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.