A Numerical Insight for the Fundamental Theorem of Calculus - Comments

Click For Summary

Discussion Overview

The discussion revolves around the Fundamental Theorem of Calculus, exploring its implications, limitations, and interpretations, particularly in the context of numerical insights and educational approaches. Participants examine the theorem's applicability to various classes of functions, including differentiable and Riemann-integrable functions, as well as connections to numerical methods.

Discussion Character

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

Main Points Raised

  • Some participants note that the statement \(\int f'(x)dx = f(x)\) is valid only for a restricted class of differentiable functions, while the reverse holds for a broader class of Riemann-integrable functions.
  • Others introduce Lebesgue's theorem, which states that if \(\phi(x)\) is a summable function, its indefinite integral is continuous and has a derivative equal to \(\phi(x)\) almost everywhere, highlighting the importance of the "almost everywhere" clause.
  • A participant emphasizes the educational aspect, suggesting that the insight is beneficial for those unfamiliar with the Fundamental Theorem of Calculus, and that generalizing the theorem is not incorrect but can obscure the importance of limiting scope.
  • Some participants discuss numerical approximations, arguing that certain formulas hold for any function, but question the relevance of these approximations in illustrating the theorem for differentiable functions.
  • There is mention of a "telescoping sum" argument related to the theorem, which is likened to concepts in Stoke's theorem, emphasizing boundary conditions.
  • One participant reflects on the intended audience for the insight, suggesting it is aimed at students new to calculus, particularly those not exposed to rigorous mathematical definitions.
  • Connections to physics are raised, with discussions on how derivatives and integrals can be understood in a non-calculus context, focusing on numerical or algebraic interpretations without limit operators.

Areas of Agreement / Disagreement

Participants express a range of views, with some agreeing on the educational intent of the insight while others contest the applicability of the theorem to various function classes. The discussion remains unresolved regarding the implications of numerical methods and the appropriateness of the theorem's generalizations.

Contextual Notes

Limitations include the dependence on definitions of differentiability and integrability, as well as the unresolved nature of certain mathematical steps related to the application of the theorem across different function classes.

Delta2
Homework Helper
Insights Author
Messages
6,002
Reaction score
2,628
Greg Bernhardt submitted a new blog post

A Numerical Insight for the Fundamental Theorem of Calculus
calc_therom.png


Continue reading the Original Blog Post.
 

Attachments

  • calc_therom.png
    calc_therom.png
    17.1 KB · Views: 1,030
  • Like
Likes   Reactions: jim mcnamara, Adam Talman, Wrichik Basu and 2 others
Physics news on Phys.org
Well - it is correct for a restricted class of functions. Saying \int f'(x)dx =f(x) presupposes that f(x) is differentiable (otherwise the expression is meaningless). The other way around (\frac{d}{dx}\int f(x)dx) allows for a larger class of functions (the Riemann-integrable functions).

Going to an even larger class of functions, we have the following theorem of Lebesgue:
If φ(x) is a summable function, its indefinite integral F(x)=\int_{a}^{x}\phi(t)dt is a continuous function of bounded variation and it has almost everywhere a derivative equal to φ(x).

Observe the "almost everywhere" clause which is typical for all integrals based on measure theory. Lebesgue also proved a theorem about the other direction:
The derivative φ(x) of an absolutely continuous function F(x) defined on the closed interval [a, b] is summable and for every x \int_{a}^{x}\phi(t)dt = F(x)-F(a).

Observe the restriction on φ(x)!
 
I think the point of the insight is that for someone unfamiliar with the Fundamental Theorem of Calculus, that reader would find the discussion useful.

Mathematicians often do exactly what @Svein did - generalize or expand the scope. Which is not an incorrect position in any way. Simply put: Sometimes knowing when to limit scope can be instructive, too.
 
  • Like
Likes   Reactions: jcw99, vela, Delta2 and 1 other person
These approximations will always be true for any function. For instance

##Σ((f(x_{i}+Δx)-f(x_{i})/Δx)Δx## will always give ##f(x_{n})-f(x_{0})## no matter what the function. So in order for the argument to be true one needs a limiting argument. One might ask "Why if this formula is true for any function at all, does it illustrate the theorem in the case that ##f## is differentiable?".

On the other hand, the picture is right as @Svein says for differentiable functions and is certainly helpful.
 
Last edited:
  • Like
Likes   Reactions: Delta2
lavinia said:
Σ((f(xi+Δx)−f(xi)/Δx)ΔxΣ((f(x_{i}+Δx)-f(x_{i})/Δx)Δx will always give f(xn)−f(x0)f(x_{n})-f(x_{0}) no matter what the function.
As usual, someone has to come up with a pathological function. Not the Dirichlet function this time, but \int_{0}^{1}\sin(\frac{1}{x})dx...
 
The "telescoping sum" argument as to why ##\int_A^B f'(x) dx = f(A) - f(B)## is a simplified case of the argument leading to Stoke's theorem. You get perfect cancellations everywhere except the boundary.
 
  • Like
Likes   Reactions: Delta2
Sorry for the late reply, its because only now I am being able to see the comments and reply (due to some conflict with my account and the insights forum login subsystem)

Well about as @jim mcnamara said, this insight was meant for students that are now introduced to calculus, for high school students or for students of technical schools that aren't taught calculus with mathematical rigor but possibly they want to gain some intuitive simple insight on calculus.

When I was writing the insight I had in mind the Rieman integrable functions but @Svein is right. But then again Lavinia is more right cause here the derivative is not the real derivative, it is just an approximation of the real derivative, so the approximations just hold for any class of functions.
 
  • Like
Likes   Reactions: jcw99
Does this view relate to the one from physics without calculus?

derivative = velocity = distance / time

integral = distance = velocity X time
 
atyy said:
Does this view relate to the one from physics without calculus?

derivative = velocity = distance / time

integral = distance = velocity X time
It is not exactly like this but one could say that this is the basic idea.

More precisely what I do is that I remove the limit operator (if I can call it that way) from the definition of integral and derivative , and I just take as integral the sum of ##f(x_i)\Delta x_i## for small enough ##\Delta x_i## and as derivative the ratio of difference for small enough ##\Delta x##. Without the limit operator everything becomes numerical or algebraic.
 

Similar threads

  • Sticky
  • · Replies 3 ·
Replies
3
Views
6K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 15 ·
Replies
15
Views
3K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 7 ·
Replies
7
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 1 ·
Replies
1
Views
4K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 42 ·
2
Replies
42
Views
5K