Taylor Expansion of ln(cos(x))

In summary, the conversation discusses a Taylor expansion of f(x) = ln(cos(x)) and the incorporation of \mathcal{O}(x^6) terms in \mathcal{O}(x^8). There is a question about the result of multiplying out \left(-\frac{x^2}{2} + \mathcal{O}(x^4)\right)^3, with a suggestion that the result should be \mathcal{O}(x^{12}) instead of \mathcal{O}(x^8). The response is that in Taylor expansions, lower exponents are more important since x is considered 'small'.
  • #1
dobry_den
115
0
[tex]\biggl(-\frac{x^2}2 + \frac{x^4}{24} - \frac{x^6}{720} +\mathcal{O}(x^8)\biggr)-\frac12\biggl(-\frac{x^2}2+\frac{x^4}{24}+\mathcal{O}(x^6)\biggr)^2+\frac13\biggl(-\frac{x^2}2+\mathcal{O}(x^4)\biggr)^3 + \mathcal{O}(x^8)\\ & =-\frac{x^2}2 + \frac{x^4}{24}-\frac{x^6}{720} - \frac{x^4}8 + \frac{x^6}{48} - \frac{x^6}{24} +\mathcal{O}(x^8)\\
[/tex]

(http://en.wikipedia.org/wiki/Taylor_series#First_example)

This is a Taylor expansion of f(x) = ln(cos(x)) . I just wonder what happened with the first three O's, especially with (O(x^6))^2 and (O(x^4))^3. Are they somehow incorporated in O(x^8)?
 
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  • #2
Both of those go to [itex]\mathcal{O}(x^8)[/itex] when you multiply out...
For example:
[tex]\left (- \frac{x^2}{2}+ \mathcal{O}(x^4}) \right)^3[/tex]
multiplies out to:
[tex]-\frac {x^6}{8} + 3\frac{x^4}{4} \mathcal{O}(x^4) - 3\frac{x^2}{2} \mathcal{O}{x^8} + \mathcal{O}(x^12)[/tex]
[tex]-\frac{x^6}{8} + \left( \mathcal{O}(x^8) - \mathcal{O}(x^{10}) + \mathcal{O}(x^{12}) \right)[/tex]
[tex]-\frac{x^6}{8} + \mathcal{O}(x^8)[/tex]
 
  • #3
that's exactly what i don't get... shouldn't the result of

[tex]\mathcal{O}(x^8) - \mathcal{O}(x^{10}) + \mathcal{O}(x^{12}) \right)[/tex]

be O(x^12) since that is the largest term?
 
Last edited:
  • #4
dobry_den said:
that's exactly what i don't get... shouldn't the result of

[tex]\mathcal{O}(x^8) - \mathcal{O}(x^{10}) + \mathcal{O}(x^{12}) \right)[/tex]

be O(x^12) since that is the largest term?

Doesn't that depend on [itex]x[/itex]? (In Taylor expansions [itex]x[/itex] is 'small', so lower exponents are more important.)
 

1. What is the Taylor expansion of ln(cos(x))?

The Taylor expansion of ln(cos(x)) is an infinite series that represents the function ln(cos(x)) at a specific point, usually centered at x=0. It is given by the formula:
ln(cos(x)) = -x^2/2 - x^4/12 - 5x^6/288 - ...

2. How is the Taylor expansion of ln(cos(x)) derived?

The Taylor expansion of ln(cos(x)) is derived using the Taylor series expansion formula, which states that any infinitely differentiable function can be represented by an infinite sum of its derivatives evaluated at a specific point. In this case, the derivatives of ln(cos(x)) are used to calculate the coefficients of the series.

3. What is the purpose of the Taylor expansion of ln(cos(x))?

The Taylor expansion of ln(cos(x)) allows us to approximate the value of the function at any point near the center of expansion. This is useful in many mathematical and scientific applications, such as calculating the value of a function at a point where it is difficult to evaluate directly.

4. Can the Taylor expansion of ln(cos(x)) be used to find the value of ln(cos(x)) at any point?

Yes, the Taylor expansion of ln(cos(x)) can be used to find the value of ln(cos(x)) at any point near the center of expansion. However, the accuracy of the approximation depends on the number of terms used in the series.

5. Are there any limitations to using the Taylor expansion of ln(cos(x))?

Yes, the Taylor expansion of ln(cos(x)) is only accurate for points near the center of expansion. As the distance from the center increases, the accuracy of the approximation decreases. Additionally, the series may not converge for certain values of x, making the approximation impossible.

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