also know for all .

So we have

(b) Show that if is bilinear then is differentiable with .

Proof:

First of all, we need to show is a linear function of .

Given and

Similarly given ,

Then finally, we have

So is differentiable with .

(c) What does this exercise say about the inner product?

Solution:

Since inner product is a bilinear function, then it's differentiable at any point of .

A little comments for part (a):

It took me a long way to reach to the solution above. Initially, I was thinking to use the following way.

Assume , where and . Then I want to show , as long as I can bound , then it's done.

So my next thought is to prove is continuous.

Given and , I want to use triangle inequality. Ideally, I would like to have the following, but it's not correct.

So I stuck here. I guess I was kinda inspired by how to prove a linear map is continuous which I learned from Gemini.

4.4.8. (A bigger generalization of the product rule.)

A function

(there are copies of ) is called multilinear if for each , for all and all ,

(a) Show that if is multilinear and then for (distinct), is . (Use the previous problem.)

Proof:

Let then is a bilinear function.

Since is from the exercise 4.4.7 and since , then we can conclude is .

(b) Show that if is multilinear then is differentiable with

Proof:

The linearity of is similarly to exercise 4.4.7 (b). So we skip here.

We would like to first prove: given a multilinear function and any , for any , we can find such that if ,

We use induction on . When , assume

Then

For each we can find such that if , then . Let , then if ,

Then assume the statement is true for .

We will prove when , assume

then

Let and is a multilinear function with only parameters.

Now we can apply the induction, for each , we can find such that if , then . Let , then if ,

So in summary, we proved given a multilinear function and any , we can find , as long as , and ,

The above statement can be generalized to given a multilinear function and any , we can find , as long as , and , we have

Then note that

From the previous induction and the generalization, as long as , then items with at least 2 are , so

Another much cleaner approach suggested by Gemini is to prove this first

Assume

Then

(c) When , what does this exercise say about the determinant?

Proof:

It means the determinant is differentiable at any point .

4.5 Calculating the Derivative

4.5.1.

Explain why in the discussion beginning this section the tangent plane consists of all points where .

4.5.2

This exercise shows that all partial derivatives of a function can exist at and about a point without being continuous at the point. Define by

(a) Show that .

Proof:

Similarly .

(b) Show that and exist and are continuous at all other .

Proof:

Similarly,

It is a continuous function.

(c) Show that and are discontinuous at .

Proof:

If we approach with , then

If we approach with , then

So is not continuous at . Similarly, is not continuous at .

4.5.3

Define by

Show that exists for all but that is discontinuous at . Explain how this disproves the converse of Theorem 4.5.3.

Proof:

When ,

When ,

Consider , then .

So is not continuous at .

4.5.4.

Discuss the derivatives of the following mappings at the following points.

(a) on at generic with .

Proof:

So

(b) on at generic with .

Proof:

So

(c)

at generic and at .

Proof:

First consider .

Similarly,

So

Then note is not continuous at . If we approach with , then we get

But if we approach with , then we get

Similarly, is not continuous at .

Now, assume is differentiable at and , and we approach approach with

So if , then and if , then . This is not possible.

So does not have derivative at .

4.5.5.

For what differentiable mappings is a diagonal matrix for all ? (A diagonal matrix is a matrix whose th entries for all are .)

Solution:

It means

So the format is like

Basically, is only one-variable function and is only determined by .

4.5.6.

Show that if then , , and z satisfy the differential equation .

Solution:

Let

So

Similarly

So we have

i.e.

4.5.7.

Let . Show that .

Proof:

Let

Then

So

Therefore

4.5.8.

If , show that .

Proof:

Let

So .

So we have

So we have .

4.5.9.

The function is called homogeneous of degree if for all scalars and vectors . Letting and denote the first and second partial derivatives of , show that such satisfies the differential equation

(Hint: First differentiate the homogeneity condition with respect to , viewing and as fixed but generic; the derivative of one side will require the chain rule. Second, since the resulting condition holds for all scalars , it holds for any particular of your choosing.)

Proof:

Let

Then ,

On the other hand since , then

If we plug in both equation, then for any we get

Then that's exactly

4.5.10

Let

be a function such that for all , the integral

exists and is differentiable with respect to , its partial derivative with respect to being obtained by passing the -derivative through the -integral,

(The "!" step requires justification, but under reasonable circumstances it can be carried out.) Define a function

Thus affects in two ways: as a parameter for the integrand, and as the upper limit of integration. What is ?

Solution:

Note , now we can consider

Now we have , so

4.6 Higher-Order Derivatives

4.6.2

Suppose , as a function of and , satisfies the differential equation . Make the change of variables . What corresponding differential equation does satisfy when viewed as a function of and ? (That is, find a nontrivial relation involving at least one of and .)

Solution:

So the function is

4.6.3. (The wave equation)

(a) Let be a constant, tacitly understood to denote the speed of light. Let and denote a space variable and a time variable, and introduce variables

Show that a quantity , viewed as a function of and , satisfies the wave equation,

if and only if it satisfies the equation

Proof:

So as required.