Challenge Math Challenge - December 2020

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The Math Challenge discussion covers a variety of complex mathematical problems, including topics such as vector fields, number theory, topology, and combinatorics. Key problems include calculating the circulation of a vector field, proving properties of odd primes in relation to sums of squares, and exploring the topology of the torus. Participants also engage in discussions about the accuracy of algorithms for calculating series and integrals, as well as the probability of random distributions in combinatorial scenarios. The thread showcases collaborative problem-solving and the sharing of insights among participants.
  • #31
Infrared said:
Fair enough! But I would go further and apply that logic to the problem statement (if tori weren't manifolds...).
Yeah, that's true. It is not so difficult, but I still want to offer problems from which students can learn something, and if it is to look up the definitions and check them. And I am really bored by the integral questions ...
I can forgive @mathwonk for not checking Hausdorff if he's more used to varieties and the Zariski topology.
You mean the only reasonable and intuitive topology! :-p
 
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  • #32
thanks for the reminder many people make these extra assumptions. Among my books, this is not assumed in Lang, Loomis-Sternberg, or Hicks, but is assumed in Spivak and Warner. Bott-Tu and Hirsch also do not assume this in their definition, but state explicitly that all manifolds they consider will satisfy these conditions. One should keep in mind however that a very interesting example of a locally euclidean but non - hausdorff space is the line with a double origin, obtained by gluing R to R along R-{0}. Note too that this example makes it clear that the classification of 1-manifolds is more complicated without those assumptions, in particular there are infinitely many compact, connected 1-manifolds in the more general case.

Algebraic varieties in projective space, with the zariski topology, are of course separated, when one gives the correct definition of separated, namely that X is separated if the diagonal is closed in the product variety XxX. (The paradox is resolved by the fact that the zariski topology on this product is not the usual product topology!)
 
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  • #33
mathwonk said:
Note too that this example makes it clear that the classification of 1-manifolds is more complicated without those assumptions, in particular there are infinitely many compact 1-manifolds in the more general case.

I think this is actually a rather large loss. For example, intersection theory on smooth manifolds relies on the fact that there are zero boundary points on a compact ##1##-manifold, counted with orientation. So theorems like Poincare-Hopf, etc. would be in danger.

Another obvious loss is the Whitney embedding theorem.

mathwonk said:
Algebraic varieties in projective space, with the zariski topology, are of course separated, when one gives the correct definition of separated, namely that X is separated if the diagonal is closed in the product variety XxX. (The paradox is resolved by the fact that the zariski topology on this product is not the usual product topology!)

Okay, but considering projective varieties would be roughly analogous to studying submanifolds of ##\mathbb{R}^n## (okay I guess these are affine varieties, but the essential point is just that they live in a "nice" space you already know) and those are automatically Hausdorff. Removing the Hausdorff condition only affects abstract manifolds, just like abstract varieties aren't necessarily separated.

Edit: Maybe "abstract variety" is vague, and there can be ambiguity as to whether it should be separated (just like there is ambiguity as to whether manifolds should be Hausdorff).
 
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  • #34
That is true of course about projective varieties being automatically separated. I gave that example to simplify my statement about the hausdorff condition in algebraic geometry. The point is that one does define general schemes without the separated condition, and also abstract varieties as you say, and then one adds on the condition of separatedness when desired.

I don't consider those examples you mention as losses, since the theorems are still true, but one must simply make clear the hypotheses that are needed to make the theorems hold. There is also a gain in remembering non - separated varieties. I once heard a conference presentation where the speaker said all he had to do to prove his theorem was exhibit a certain type of mapping (a finite birational map of normal varieties that is not an isomorphism). (Must an injective continuous map of compact connected 1-manifolds be surjective?) Someone in the audience pointed out that the desired example would violate Zariski's "main theorem". The speaker said "that bothered me too, at first" to general laughter. then he pointed out that relaxing the condition of separation would solve the contradiction, but would still suffice to prove his result. In other words, consideration of a non - separated example allowed a proof of a result which he wanted mainly to apply to separated ones!

I guess the main issue is to remember that if one does not give ones definitions, we cannot assume everyone will use the same ones.
 
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  • #35
fresh_42 said:
I haven't checked since you said you did only half of it. I thought you would do the rest, too.
There's a failed attempt at solving the other side in that post, I'm not knowing how to use the weak law of large numbers here, since a statement of it is ##\lim_{n\to\infty}P\left( \left|\bar{x}_n-\mu \right|\geq \epsilon\right) =0##, not really knowing how to approximate the required ##n## value from that, the associated Chebychev's inequality might be useful though, namely ##P\left( \left|\bar{x}_n-\mu \right|\geq \epsilon\right)\leq \tfrac{\sigma ^2}{n\epsilon ^2}##? Anyhow, could you please take a look and my original post? Thanks @fresh_42

The rest will hopefully follow soon...
 
  • #36
benorin said:
Anyhow, could you please take a look and my original post? Thanks @fresh_42

The rest will hopefully follow soon...
I will, but I'll be busy the next two days, so it will take a while.
 
  • #37
It surprises me that nobody solved 5 yet.

For those who are interested and too lazy to look up the definition: A Hamilton group is a non-abelian group in which all subgroups are normal.
 
  • #38
Problem 10 is called a derangement. Derangement is when the objects of the permutation is not placed in the exact spot.
 
  • #39
Proof: First we show ##Q_8## is non abelian. We know ##ijk = -1##. Multiplying by ##ji## on the left gives ##k = -ji##. Similarly, multiplying by ##k## on the right gives ##-ij = -k##. So, ##(-j)i = k \neq i(-j)##.

We note that if ##G## is a group and ##H## is a subgroup of ##G## with index ##2##, then ##H## is normal in ##G##. It seems clear that any nontrivial subgroup of ##Q_8## is generated by a single element of ##Q_8##. Any subgroup generated by ##\pm i, \pm j, \pm k## has index ##2## and is therefore normal. The subgroup generated by ##-1## is the center of ##Q_8## and therefore is normal. So, ##Q_8## is Hamiltonian.

Next we note from Wikipedia: Let ##N## be a normal subgroup of ##G## and ##H## a subgroup of ##G##. We say ##G## is the semi direct product written ##N \rtimes H## if ##G = NH##, and these subgroups intersect trivially.

Let ##A, B## be two non trivial subgroups of ##G##. Then ##A \cap B \neq \lbrace 1 \rbrace## since ##-1 \in A \cap B##. And so the only way to write ##Q_8## as a semi direct product is ##Q_8 = 1 \rtimes Q_8##. []
[\SPOILER]
 
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  • #40
Math_QED said:
It surprises me that nobody solved 5 yet.

For those who are interested and too lazy to look up the definition: A Hamilton group is a non-abelian group in which all subgroups are normal.
... where the latter are Dedekind groups. Thus a Hamilton group is a non abelian Dedekind group.
 
  • #41
fishturtle1 said:
Proof: First we show ##Q_8## is non abelian. We know ##ijk = -1##. Multiplying by ##ji## on the left gives ##k = -ji##. Similarly, multiplying by ##k## on the right gives ##-ij = -k##. So, ##(-j)i = k \neq i(-j)##.

We note that if ##G## is a group and ##H## is a subgroup of ##G## with index ##2##, then ##H## is normal in ##G##. It seems clear that any nontrivial subgroup of ##Q_8## is generated by a single element of ##Q_8##. Any subgroup generated by ##\pm i, \pm j, \pm k## has index ##2## and is therefore normal. The subgroup generated by ##-1## is the center of ##Q_8## and therefore is normal. So, ##Q_8## is Hamiltonian.
Why is the center the only possible subgroup of index ##4##?
Next we note from Wikipedia: Let ##N## be a normal subgroup of ##G## and ##H## a subgroup of ##G##. We say ##G## is the semi direct product written ##N \rtimes H## if ##G = NH##, and these subgroups intersect trivially.

Let ##A, B## be two non trivial subgroups of ##G##. Then ##A \cap B \neq \lbrace 1 \rbrace## since ##-1 \in A \cap B##. And so the only way to write ##Q_8## as a semi direct product is ##Q_8 = 1 \rtimes Q_8##. []
 
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  • #42
benorin said:
I think I've got the first half done ok: CLT.

From the Central Limit Theorem (CLT) we have that ##Z=\tfrac{np - \mu _{p^{\prime}}}{\sigma _{p^{\prime}}}=1.645## where the value ##Z=1.645## comes from the ##95%## confidence level from a Z-table, ##\mu _{p^{\prime}} =np## is the population mean, and ##\sigma _{p^{\prime}} = \sqrt{\tfrac{p(1-p)}{n}}## because it's CLT for a proportion and here ##p=.48## is the probability of heads for the sample of biased coin flips and we get

$$Z= \tfrac{0.48n-0.5n}{\sqrt{ n(0.48)(0.52) }} = 1.645 \Rightarrow n=\left( 1.645 \tfrac{\sqrt{ (0.48)(0.52)}}{0.02} \right) ^{\tfrac{2}{3}} = 12$$

where the ceiling function was applied because ##n## is integer.

Here's where it get fuzzy...

According to the weak law of large numbers, in particular the associated Chebyshev's inequality we have

$$P\left( \left| \bar{x}_n - \mu\right|\geq \epsilon\right)\leq \tfrac{\sigma ^2}{n\epsilon ^2}$$

From the margin of error we have ##\epsilon =.02,## and since it's binomial trials we have that ##\sigma ^2 = np(1-p),## here ##p## is the probability of heads for the sample being ##p=0.48##. Hence
$$P\left( \left| p - \mu\right|\geq .02\right)\leq \tfrac{ n(0.48)(0.52)}{ n(0.02)^2}=0.05$$
since we are testing at the 95% confidence level--and freaking ##n## cancels instead of letting us solve for it: was I supposed to have used ##\sigma _{p^{\prime}} ^2 = \tfrac{p(1-p)}{n}## as in the CLT version? It might be wrong it's been a long while since my last stats course, and I'm kinda stoned so may have gremlins mucking about, speaking of which ##n=12## seems low.
You have to calculate ##P\left(\dfrac{S_n}{n};0.5\right) = P(Z<0.02)## for CLT and ##P\left(\left| \bar{X}-0.48 \right|>0.02\right)\leq \dfrac{0.2496}{n(0.02)^2}## for WLLN.
 
  • #43
#14:
An equilateral triangle with area 1 has the side length##\frac{2}{\sqrt[4]3} ##, and the triangle can be divided into 3 smaller triangles by connecting PA, PB and PC, with x,y and z being their height respectively.

##\frac{2}{\sqrt[4]3}\cdot(x+y+z)\cdot\frac{1}{2}=1##
##x+y+z = \sqrt[4]3##
 
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  • #44
Subgroups which contain at least one pure quaternion have at least ##4## elements ##\{\pm 1, \pm i\}## hence index ##2## or less. And the center has index ##4##. Other indices are not possible except for ##Q_8## and ##\{1\}##. So the only question is: what are the subgroups of index ##4##? (Or you could simply conjugate elements and calculate what happens, but your idea is nicer.)

Edit: I just saw that I answered the question ...
 
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  • #45
fresh_42 said:
They have ##4## elements ##\{\pm 1, \pm i\}## hence index ##2##. And the center has index ##4##. Other indices are not possible except for ##Q_8## and ##\{1\}##. So the only question is: what are the subgroups of index ##4##? (Or you could simply conjugate elements and calculate what happens, but your idea is nicer.)
I think the only subgroup of index ##4## is the center ##\lbrace \pm1 \rbrace##. Any subgroup of order ##2## must be generated by an element of order ##2##. There is only one element of order ##2## in ##Q_8##, namely ##-1##, and so there can only be one subgroup of order ##2##. Equivalently, there is only one subgroup of index ##4## which we have found.

Since every element in the center commutes with any element in the group, we see the center is normal in ##Q_8##.
 
  • #46
I sort of brute forced this hopefully its fine.

I solved simply added up the fractions and expanded everything out until I got the inequality:
$$
y^2z+y^2zx^2+2y^2zx+y^2z^2x+2yz+2yzx^2+yz^2x^2+yx^2+6yzx+2yz^2x+2yx+y+z+z^2x+2zx+x

\leq

zy^2+2zy+2zy^2x+4zyx+2zyx^2+2z^2yx+z^2yx^2+zy^2x^2+z^2y^2x+z^2y^2x^2+2yx+yx^2+y+z+2zx+z^2x+x+1$$

Then, I subtracted from both sides until I ended up with:
## 6xyz \leq 4xyz + x^2y^2z^2 + 1 ##

I got my final inequality: ##x^2y^2z^2+1-2xyz \geq 0## Here's kind of where I didn't know what to do, haven't studied multivariable minima and maxima, but let's try anyways. I don't really know the notation, I kind of just went along with whatever came up.

##\frac{dv}{dx} = 2z^2y^2x-2zy = 0##

The other partial derivatives are pretty much the same. You can solve and get that ##x y z = 1##. Hence, the initial equation at this minimum, not sure if its local or global, would be satisfied (##1^2 + 1 - 1 \geq 0##). I think there are other possibilities where xyz = 0 and that also satisfies a minimum, local or global, in which case the inequality is also satisfied (##0^2 + 1 - 0 \geq 0##). I think that ends up covering it all.

I hope I didn't mess anything up in the original calculation, and I hope my "proof" works (yeah it's definitely not a good proof).

I'd be interested in a non-brute force method.
 
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  • #47
lekh2003 said:
I'd be interested in a non-brute force method.
You can definitely write it in a more elegant way, because it is troublesome to proofread your solution. The key inequality comes directly from ##(xyz−1)^2>0.## If you multiply the inequality by its denominators and apply it, then things become at least readable. And of course: write down the solution in reverse order!
 
  • #48
fresh_42 said:
You can definitely write it in a more elegant way, because it is troublesome to proofread your solution. The key inequality comes directly from ##(xyz−1)^2>0.##
Ahh, that is exactly what I ended up with. So, I did it? Do I need to prove that (xyz-1)^2 is >= 0?
 
  • #49
lekh2003 said:
Ahh, that is exactly what I ended up with. So, I did it? Do I need to prove that (xyz-1)^2 is >= 0?
##\geq ## is sufficient, since we have all inequalities with the possibility of being equal. And ##\geq 0## is obvious. There is another little thing to consider: ##6+\ldots = 4+2+\ldots \leq 4+ xyz +\frac{1}{xyz}.##
 
  • #50
Time for another half-assed proof :P I hope I interpreted the problem correctly.
To maximise the area of the tetrahedron would involve maximising the area of the face ABC, which can maximise the lengths of BC, BA, and AC. This would involve taking the limit of the tetrahedron as it approaches a flat tetrahedron where the area of ABC is equal to the area of ABD+BCD+ADC. Any other type of tetrahedron will slowly reduce the area since AD, BD, CD are constant and the more spread out they are, the larger ABC's area is.

Hence, this is simply a problem of finding the area of an equilateral triangle with a distance of 1 from the center to each of the vertices. Using simple trigonometry and law of cosines, you can find the side length of this equilateral triangle. I used a triangle with tau/3 and a side of length 1 on either side. The opposite is ##\sqrt 3##. That's the side length of the equilaterqal triangle. Area of an equilateral triangle is ##\frac{\sqrt 3}{4}s^2##. Hence, the triangle has area ##\frac{3\sqrt 3}{4}##.

Since the surface area of the tetrahedron must be double the area of this equilateral triangle (when flat, this being the limit), then the maximum limit of area is ##\frac{3\sqrt 3}{2}.
 
  • #51
fresh_42 said:
##\geq ## is sufficient, since we have all inequalities with the possibility of being equal. And ##\geq 0## is obvious.
Oh yeah, of course its ##\geq 0##, I'm a fool.
fresh_42 said:
There is another little thing to consider:
How is this related?
 
  • #52
lekh2003 said:
Time for another half-assed proof :P I hope I interpreted the problem correctly.
To maximise the area of the tetrahedron would involve maximising the area of the face ABC, which can maximise the lengths of BC, BA, and AC. This would involve taking the limit of the tetrahedron as it approaches a flat tetrahedron where the area of ABC is equal to the area of ABD+BCD+ADC. Any other type of tetrahedron will slowly reduce the area since AD, BD, CD are constant and the more spread out they are, the larger ABC's area is.

Hence, this is simply a problem of finding the area of an equilateral triangle with a distance of 1 from the center to each of the vertices. Using simple trigonometry and law of cosines, you can find the side length of this equilateral triangle. I used a triangle with tau/3 and a side of length 1 on either side. The opposite is ##\sqrt 3##. That's the side length of the equilaterqal triangle. Area of an equilateral triangle is ##\frac{\sqrt 3}{4}s^2##. Hence, the triangle has area ##\frac{3\sqrt 3}{4}##.

Since the surface area of the tetrahedron must be double the area of this equilateral triangle (when flat, this being the limit), then the maximum limit of area is ##\frac{3\sqrt 3}{2}.
This is too hand wavy with too many unproven statements. Here is an image along which you (hopefully) formalize your argument:

tetrahedron.png
 
  • #53
lekh2003 said:
Oh yeah, of course its ##\geq 0##, I'm a fool.

How is this related?
Well, since you already got the credit and the solution is in any case a kind of brute force, I think I could simply post my solution:
##0\leq (xyz-1)^2=x^2y^2z^2-2xyz+1## and thus ##2\leq xyz+\dfrac{1}{xyz}.## Therefore
\begin{align*}
6&+2x+2y+2z+\dfrac{2}{x}+\dfrac{2}{y}+\dfrac{2}{z}+xy+yz+zx\\
&+\dfrac{1}{xy}+\dfrac{1}{yz}+\dfrac{1}{zx}+\dfrac{y}{x}+\dfrac{z}{y}+\dfrac{x}{z}\\
&\leq xyz+\dfrac{1}{xyz}+4+2x+2y+2z+\dfrac{2}{x}+\dfrac{2}{y}+\dfrac{2}{z}+xy+yz+zx\\&+\dfrac{1}{xy}+\dfrac{1}{yz}+\dfrac{1}{zx}+\dfrac{y}{x}+\dfrac{z}{y}+\dfrac{x}{z}\\
&\Longleftrightarrow \\
&\left(1+x+\dfrac{1}{y}\right)\cdot \left(1+y+\dfrac{1}{z}\right)+\left(1+y+\dfrac{1}{z}\right)\cdot\left(1+z+\dfrac{1}{x}\right)\\&+\left(1+z+\dfrac{1}{x}\right)\cdot\left(1+x+\dfrac{1}{y}\right)\\
&\leq \left(1+x+\dfrac{1}{y}\right)\cdot\left(1+y+\dfrac{1}{z}\right)\cdot\left(1+z+\dfrac{1}{x}\right)
\end{align*}
 
  • #54
I know it's been solved, but I just want to give it a shot myself for fun.

8d:

The denominator is almost a perfect square. Adding "zero" we can obtain:
$$I = \int_{-\infty}^{\infty} \frac{1}{x^2-2x+2}dx = \int_{-\infty}^{\infty} \frac{1}{x^2-2x+2 - 1 + 1}dx = \int_{-\infty}^{\infty} \frac{1}{(x-1)^2+1}dx$$
Using u-substitution, we obtain (the bounds don't change in this particular case).
$$I = \int_{-\infty}^{\infty} \frac{1}{u^2+1}dx$$
This is just a standard integral:
$$I = \left [\arctan(u) \right ]^\infty_{-\infty}$$
which leaves us with the two limits
$$I = \lim_{u \rightarrow \infty} \arctan(u) - \lim_{u \rightarrow -\infty} \arctan(u) = \frac{\pi}{2} - \left(- \frac{\pi}{2}\right) = \pi$$

For my own edification, how do I prove that ##\int \frac{1}{x^2+1} dx = \arctan(x) + C## and the value of the two limits? These are the things my professor would just tell us to "look up in a table" as our math course doesn't dig very deep.
 
  • #55
Mayhem said:
For my own edification, how do I prove that ##\int \frac{1}{x^2+1} dx = \arctan(x) + C##...
You can differentiate ##x \longmapsto \tan(x)=\dfrac{\sin(x)}{\cos(x)}## and use it to differentiate ##x\longmapsto x=(\tan \circ \operatorname{arctan})(x).## This would be a proof by differentiation instead of a direct integration. For a direct integration I'd try to do it with a Weierstraß substitution:
https://en.wikipedia.org/wiki/Weierstrass_substitution
... and the value of the two limits?
This depends on what you take for granted. E.g. if you know the graph of the tangent function then you automatically have the graph of the inverse function by reflection at the diagonal ##y=x##. Another possibility is to use approximation formulas like
$$
\operatorname{arctan} x \approx \begin{cases}
\dfrac{x}{1+0.28x^2} &\text{ if } |x|\leq 1\\
\dfrac{\pi}{2}-\dfrac{x}{x^2+0.28}&\text{ if }x>1\\
-\dfrac{\pi}{2}-\dfrac{x}{x^2+0.28}&\text{ if }x<-1
\end{cases}
$$
 
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  • #56
fresh_42 said:
You can differentiate ##x \longmapsto \tan(x)=\dfrac{\sin(x)}{\cos(x)}## and use it to differentiate ##x\longmapsto x=(\tan \circ \operatorname{arctan})(x).## This would be a proof by differentiation instead of a direct integration. For a direct integration I'd try to do it with a Weierstraß substitution:
https://en.wikipedia.org/wiki/Weierstrass_substitution

This depends on what you take for granted. E.g. if you know the graph of the tangent function then you automatically have the graph of the inverse function by reflection at the diagonal ##y=x##. Another possibility is to use approximation formulas like
$$
\operatorname{arctan} x \approx \begin{cases}
\dfrac{x}{1+0.28x^2} &\text{ if } |x|\leq 1\\
\dfrac{\pi}{2}-\dfrac{x}{x^2+0.28}&\text{ if }x>1\\
-\dfrac{\pi}{2}-\dfrac{x}{x^2+0.28}&\text{ if }x<-1
\end{cases}
$$
Can arctan(x) be differentiated using the definition of the derivative? Then you could use F'(x) = f(x) as a "proof".
 
  • #57
Mayhem said:
Can arctan(x) be differentiated using the definition of the derivative? Then you could use F'(x) = f(x) as a "proof".
It might work if you write it as a power series, but I guess it is quite hard if you only have
$$
\lim_{h \to 0} \dfrac{\operatorname{arctan}(x+h)-\operatorname{arctan}(x)}{h}
$$
The problem with any proof is always: 'Where are we allowed to start?', means what do we know already. If you can show ##F'(x)=f(x)## then you have automatically proven ##\int F'(x)\,dx = f(x)+C##. And even this uses the fundamental theorem of calculus.
 
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  • #58
fresh_42 said:
It might work if you write it as a power series, but I guess it is quite hard if you only have
$$
\lim_{h \to 0} \dfrac{\operatorname{arctan}(x+h)-\operatorname{arctan}(x)}{h}
$$
The problem with any proof is always: 'Where are we allowed to start?', means what do we know already. If you can show ##F'(x)=f(x)## then you have automatically proven ##\int F'(x)\,dx = f(x)+C##. And even this uses the fundamental theorem of calculus.
I think any starting point is fine as long as the starting point is 1) well defined 2) doesn't result in circular reasoning. Using the fact that ##(\arctan(x))' = 1/x^2 + 1 ## isn't circular, but in practice it is a bad way thinking, as guess-and-check quickly becomes unfeasible.
 
  • #59
Mayhem said:
I think any starting point is fine as long as the starting point is 1) well defined 2) doesn't result in circular reasoning. Using the fact that ##(\arctan(x))' = 1/x^2 + 1 ## isn't circular, but in practice it is a bad way thinking, as guess-and-check quickly becomes unfeasible.
My first suggestion should work. ##(\tan x)'=\left(\dfrac{\sin x}{\cos x}\right)'=1+\tan^2 x.## So
\begin{align*}
(id)'(x)=1&=(\tan \circ \operatorname{arctan})'(x)=(\tan y)'\cdot \operatorname{arctan }'(x)\\
&\Longrightarrow \\
\operatorname{arctan}'(x)&=\dfrac{1}{1+\tan^2(y)}=\dfrac{1}{1+\tan^2(\operatorname{arctan}(x))}=\dfrac{1}{1+x^2}
\end{align*}
but this uses ##(\sin)'=\cos\, , \,(\cos)'=-\sin## and ##1=\sin^2+\cos^2## in order to differentiate the tangent function.

I think that the direct way for ##\int\frac{dx}{1+x^2}## with the Weierstraß substitution works as well: ##t:=\tan\left(\dfrac{x}{2}\right)## which yields ##dx=\dfrac{2dt}{1+t^2}.## At least it immediately connects the rational polynomial with the tangent function.
 
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  • #60
fresh_42 said:
My first suggestion should work. ##(\tan x)'=\left(\dfrac{\sin x}{\cos x}\right)'=1+\tan^2 x.## So
\begin{align*}
(id)'(x)=1&=(\tan \circ \operatorname{arctan})'(x)=(\tan y)'\cdot \operatorname{arctan }'(x)\\
&\Longrightarrow \\
\operatorname{arctan}'(x)&=\dfrac{1}{1+\tan^2(y)}=\dfrac{1}{1+\tan^2(\operatorname{arctan}(x))}=\dfrac{1}{1+x^2}
\end{align*}
but this uses ##(\sin)'=\cos\, , \,(\cos)'=-\sin## and ##1=\sin^2+\cos^2## in order to differentiate the tangent function.

I think that the direct way for ##\int\frac{dx}{1+x^2}## with the Weierstraß substitution works as well: ##t:=\tan\left(\dfrac{x}{2}\right)## which yields ##dx=\dfrac{2dt}{1+t^2}.## At least it immediately connects the rational polynomial with the tangent function.
I'm not super familiar with Weierstrass substitution, but it does seem to yield a useful result.
 

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