Challenging Integral: A Test of Mathematical Prowess
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Homework Help Overview
The discussion revolves around a challenging integral problem, likely involving techniques from calculus, particularly integration and substitution methods. Participants are exploring various approaches to simplify and solve the integral.
Discussion Character
- Exploratory, Mathematical reasoning, Problem interpretation, Assumption checking
Approaches and Questions Raised
- Participants discuss the substitution \( u = \ln(x) \) and its implications. There are attempts to factor expressions under square roots and to complete the square. Some participants express frustration over perceived lack of progress and question the effectiveness of certain methods.
Discussion Status
The discussion is active, with participants sharing their thoughts on various substitution techniques and transformations. There is a mix of guidance and challenges presented, with some participants questioning assumptions and others suggesting alternative approaches. No explicit consensus has been reached, but there are indications of productive exploration.
Contextual Notes
Some participants mention a lack of familiarity with prior exercises or guidance, which may affect their understanding of the current problem. There are references to specific mathematical identities and techniques that are under discussion, indicating a focus on deeper mathematical concepts.
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So:
Post the result of that substitution.
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After you use the substituion, the 1/x factor will go away and you can factorize that junk in the root sign, I think you can take it from there.
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HomogenousCow said:...I think the u=lnx substitution is quite obvious, I mean the 1/x factor is right there.
After you use the substituion, the 1/x factor will go away and you can factorize that junk in the root sign, I think you can take it from there.
Factorization under the square root won't help you a bit, but completing the square beneath it will.
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No, you haven't.omri_mar said:thank you all but I've tried it all...
And, you won't get any further help, because you are too damn lazy and refuse to follow up the exercises I give you. What do wish for? A solution handout you don't have to work for? You're not getting it.
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And, for the last time:omri_mar said:what execises? I am new here and I have no idea what your talking about. believe me I know a thing or two in math and this integral i couldn't solve so don't call me laze because I've tried for 5 hours befor I decided to ask for help. you can see that it is my first post
I gave you an exercise in POSTING your result when you make that u-substitution. Do so.
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Now, the first learning point is to compare THAT expression with the previous one. Do you agree that the new one is strictly simpler than what you began with? I assume you do (if not, disagree!).
Now, why is this important?
Simply because you should NOT, ever, believe that a single substition will make the rest trivial, or at least, easier than your first substition.
By the u-substition, you have made definite progress relative to your starting point, and THAT is why it is a good substitution! We have removed SOME nasties from the original, now we'll tackle the next one trying to frighten us.
Now, the really ugly thing confronting us is that square root expression, with a second degree polynomial inside it.
Square roots can only be removed by having a perfect square beneath it. But, we haven't got that.
Can we manipulate the stuff underneath the root sign to get a perfect square? That's our next job!
1. Option 1: We could FACTORIZE easily enough what's beneath the root, but that doesn't give us a required SQUARE, does it? So, we'll drop factorization.
2. option 2: What other manipulation than factorization can we do with a second-degree polynomial? We can "complete" the square.
Let's see where THAT takes us, so your next exercise is to write what is beneath the root sign in the shape (u+a)^2+b, where "a" and "b" will be numbers.
Post your result, so that we get a progressing solution in this thread.
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Well, how to proceed next?
Note that essentially, what we've got now is an expression of the shape:
[tex]\sqrt{v^{2}+w^{2}}, v=u+1, w=\sqrt{3}[/tex]
That is, we have a sum of squares under our root sign, rather than a single square which is what we REALLY want!
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Isn't, however, that expression awfully alike the expression for the length of the hypotenuse in a right-angled triangle?
And the functions of sine, cosine are tightly related to trigonometry..
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Thus, it would make sense to study trigonometric relations a bit, to see if they include an expression where a sum of squares can transform itself into a single square (our dearest wish!)
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Generally, we have the identity:
[tex]\sin^{2}(v)+\cos^{2}(v)=1[/tex]
Here, we DO have a sum of squares, but it is distinctly different from the one WE've got, because in that expression, only ONE of the addends is a variable, the other being the pesky number 3.
How can we improve on that nastiness?
If we divide through our identity with the squared cosine, we get:
[tex]\tan^{2}(v)+1=\frac{1}{\cos^{2}(v)}[/tex]
(Remember THAT identity in the future, it is extremely useful!)
If we now multiply that identity throughout with [itex](\sqrt{3})^{2})[/itex], we get:
[tex](\sqrt{3}\tan(v))^{2}+3=(\frac{\sqrt{3}}{\cos(v)})^{2}[/tex]
Here, we have precisely what we need to transform the sum of squares (LHS) beneath our root sign, into a single square on the RHS!
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Thus, our next substitution should be [itex]u+1=\sqrt{3}\tan(v)[/itex]
Make that substitution, remember also to use it on the "u" outside the rootside, and on the differential element "du"
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Now, write down what you then get, and I'll provide you with a really sleazy substitution that will help you further on!
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Now, we multiply that cosine factor into the parenthesis, and we get the integral:
[tex]\int\frac{dv}{\sqrt{3}\sin(v)-\cos(v)}[/tex]
Agreed?
We have managed to simplify our original integral into one with a linear combination of trig functions in the denominator.
The major sleaze now, is to use the half-angle formulas for the trig functions in a creative way.
We set:
[tex]s=\tan(\frac{v}{2})[/tex]
(This is called the Weierstrass substitution)
Note that:
[tex]\frac{ds}{dv}=\frac{1}{2}\frac{1}{\cos^{2}(\frac{v}{2})}=\frac{1}{2}(1+\tan^{2}(\frac{v}{2}))=\frac{1}{2}(1+s^{2}), dv=\frac{2ds}{1+s^{2}}[/tex]
Furthermore, we have, by the half-angle formulas,
[tex]\sin(v)=2\sin(\frac{v}{2})\cos(\frac{v}{2}), cos(v)=\cos^{2}(\frac{v}{2})-\sin^{2}(\frac{v}{2})[/tex]
and, of course (for use of numerator transformation: [tex]1=\cos^{2}(\frac{v}{2})+\sin^{2}(\frac{v}{2})[/tex]
Now, inserting all these relations into your integral, and dividing through with the square of cosines (remembering that s equals the "tan of v half", you get:
[tex]\int\frac{1+s^{2}}{2\sqrt{3}s-(1-s^{2})}\frac{2ds}{1+s^{2}}=\int\frac{2ds}{s^{2}+2\sqrt{3}s-1}[/tex]
Verify these steps, and see if the road ahead looks a bit brighter!
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[tex]Integral=\sqrt{2}\arctan(w)+C[/tex]
[tex]w=\frac{s+\sqrt{3}}{\sqrt{2}}[/tex]
[tex]s=\tan(\frac{v}{2})[/tex]
[tex]v=\arctan(\frac{u+1}{\sqrt{3}}[/tex]
[tex]u=\ln(x)[/tex]
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arildno said:Correct!
Now, we multiply that cosine factor into the parenthesis, and we get the integral:
[tex]\int\frac{dv}{\sqrt{3}\sin(v)-\cos(v)}[/tex]
At this stage, I'd look to recast the denominator into a single trig ratio in the form of ##R\sin(\theta - \phi)## and integrate the cosecant term. But half-angles are fine also. Not sure which approach is more work when you "unfurl" all the substitutions back to the original variable.
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Well, I haven't bothered to check. They'll differ by at most a well-hidden constant.Curious3141 said:At this stage, I'd look to recast the denominator into a single trig ratio in the form of ##R\sin(\theta - \phi)## and integrate the cosecant term. But half-angles are fine also. Not sure which approach is more work when you "unfurl" all the substitutions back to the original variable.
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arildno said:Well, I haven't bothered to check. They'll differ by at most a well-hidden constant.
No, at most two constants. The domain of the integrand is disconnected ## x \in (0,1)\cup(1,\infty)##. It's possible to have one constant for the first connected component and a different constant for the other.
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Since one of them actually hid itself from me, proves they are well-hidden, as I said.pwsnafu said:No, at most two constants. The domain of the integrand is disconnected ## x \in (0,1)\cup(1,\infty)##. It's possible to have one constant for the first connected component and a different constant for the other.
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omri_mar said:aaaa
I don't know if u need this or not, but
Substitution1: u=ln(x)
Substitution2: t=1/u
Makes it much easier.
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