How Does U-Substitution Simplify Integration Problems?

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SUMMARY

The discussion focuses on the application of U-substitution in integration, specifically using the substitution \( u = 1 + x^2 \) to simplify the integral \( \int \frac{x}{u^2} dx \). Participants confirm that the derivative \( \frac{du}{dx} = 2x \) allows for the cancellation of \( x \) in the integrand, leading to the simplified integral \( \int \frac{1}{u^2} \frac{1}{2} du \). The conversation emphasizes the importance of experience in recognizing when substitutions will work effectively, as well as the necessity of practice in mastering integration techniques.

PREREQUISITES
  • Understanding of basic calculus concepts, including derivatives and integrals.
  • Familiarity with U-substitution in integration.
  • Knowledge of the chain rule for differentiation.
  • Ability to manipulate algebraic expressions involving variables and constants.
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  • Study the method of U-substitution in greater depth, focusing on various examples.
  • Learn about integration techniques such as integration by parts and trigonometric substitution.
  • Practice solving integrals that require recognizing patterns for substitution.
  • Explore the Fundamental Theorem of Calculus and its implications for definite integrals.
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Students and educators in calculus, particularly those seeking to improve their skills in integration techniques and U-substitution methods.

  • #31
QuarkCharmer said:
I already have, I was just thinking that the book would explain it, at least the idea, but it looks like it's jumping right into some sample definite integral problems instead. Ah well. I don't even know what a cauchy is :smile:

There are two ways to learn calculus: intuitive and easy, or rigorous with proofs. You need to know it intuitively before you can do it rigorously. But that means that the books will leave out facts that you don't find obvious at first. You'll need a more formal book if you want to understand everything , but I wouldn't advise this when first confronted with definite integrals :smile:
 
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  • #32
I'm reading from the Stewart book, and using the Spivak book as a reference, because I find it hard to understand sometimes.

Char. Limit said:
Well, that's mainly because as the number of "rectangles" increases (or goes to infinity), the difference between the area of all those rectangles and the area under the function will tend to 0, regardless of whether you use a left, right, or a mid point.

At least I think so.

Now that I think about it, this makes sense, because as the number of "n" increases, the width of each "n" decreases, and since x_i is always within \Delta x, the squeeze theorem would dictate that as \Delta x approaches 0, so does x_i. Does that make sense?
 
  • #33
QuarkCharmer said:
I'm reading from the Stewart book, and using the Spivak book as a reference, because I find it hard to understand sometimes.



Now that I think about it, this makes sense, because as the number of "n" increases, the width of each "n" decreases, and since x_i is always within \Delta x, the squeeze theorem would dictate that as \Delta x approaches 0, so does x_i. Does that make sense?

That makes sense to me, and is probably a good intuitive basis for this fact. Now, the Fundamental Theorem of Calculus, that doesn't really have much of an intuitive basis, unfortunately.
 
  • #34
Char. Limit said:
That makes sense to me, and is probably a good intuitive basis for this fact. Now, the Fundamental Theorem of Calculus, that doesn't really have much of an intuitive basis, unfortunately.
It sort of does, actually, but I've never found it all that helpful. Say you have a function f(x). At x=x0, it has a value f(x0). You can approximate the value of the function at a nearby point x1=x0+Δx as
f(x_1)=f(x_0+\Delta x) \approx f(x_0) + f'(x_0) \Delta x
You can see this easily from the graph. The intuition is simply that f'(x0) tells you which way the function is going at x=x0. If you know where you are, i.e., f(x0), and which way you're going, i.e., f'(x0), you can figure out where you'll end up, i.e., f(x1). If you rearrange it slightly, you already see an inkling of the fundamental theorem:
f(x_1) - f(x_0) \approx f'(x_0)\Delta x

Repeating the process, at the point x2=x1+Δx, you obtain
f(x_2)=f(x_1+\Delta x) \approx f(x_1) + f'(x_1) \Delta x \approx f(x_0) + f'(x_0) \Delta x + f'(x_1) \Delta x
and so on. Now let x0=a, xn=b, and Δx=(b-a)/n. Then xi=x0+i Δx, and
f(b) \approx f(a) + f'(a) \Delta x + f'(x_1) \Delta x + \cdots + f'(x_{n-1})\Delta x
or
f(b)-f(a) \approx f'(a) \Delta x + f'(x_1) \Delta x + \cdots + f'(x_{n-1})\Delta x
The righthand side is a Riemann sum, and in the limit Δx→0, you get
f(b)-f(a) = \int_a^b f'(x)\,dx
 
  • #35
I found a video of this rather strange looking man doing the proof:


Going to check to see if it's proven on ocw.mit.
 
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  • #36
QuarkCharmer said:
Related to this question:

\int sec^{3}(x)tan(x) dx

u=sec(x), and so, \frac{du}{dx}=sec(x)tan(x), and dx=\frac{du}{sec(x)tan(x)}

\int u^{3}tan(x) dx
\int \frac{u^{3}tan(x)}{sec(x)tan(x)} du
\int \frac{u^{3}}{sec(x)} du

I have no idea what to do with this one? Can I put my u=sec back in and try again now?

Edit: Na, that just gets me back to where I started.

Oh wait, because u is equal to sec, can I just call that \frac{u^{3}}{u} ?

You could note that f(x) = \sec^{3}(x) \tan(x) has the form f(x) = \sin(x)/ \cos^{4}(x), so substituting u = \cos(x) gives f(x) dx = - du/u^4.

RGV
 

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