Taylor series at x = 1: arctan(x)

In summary, the conversation discusses using the Maclaurin series of arctan(x) to obtain the Taylor series of arctan(x) at x=1. The suggested method is to substitute z=x-1, which results in arctan(z+1) and taking the derivatives at z=0. However, there is confusion about the change in the point of differentiation and whether it is valid to shift the nth derivative from f^(n)(1) to f^(n)(0). It is eventually concluded that taking derivatives at x=1 is necessary to obtain the Taylor series.
  • #1
SweatingBear
119
0
Hey forum. Is there any way one can take advantage of the Maclaurin series of \(\displaystyle \arctan (x)\) to obtain the Taylor series of \(\displaystyle \arctan (x)\) at \(\displaystyle x = 1\)? I attempted to obtain the series in the suggested manner but to no avail.

We have

\(\displaystyle \arctan (x) = \sum_{n=0}^\infty \frac { f^{(n)}(1) }{n!} (x - 1)^n \, . \)

Let \(\displaystyle z = x - 1 \iff x = z + 1\). Thus

\(\displaystyle \arctan (z + 1) = \sum_{n=0}^\infty \frac { f^{(n)}(0) }{n!} z^n \, . \)

We are taking the derivatives at \(\displaystyle z = 0\) in the sum in the right-hand side, because \(\displaystyle z = 0\) when \(\displaystyle x = 1\). But it seems we cannot use the Maclaurin series for \(\displaystyle \arctan (z + 1)\) since the argument is not around \(\displaystyle 0\) when \(\displaystyle z\) is around \(\displaystyle 0\).

It seems as if I will have to resort to brute-force derivative computations?
 
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  • #2
How did \(\displaystyle f^{(n)}(1) \) changed to \(\displaystyle f^{(n)}(0)\) by substitution ?
 
  • #3
Let us start by the following

\(\displaystyle \frac{1}{1+(x-1)^2} = \sum^{\infty}_{n=0} (-1)^n(x-1)^{2n}\) converges \(\displaystyle |x-1|<1 \)

\(\displaystyle \arctan(x-1) = \sum^{\infty}_{n=0} \frac{(-1)^n (x-1)^{2n+1}}{2n+1}\) converges on the same disk .



\(\displaystyle \frac{1}{1+x^2} = \sum^{\infty}_{n=0} (-1)^n x^{2n}\) converges \(\displaystyle |x|<1\)

\(\displaystyle \arctan(x) = \sum^{\infty}_{n=0} \frac{(-1)^n x^{2n+1}}{2n+1}\) converges on the same disk
 
  • #4
ZaidAlyafey said:
How did \(\displaystyle f^{(n)}(1) \) changed to \(\displaystyle f^{(n)}(0)\) by substitution ?

Does not the point of differentiation change when you introduce \(\displaystyle z\)? We were first wanting to take derivatives at \(\displaystyle x = 1\). But after the variable substitution we have a polynomial of \(\displaystyle z\) and when \(\displaystyle x = 1\), \(\displaystyle z\) is equal to \(\displaystyle 0\). Hence the point of differentiation must be zero and not one? Isn't this really the whole reason behind why we are able to manipulate Maclaurin series for Taylor series about expansion points other than zero. I am not entirely confident though, correct me if I am wrong.
 
  • #5
If we started with the following :

\(\displaystyle f(z)= \arctan (z) = \sum_{n=0}^\infty \frac { f^{(n)}(1) }{n!} (z - 1)^n \, . \) around 1

\(\displaystyle g(z) = \arctan (z + 1) = \sum_{n=0}^\infty \frac { g^{(n)}(0) }{n!} z^n \, . \) around 0

but since \(\displaystyle g(z) = f(z+1) \)

\(\displaystyle \arctan (z + 1) = \sum_{n=0}^\infty \frac { f^{(n)}(1) }{n!} z^n \, . \) around 0
 
  • #6
ZaidAlyafey said:
If we started with the following :

\(\displaystyle f(z)= \arctan (z) = \sum_{n=0}^\infty \frac { f^{(n)}(1) }{n!} (z - 1)^n \, . \) around 1

\(\displaystyle g(z) = \arctan (z + 1) = \sum_{n=0}^\infty \frac { g^{(n)}(0) }{n!} z^n \, . \) around 0

Hm, I am not quite sure I understand how it became an approximation around 0 just by increasing the argument by one. How we are suddenly taking the derivative at 1? Could you please elaborate?
 
  • #7
I believe you have to brute-force the evaluations of $\arctan^{(n)}(1)$ to get your Taylor expansion.
 
  • #8
I like Serena said:
I believe you have to brute-force the evaluations of $\arctan^{(n)}(1)$ to get your Taylor expansion.

Hm, all right thanks. But I would really appreciate it if somebody could help me understand this better:

sweatingbear said:
Does not the point of differentiation change when you introduce \(\displaystyle z\)? We were first wanting to take derivatives at \(\displaystyle x = 1\). But after the variable substitution we have a polynomial of \(\displaystyle z\) and when \(\displaystyle x = 1\), \(\displaystyle z\) is equal to \(\displaystyle 0\). Hence the point of differentiation must be zero and not one? Isn't this really the whole reason behind why we are able to manipulate Maclaurin series for Taylor series about expansion points other than zero. I am not entirely confident though, correct me if I am wrong.
 
  • #9
sweatingbear said:
Does not the point of differentiation change when you introduce \(\displaystyle z\)? We were first wanting to take derivatives at \(\displaystyle x = 1\). But after the variable substitution we have a polynomial of \(\displaystyle z\) and when \(\displaystyle x = 1\), \(\displaystyle z\) is equal to \(\displaystyle 0\). Hence the point of differentiation must be zero and not one? Isn't this really the whole reason behind why we are able to manipulate Maclaurin series for Taylor series about expansion points other than zero. I am not entirely confident though, correct me if I am wrong.

Yes. The point of differentiation changes.

You're talking a Taylor expansion of either $\arctan(x)$ around $x=1$, or of $\arctan(1+z)$ around $z=0$.
But I'm afraid that in both cases the Taylor expansion requires you to evaluate $\arctan^{(n)}(1)$.
 
  • #10
I like Serena said:
Yes. The point of differentiation changes.

Ok thank you! So would you say my line of argument is valid here:

sweatingbear said:
We have

\(\displaystyle \arctan (x) = \sum_{n=0}^\infty \frac { f^{(n)}(1) }{n!} (x - 1)^n \, . \)

Let \(\displaystyle z = x - 1 \iff x = z + 1\). Thus

\(\displaystyle \arctan (z + 1) = \sum_{n=0}^\infty \frac { f^{(n)}(0) }{n!} z^n \, . \)

We are taking the derivatives at \(\displaystyle z = 0\) in the sum in the right-hand side, because \(\displaystyle z = 0\) when \(\displaystyle x = 1\).

Namely that I shifted the \(\displaystyle n\):th derivative from \(\displaystyle f^{(n)}(1)\) to \(\displaystyle f^{(n)}(0) \)? Zaid seemingly objected this procedure, so I am a tad bit dubious...

____________________________________

I like Serena said:
You're talking a Taylor expansion of either $\arctan(x)$ around $x=1$, or of $\arctan(1+z)$ around $z=0$.
But I'm afraid that in both cases the Taylor expansion requires you to evaluate $\arctan^{(n)}(1)$.

All right, derivatives it is. Thank you!
 
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  • #11
sweatingbear said:
Ok thank you! So I my line of argument is valid here:

Erm... there's a small inconsistency there that is confusing.

You have the function $f$ in both formulas.
But $f$ also changes.
In the first formula you have $f(x)=\arctan(x)$, while in the second formula you should have $f^*(z)=\arctan(1+z)$.
Note that I have added a star * to indicate it's a different function.

In particular ${f^*}^{(n)}(0)=\arctan^{(n)}(1+0)=\arctan^{(n)}(1)$.
 
  • #12
I like Serena said:
You have the function $f$ in both formulas.
But $f$ also changes.
In the first formula you have $f(x)=\arctan(x)$, while in the second formula you should have $f^*(z)=\arctan(1+z)$.
Note that I have added a star * to indicate it's a different function.

In particular ${f^*}^{(n)}(0)=\arctan^{(n)}(1+0)=\arctan^{(n)}(1)$.

All right, but look at Zaid's post:

ZaidAlyafey said:
If we started with the following :

\(\displaystyle f(z)= \arctan (z) = \sum_{n=0}^\infty \frac { f^{(n)}(1) }{n!} (z - 1)^n \, . \) around 1

\(\displaystyle g(z) = \arctan (z + 1) = \sum_{n=0}^\infty \frac { g^{(n)}(0) }{n!} z^n \, . \) around 0

but since \(\displaystyle g(z) = f(z+1) \)

\(\displaystyle \arctan (z + 1) = \sum_{n=0}^\infty \frac { f^{(n)}(1) }{n!} z^n \, . \) around 0

He seemingly disagrees. What is going on?
 
  • #13
sweatingbear said:
All right, but look at Zaid's post:

He seemingly disagrees. What is going on?

It's the same thing.
Zaid name the other function $g$, where I named it $f^*$.
He introduced $g$ to write the Taylor expansion around z=0.
Then he showed that you still have to evaluate the $\arctan$ derivatives at 1.
 
  • #14
I like Serena said:
It's the same thing.
Zaid name the other function $g$, where I named it $f^*$.
He introduced $g$ to write the Taylor expansion around z=0.
Then he showed that you still have to evaluate the $\arctan$ derivatives at 1.

Hm, all right. Great, good to know that I was thinking correct in terms of changing the point of differentation.

ZaidAlyafey said:
How did \(\displaystyle f^{(n)}(1) \) changed to \(\displaystyle f^{(n)}(0)\) by substitution ?

ZaidAlyafey, is it wrong to do that according to you or were you thinking of something else? I would really like to know what you had in mind!

ZaidAlyafey said:
Let us start by the following

\(\displaystyle \frac{1}{1+(x-1)^2} = \sum^{\infty}_{n=0} (-1)^n(x-1)^{2n}\) converges \(\displaystyle |x-1|<1 \)

\(\displaystyle \arctan(x-1) = \sum^{\infty}_{n=0} \frac{(-1)^n (x-1)^{2n+1}}{2n+1}\) converges on the same disk .



\(\displaystyle \frac{1}{1+x^2} = \sum^{\infty}_{n=0} (-1)^n x^{2n}\) converges \(\displaystyle |x|<1\)

\(\displaystyle \arctan(x) = \sum^{\infty}_{n=0} \frac{(-1)^n x^{2n+1}}{2n+1}\) converges on the same disk

I understand where every series comes from, but I am afraid I don't understand what you wanted to put across. Could you please elaborate?
 
  • #15
Would really appreciate it if somebody could help me see things clearer!
 
  • #16
ZaidAlyafey said:
Let us start by the following

\(\displaystyle \frac{1}{1+(x-1)^2} = \sum^{\infty}_{n=0} (-1)^n(x-1)^{2n}\) converges \(\displaystyle |x-1|<1 \)

\(\displaystyle \arctan(x-1) = \sum^{\infty}_{n=0} \frac{(-1)^n (x-1)^{2n+1}}{2n+1}\) converges on the same disk .



\(\displaystyle \frac{1}{1+x^2} = \sum^{\infty}_{n=0} (-1)^n x^{2n}\) converges \(\displaystyle |x|<1\)

\(\displaystyle \arctan(x) = \sum^{\infty}_{n=0} \frac{(-1)^n x^{2n+1}}{2n+1}\) converges on the same disk

what is the difference between the expansion of \(\displaystyle \arctan(x)\) and \(\displaystyle \arctan(x-1)\) ?
 
  • #17
ZaidAlyafey said:
what is the difference between the expansion of \(\displaystyle \arctan(x)\) and \(\displaystyle \arctan(x-1)\) ?

The first one is about \(\displaystyle x = 0\) and the other one about \(\displaystyle x=1\), right?
 
  • #18
sweatingbear said:
The first one is about \(\displaystyle x = 0\) and the other one about \(\displaystyle x=1\), right?

I meant in the expansion , you realize that we only needed to put \(\displaystyle x-1\) instead of \(\displaystyle x\) to find the expansion of \(\displaystyle \arctan(x-1)\) using \(\displaystyle \arctan(x)\) but the coefficients are still the same right ?
 
  • #19
ZaidAlyafey said:
I meant in the expansion , you realize that we only needed to put \(\displaystyle x-1\) instead of \(\displaystyle x\) to find the expansion of \(\displaystyle \arctan(x-1)\) using \(\displaystyle \arctan(x)\) but the coefficients are still the same right ?

Yes the coefficients remain the same but simply changing the argument from \(\displaystyle x\) to \(\displaystyle x-1\) didn't really change the point of expansion, right? About \(\displaystyle x = 0\), we have

\(\displaystyle \arctan (x) = \sum_{n=0}^\infty (-1)^n \frac{x^{2n+1}}{2n+1} \, .\)

If we suddenly change the argument to \(\displaystyle x-1\), we get

\(\displaystyle \arctan (x - 1) = \sum_{n=0}^\infty (-1)^n \frac{(x-1)^{2n+1}}{2n+1} \, ,\)

but we are still expanding about \(\displaystyle x = 0\), not \(\displaystyle x = 1\). The problem is that we want an expansion about \(\displaystyle x=1\), hence my confusion.
 
  • #20
sweatingbear said:
Hey forum. Is there any way one can take advantage of the Maclaurin series of \(\displaystyle \arctan (x)\) to obtain the Taylor series of \(\displaystyle \arctan (x)\) at \(\displaystyle x = 1\)?
The blunt answer is NO. For any sufficiently smooth function $f$, the Taylor series for $f$ at the point $a$ is given by \(\displaystyle f(a+x) = \sum_{n=0}^\infty \frac{f^{(n)}(a)}{n!}x^n.\) In particular, the first term in the series, the constant term, is $f(a)$. For the function $f(x) = \arctan x$ and the point $a=1$, the series starts with the constant term $\arctan(1) = \pi/4$. So any answer that does not start with the constant term $\pi/4$ must be wrong. Of course, the Maclaurin series for $\arctan x$ does not contain any terms involving $\pi$, so you cannot expect to get the Taylor series at $x=1$ from that.

What we want to do here is to find a power series for $\arctan(1+x)$. One way to try to do that would be to notice that the first derivative of $\arctan(1+x)$ is \(\displaystyle \frac1{1+(1+x)^2}.\) So a good strategy would be to try to find a power series for that function and then integrate it term by term, adding the constant term $\pi/4$ at the start. That way, you can at least find the first few terms of the series: $$ \frac1{1+(1+x)^2} = \frac1{2+2x+x^2} = \frac12\,\frac1{1 + x\bigl(1+\frac x2\bigr)}.$$ Now use the series $(1+t)^{-1} = 1-t +t^2-t^3 + \ldots$, with $t = x\bigl(1+\frac x2\bigr)$, to get $$ \frac12\,\frac1{1 + x\bigl(1+\frac x2\bigr)} = \frac12\Bigl(1 - x\bigl(1+\tfrac x2\bigr) + x^2\bigl(1+\tfrac x2\bigr)^2 - x^3\bigl(1+\tfrac x2\bigr)^3 + \ldots\Bigr).$$ You can pick out the coefficients of the first few powers of $x$ to get a series starting $\frac12 - \frac12x + \frac14x^2 +\ldots$. (I think that the next term is $0$ but I haven't checked that.) Now integrate each term, add on the $\pi/4$ at the start, and you have the beginnings of the Taylor series for $\arctan x$ around $x=1$. But I don't believe that there is any simple formula for the general term of the series.
 
  • #21
sweatingbear said:
Yes the coefficients remain the same but simply changing the argument from \(\displaystyle x\) to \(\displaystyle x-1\) didn't really change the point of expansion, right? About \(\displaystyle x = 0\), we have

\(\displaystyle \arctan (x) = \sum_{n=0}^\infty (-1)^n \frac{x^{2n+1}}{2n+1} \, .\)

If we suddenly change the argument to \(\displaystyle x-1\), we get

\(\displaystyle \arctan (x - 1) = \sum_{n=0}^\infty (-1)^n \frac{(x-1)^{2n+1}}{2n+1} \, ,\)

but we are still expanding about \(\displaystyle x = 0\), not \(\displaystyle x = 1\). The problem is that we want an expansion about \(\displaystyle x=1\), hence my confusion.

Exactly . I just tried to point out that the substitution you did was not correct in the first post. It is not easy to find the Taylor expansion using the Maclaurin By substitution because you are transforming the function into different function .
 
  • #22
Thanks a bunch for the answers. I understand now that one cannot take advantage of the Maclaurin series of \(\displaystyle \arctan(x)\) in order to find the Taylor series about \(\displaystyle x=1\) for the function.

I will start a new thread regarding a question the discussion in this thread gave rise to (in order to avoid serious digressions).
 
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FAQ: Taylor series at x = 1: arctan(x)

1. What is a Taylor series?

A Taylor series is a mathematical representation of a function as an infinite sum of terms, where each term is a polynomial function of increasing degree.

2. How is a Taylor series different from other types of series?

A Taylor series is unique in that it is centered around a specific point, usually denoted as "a", and uses the derivatives of the function at that point to calculate the terms of the series.

3. What is the Taylor series at x = 1?

The Taylor series at x = 1 is a specific type of Taylor series where the center point is at x = 1. It is also known as the Maclaurin series, where the center point is at x = 0.

4. How is arctan(x) represented in a Taylor series at x = 1?

The Taylor series at x = 1 for arctan(x) is: arctan(x) = (π/4) + (x-1) - (x-1)^2/2 + (x-1)^3/3 - (x-1)^4/4 + ...

5. What are the applications of using a Taylor series at x = 1 for arctan(x)?

A Taylor series at x = 1 for arctan(x) can be used to approximate values of arctan(x) for any value of x, as long as it is within the convergence radius of the series. This can be useful in calculus, physics, and engineering applications where an exact value of arctan(x) may not be readily available.

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