Taking the derivative of a definite integral

Click For Summary

Discussion Overview

The discussion revolves around the process of taking the derivative of a definite integral, specifically in the context of mathematical operations related to Laplace transforms. Participants explore various aspects of differentiation, including the implications of definite versus indefinite integrals and the application of the Mean Value Theorem (MVT).

Discussion Character

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

Main Points Raised

  • One participant questions how to take the derivative of a definite integral, providing an example with an integral from 0 to infinity.
  • Another participant asserts that the derivative of a definite integral evaluated as a number is zero, but notes that derivatives of integrals with variable limits or parameters may not be zero.
  • Some participants discuss the implications of keeping the integral in algebraic form and the potential use of the Mean Value Theorem to evaluate derivatives.
  • A participant introduces the Leibniz formula for differentiation under the integral sign, noting that it leads to a zero derivative for definite integrals with constant limits.
  • Concerns are raised about the correctness of limits in the context of the Leibniz rule, prompting further clarification and exploration of the topic.
  • One participant expresses uncertainty about the implications of their reasoning and seeks feedback on their interpretation of the derivative of a definite integral.
  • Another participant mentions a specific problem related to Laplace transforms and the challenges of differentiating both sides of an equation involving definite integrals.
  • There is a suggestion that certain mathematical tricks may be necessary to manipulate integrals involving delta functions in the context of Laplace transforms.

Areas of Agreement / Disagreement

Participants express differing views on the implications of taking derivatives of definite versus indefinite integrals, with no consensus reached on the best approach or interpretation. The discussion remains unresolved with multiple competing perspectives.

Contextual Notes

Some participants highlight the importance of understanding the conditions under which derivatives of integrals are evaluated, particularly in relation to limits and the nature of the functions involved.

Who May Find This Useful

This discussion may be of interest to those studying calculus, particularly in the context of integration and differentiation, as well as students working with Laplace transforms and related mathematical concepts.

Alex6200
Messages
75
Reaction score
0
How do I do it? For example, if I have:

[tex]\int_{0}^{\infty}sf(x) dx[/tex]

How do I take the derivative with respect to x?

I was trying to derive the formula for an inverse laplace transform when I realized that I didn't know how to take the derivative of a definite integral.
 
Physics news on Phys.org
[tex]\frac{d}{dx} \left( \int_{0}^{\infty}sf(x) dx \right) = 0[/tex]
because the bracketed thing does not depend on x (it is just a number). It doesn't matter whether the integral is definite or not by the way.

Note however, that
[tex]\frac{d}{da} \left( \int_{0}^{a}sf(x) dx \right) \neq 0[/tex]
and
[tex]\frac{d}{db} \left( \int_{0}^{\infty}s f(x, b) dx \right) \neq 0[/tex]
and
[tex]\frac{d}{ds} \left( \int_{0}^{a}sf(x) dx \right) \neq 0[/tex]
in general!
 
CompuChip said:
[tex]\frac{d}{dx} \left( \int_{0}^{\infty}sf(x) dx \right) = 0[/tex]
because the bracketed thing does not depend on x (it is just a number). It doesn't matter whether the integral is definite or not by the way.


Interesting, but I’m not so sure about the last part of your statement. Since the indefinite integral does not result in just a number but an algebraic. If it is an indefinite integral, then the derivative of the integral of f(x) should be f(x), as the two operations cancel each other.



As far as the derivative of the definite integral, once you reduce the definite integral to just a number, then certainly the derivative is zero. However, what if you kept it in algebraic form? Then the question would be at what value do you evaluate the derivative? Can you not use the MVT to determine where to evaluate the derivative?
 
schroder said:
Interesting, but I’m not so sure about the last part of your statement.
You are right, I don't know what I was thinking. Of course, [itex]\int f(x) dx[/itex] still depends on x. Never mind that part.

As far as the derivative of the definite integral, once you reduce the definite integral to just a number, then certainly the derivative is zero. However, what if you kept it in algebraic form? Then the question would be at what value do you evaluate the derivative? Can you not use the MVT to determine where to evaluate the derivative?
You mean something like this?
[tex]\frac{d}{dx} \left( \int_a^b f'(x) \, dx \right) = \frac{d}{dx}( f(b) - f(a) ) = 0[/tex]

Otherwise, it's not quite clear to me what you mean.
 
CompuChip said:
You mean something like this?
[tex]\frac{d}{dx} \left( \int_a^b f'(x) \, dx \right) = \frac{d}{dx}( f(b) - f(a) ) = 0[/tex]

Otherwise, it's not quite clear to me what you mean.

To be candid, I am not 100% sure of what I mean either,:confused: but something is tugging at my brain concerning taking the derivative of a definite integral.

Maybe if I try an example that will at least clarify what I am thinking of.
Suppose we have a simple f(x) = x^2 Now we take the definite integral of that within the limits x = 3 and x = 4 . The numerical result is 12.333…
And of course if we differentiate that number the result is zero. Nothing Earth shaking about any of that.

But let’s leave the integral of x^2 in its algebraic format so we have this:
(x^3/3 where x = 4) – (x^3/3 where x =3) and Not evaluate that but differentiate it as it is which results in:
(x^2 where x = 4) – (x^2 where x = 3) and then we evaluate that we have
16 – 9 = 7.

The significance of this comes in when we consider the MVT which states
( f(4) – f(3) ) / 4 – 3 = Df(c) where c is the mean value on the interval from 3 to 4.
For f(x) = x^2, Df(x) = 2X
Putting it all together then for f(x) = x^2, 7 = 2x and x = 3.5 which is the mean value on the interval.

So, I come to my very tentative conclusion that the derivative of a definite integral of f(x) should be f(x) evaluated at the mean value on the interval defined by the limits of the definite integral. At least, this interpretation gives some meaning to the limits of integration of the definite integral which carries over into the derivative.

I am interested in getting your reaction to this idea no matter how critical.:smile:
 
You might be thinking of the very general "Leibniz' formula":
[tex]\frac{d}{dx}\int_{\alpha(x)}^{\beta(x)} f(x,t)dt= \frac{d\beta(x)}{dx}f(x,\beta(x))- \frac{d\alpha(x)}{dx}f(x,\alpha(x))+ \int_{\alpha(x)}^{\beta(x)}\frac{\partial f}{\partial x}dt[/tex]
One result of that is that
[tex]\frac{d }{dx} \int_a^b f(t)dt= 0[/tex]
because all of those derivatives are 0.

(Edited to correct sign error. Thanks, NoMoreExams.)
 
Last edited by a moderator:
HallsofIvy said:
You might be thinking of the very general "Leibniz' formula":
[tex]\frac{d}{dx}\int_{\alpha(x)}^{\beta(x)} f(x,t)dt= \frac{d\alpha(x)}{dx}f(x,\alpha(x))- \frac{d\beta(x)}{dx}f(x,\beta(x))+ \int_{\alpha(x)}^{\beta(x)}\frac{\partial f}{\partial x}dt[/tex]
One result of that is that
[tex]\frac{d }{dx} \int_a^b f(t)dt= 0[/tex]
because all of those derivatives are 0.

Are your limits correct?
 
schroder said:
As far as the derivative of the definite integral, once you reduce the definite integral to just a number, then certainly the derivative is zero. However, what if you kept it in algebraic form?
This algebraic form?

[tex]g(s) = \left( \int_{0}^{\infty}sf(x) dx \right) = s\int_{0}^{\infty}f(x) dx[/tex]

This is just a number times s; it doesn't depend on x at all, so the derivative wrt x is zero.

NoMoreExams said:
Are your limits correct?
Halls is correct. You can google "Liebniz integral rule" for more info.
 
D H said:
Halls is correct. You can google "Liebniz integral rule" for more info.

I did :)
 
  • #10
Well, the actual problem I want to solve is:

[tex]F(s) = \int_{0}^{\infty} e^{-st}f(t) dt[/tex]

for f(t). Now I want to take the derivative of both sides, and then multiply by [tex]e^{-st}[/tex], and then get f(t).

Now I know from looking at Laplace transforms that the infinity part always evaluates to 0, so in reality the laplace transform is just that integral evaluated at 0.

So I have:


[tex]F(s) = \int e^{-st}f(t) dt \left|t = 0[/tex]

But the problem is that I can't just plug in the infinity or 0 because I want to take the derivative of both sides, and I can't just take the derivative because the integral is definite. This is going to sound really stupid but is there a way to cancel the "plug in" operation?

And just to let you guys know my most advanced math class is differential equations.
 
  • #11
I don't think that's going to work. Probably you have to pull some trick like
[tex]\int_{\cdots}^{\cdots} e^{-a x} dx = \delta(a)[/tex]
(sorry haven't done math in like 6 weeks, bit rusty here) and use that to write some integral over F(s) which in the end gives you [tex]\int f(t) \delta(t - s) dt = f(s)[/tex].
 
  • #12
NoMoreExams said:
Are your limits correct?

D H said:
Halls is correct. You can google "Liebniz integral rule" for more info.
I am now. I edited what I had before because of NoMoreExams' question!
 

Similar threads

  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 27 ·
Replies
27
Views
3K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 8 ·
Replies
8
Views
3K
  • · Replies 25 ·
Replies
25
Views
4K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 6 ·
Replies
6
Views
3K