Differentialbility & Continuity of Multivariable Functions

In summary: Duistermaat and Kolk's Multidimensional Real Analysis I: Differentiation begins by stating that he is reading the book and is focusing on Chapter 2: Differentiation. He needs help with an aspect of the proof of Lemma 2.2.7 and asks Fresh_42 for help. Fresh_42 follows Peter's advice and things fall into place. Lastly, Peter thanks Fresh_42 and ends his summary.
  • #1
Math Amateur
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I am reading "Multidimensional Real Analysis I: Differentiation" by J. J. Duistermaat and J. A. C. Kolk ...

I am focused on Chapter 2: Differentiation ... ...

I need help with an aspect of the proof of Lemma 2.2.7 (Hadamard...) ... ...

Duistermaat and Kolk's Lemma 2.2.7 and its proof read as follows:
D&K - 1 -  Lemma 2.2.7 ... ... PART 1 ... .png

D&K - 2 -  Lemma 2.2.7 ... ... PART 2 ... .png

In the above proof we read the following:

" ... ... Or, in other words since ##(x - a)^t y = \langle x - a , y \rangle \in \mathbb{R}## for ##y \in \mathbb{R}^n##,##\phi_a(x) y = Df(a)y + \frac{ \langle x - a , y \rangle }{ \| x - a \|^2 } \epsilon_a ( x _ a ) \in \mathbb{R}^p \ \ \ (x \in U \setminus \{ a \} , y \in \mathbb{R}^n )##.

Now indeed we have ##f(x) = f(a) + \phi_a(x ) ( x - a )##. ... ... "
My question is as follows:How/why does ##\phi_a(x) y = Df(a)y + \frac{ \langle x - a , y \rangle }{ \| x - a \|^2 } \epsilon_a ( x _ a ) \in \mathbb{R}^p##

... imply that ...

##f(x) = f(a) + \phi_a(x )( x - a )## ... ... ... ?
Help will be much appreciated ...

Peter==========================================================================================

NOTE:

The start of D&K's section on differentiable mappings may help readers of the above post understand the context and notation of the post ... so I am providing the same as follows:
D&K - 2 -  Lemma 2.2.7 ... ... PART 2 ... .png

D&K - 2 - Start of Section 2.2 on Differentiable Mappings ... PART 2 ... .png

The start of D&K's section on linear mappings may also help readers of the above post understand the context and notation of the post ... so I am providing the same as follows:
D&K - 1 -  Linear Mappings ... Start of Section - PART 1.png

D&K - 2 -  Linear Mappings ... Start of Section - PART 2 ... ... .png

D&K - 3 -  Linear Mappings ... Start of Section - PART 3 ... ... .png
 

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  • D&K - 1 -  Lemma 2.2.7 ... ... PART 1 ... .png
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  • D&K - 2 -  Lemma 2.2.7 ... ... PART 2 ... .png
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  • D&K - 1 - Start of Section 2.2 on Differentiable Mappings ... PART 1 ... .png
    D&K - 1 - Start of Section 2.2 on Differentiable Mappings ... PART 1 ... .png
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  • D&K - 2 - Start of Section 2.2 on Differentiable Mappings ... PART 2 ... .png
    D&K - 2 - Start of Section 2.2 on Differentiable Mappings ... PART 2 ... .png
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  • D&K - 1 -  Linear Mappings ... Start of Section - PART 1.png
    D&K - 1 - Linear Mappings ... Start of Section - PART 1.png
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  • D&K - 2 -  Linear Mappings ... Start of Section - PART 2 ... ... .png
    D&K - 2 - Linear Mappings ... Start of Section - PART 2 ... ... .png
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  • D&K - 3 -  Linear Mappings ... Start of Section - PART 3 ... ... .png
    D&K - 3 - Linear Mappings ... Start of Section - PART 3 ... ... .png
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  • #2
Math Amateur said:
My question is as follows:

How/why does ##\phi_a(x) y = Df(a)y + \frac{ \langle x - a , y \rangle }{ \| x - a \|^2 } \epsilon_a ( x _ a ) \in \mathbb{R}^p\quad (1)##

... imply that ...

##f(x) = f(a) + \phi_a(x )( x - a )\quad (2)## ... ... ... ?
Substitute ##(x-a)## for ##y## in (1) and simplify, noting that ##\langle v,v\rangle = \|v\|^2##. Then make ##Df(a)(x-a)## the subject of that equation on the LHS. Insert the RHS of that equation into 2.10, replacing ##h## by ##(x-a)##, do a bit of simplification and voilà!
 
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  • #3
andrewkirk said:
Substitute ##(x-a)## for ##y## in (1) and simplify, noting that ##\langle v,v\rangle = \|v\|^2##. Then make ##Df(a)(x-a)## the subject of that equation on the LHS. Insert the RHS of that equation into 2.10, replacing ##h## by ##(x-a)##, do a bit of simplification and voilà!
Thanks Andrew ...

Followed your advice and things fell into place as you indicated!

Thanks again,

Peter
 
  • #4
andrewkirk said:
Substitute ##(x-a)## for ##y## in (1) and simplify, noting that ##\langle v,v\rangle = \|v\|^2##. Then make ##Df(a)(x-a)## the subject of that equation on the LHS. Insert the RHS of that equation into 2.10, replacing ##h## by ##(x-a)##, do a bit of simplification and voilà!
Thanks again Andrew ...

BUT ... just a comment on D&K's proof ...

I have to say that D&K's proof of Hadamard's Lemma though valid, is not very intuitive, starting as it does with a fairly complicated definition of ##\phi_a(x)## ... ...

Do you have any comments ... ?

Peter
 
  • #5
Math Amateur said:
Thanks again Andrew ...

BUT ... just a comment on D&K's proof ...

I have to say that D&K's proof of Hadamard's Lemma though valid, is not very intuitive, starting as it does with a fairly complicated definition of ##\phi_a(x)## ... ...

Do you have any comments ... ?

Peter
It's not that much lacking intuition. At ##x=a## we already have the differential as operator valued function: ##a \mapsto D_a##. So what's left is a linear function for the entire neighborhood ##U## of ##x=a##. This must be done continuously, so we have to approach ##D_a##. ##(x-a)(x-a)^t## supplies the required linear function (a matrix), ##||x-a||^2## in the denominator norms it, so that it cannot "run away", and the ##\varepsilon_a## from the definition and precondition of differentialbility guarantees, that the additional term vanishes the closer we get to ##x=a##. Thus the lack of intuition is more a lack of practice and experience, which the author probably doesn't lack of.
 
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  • #6
fresh_42 said:
It's not that much lacking intuition. At ##x=a## we already have the differential as operator valued function: ##a \mapsto D_a##. So what's left is a linear function for the entire neighborhood ##U## of ##x=a##. This must be done continuously, so we have to approach ##D_a##. ##(x-a)(x-a)^t## supplies the required linear function (a matrix), ##||x-a||^2## in the denominator norms it, so that it cannot "run away", and the ##\varepsilon_a## from the definition and precondition of differentialbility guarantees, that the additional term vanishes the closer we get to ##x=a##. Thus the lack of intuition is more a lack of practice and experience, which the author probably doesn't lack of.
Thanks fresh_42 ...

Now reflecting on what you have written ...

Peter
 

Related to Differentialbility & Continuity of Multivariable Functions

What is the definition of differentialbility for multivariable functions?

Differentialbility for multivariable functions refers to the ability of a function to be approximated by a linear function at a specific point. This is similar to the concept of differentiability for single variable functions, but it takes into account multiple variables.

How is the differentiability of a multivariable function determined?

The differentiability of a multivariable function can be determined by calculating the partial derivatives of the function with respect to each variable and checking if they exist and are continuous at a specific point.

What is the significance of continuity in multivariable functions?

Continuity is important in multivariable functions because it ensures that the function is well-behaved and has no sudden jumps or breaks. It also guarantees that the function can be differentiated and integrated, which is necessary for many applications in physics, engineering, and other scientific fields.

Can a multivariable function be differentiable but not continuous?

No, a multivariable function cannot be differentiable if it is not continuous. This is because differentiability requires the existence and continuity of partial derivatives, which in turn requires the overall function to be continuous.

What is the relationship between differentiability and continuity in multivariable functions?

Differentiability and continuity are closely related in multivariable functions. If a function is differentiable at a point, it must also be continuous at that point. However, a function can be continuous but not differentiable, as long as its partial derivatives do not exist or are not continuous at that point.

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