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Find the Taylor series of the given function centered at the indicated point. \(\quad F(x)=\int_{0}^{x} \cos (\sqrt{t}) d t ; f(t)=\sum_{n=0}^{\infty}(-1)^{n} \frac{t^{n}}{(2 n) !}\) at \(a=0\) (Note: \(f\) is the Taylor series of \(\cos (\sqrt{t}) .)\)

Short Answer

Expert verified
The Taylor series of \( F(x) \) is \( \sum_{n=0}^{\infty} (-1)^n \frac{x^{n+1}}{(n+1)(2n)!} \).

Step by step solution

01

Understand Taylor Series Expansion

The Taylor series of a function \( f(t) \) centered at \( a=0 \) is given by \( \sum_{n=0}^{\infty} \frac{f^{(n)}(0)}{n!} x^n \). This formula expresses a function as an infinite sum of terms calculated from the values of its derivatives at a single point.
02

Note the Provided Series

We are given the Taylor series of \( f(t) = \cos(\sqrt{t}) \) as \( \sum_{n=0}^{\infty}(-1)^{n} \frac{t^{n}}{(2n)!} \). This series expansion is centered at \( t = 0 \).
03

Express \( F(x) \) as a Taylor Series

\( F(x) = \int_{0}^{x} \cos(\sqrt{t}) \, dt \) can be expressed as a series by integrating the given series for \( \cos(\sqrt{t}) \). Thus, \( F(x) = \int_{0}^{x} \sum_{n=0}^{\infty}(-1)^{n} \frac{t^{n}}{(2n)!} dt = \sum_{n=0}^{\infty}(-1)^{n} \int_{0}^{x} \frac{t^{n}}{(2n)!} dt \).
04

Integrate Term by Term

Integrate each term \( \int_{0}^{x} \frac{t^{n}}{(2n)!} dt \). The integral of \( t^n \) is \( \frac{t^{n+1}}{n+1} \) evaluated from 0 to x. Thus, the term becomes \( \frac{x^{n+1}}{(n+1)(2n)!} \).
05

Form the Taylor Series of \( F(x) \)

The Taylor series of \( F(x) \) centered at \( a=0 \) is then \[ F(x) = \sum_{n=0}^{\infty} (-1)^n \frac{x^{n+1}}{(n+1)(2n)!}. \] This is the Taylor series expansion of the integral function centered at 0.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Power Series
A power series is an infinite series of the form \( \sum_{n=0}^{\infty} a_n (x-c)^n \), where \( a_n \) are coefficients and \( c \) is the center of the series. Power series provide a way to represent functions as sums of polynomials, making complex functions easier to analyze and compute. The idea is that the series will converge to the function within a certain interval. This interval depends on the radius of convergence
  • A series may converge to a function, like the cosine function.
  • Powers like \( (x-c)^n \) expand around \( c \), simplifying functions that are analytically complex.
  • Power series are used in approximating functions across applied mathematics.
In our problem, we are given a power series for \( \cos(\sqrt{t}) \). From this, we aim to understand how \( F(x) = \int_{0}^{x} \cos(\sqrt{t}) dt \) can be expressed using series terms.
Cosine Function
The cosine function, \( \cos(x) \), is a trigonometric function characterized by its wave-like graph and periodicity. In mathematical terms, it can be expressed as a power series: \[ \cos(x) = \sum_{n=0}^{\infty} (-1)^n \frac{x^{2n}}{(2n)!} \]
  • Cosine is even, meaning \( \cos(-x) = \cos(x) \).
  • It repeats every \( 2\pi \), essential for many periodic processes.
  • Understanding its series helps evaluate integrals and find series expansions of more complex functions.
Using its power series representation aids in tasks such as the integration of \( \cos(\sqrt{t}) \), crucial for our original exercise.
Integration of Series
The integration of series involves finding the integral of each term in a power series representation separately. This process transforms a series term by term:
  • For \( \cos(\sqrt{t}) \), the original series is \( \sum_{n=0}^{\infty} (-1)^n \frac{t^n}{(2n)!} \).
  • Integrating individually, we use \( \int_{0}^{x} t^n dt = \frac{x^{n+1}}{n+1} \).
  • This allows converting the series of \( \cos(\sqrt{t}) \) into that of its integral, \( F(x) \).
The result is a new power series accurate for \( F(x) \) within the original's radius of convergence.
Centered Expansion
Centered expansion refers to the point around which a function's series is developed, fundamentally affecting convergence and accuracy. For Taylor series, this point is denoted as \( a \) and in our exercise is set to zero, making it a "Maclaurin series" as a special case of Taylor's.
  • The choice of \( a = 0 \) simplifies polynomial expressions.
  • Every term \( (x-a)^n \) becomes \( x^n \), streamlining calculations.
  • Centering expands cosine and integral functions symmetrically for small values of \( x \).
Choosing \( a = 0 \) leverages symmetry and eases computations crucial to derive the power series representation for \( \cos(\sqrt{t}) \). This centered approach ensures maximal simplicity and efficiency when dealing with such series.

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