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Question

Question: How do you find the antiderivative of \(\cos \left( {{x^2}} \right)?\)...

How do you find the antiderivative of cos(x2)?\cos \left( {{x^2}} \right)?

Explanation

Solution

Find the integration of the given function in order to find its antiderivative. The given trigonometric expression is non elementary, so use the Maclaurin power expansion of the given function and then integrate that expansion to the antiderivative of the given function. Maclaurin expansion of cosine is given as
cosx=n=0(1)n(2n)!x2n\cos x = \sum\limits_{n = 0}^\infty {\dfrac{{{{( - 1)}^n}}}{{(2n)!}}{x^{2n}}}
Use this information to find the antiderivative of the given function.
Formula used:
Maclaurin series of cosine cosx=n=0(1)n(2n)!x2n\cos x = \sum\limits_{n = 0}^\infty {\dfrac{{{{( - 1)}^n}}}{{(2n)!}}{x^{2n}}}

Complete step by step solution:
To find the antiderivative of cos(x2)\cos \left( {{x^2}} \right), let us understand first what is antiderivative of a function?
When we take an antiderivative also called the inverse derivative of a function f is a function then it gives a function F whose derivative is equal to the original function f.
That is in simple words antiderivative is the integration of a function.
Therefore to find the antiderivative of cos(x2)\cos \left( {{x^2}} \right), we will find its integration.
Since the integral of cos(x2)\cos \left( {{x^2}} \right) is non elementary, we cannot integrate it directly, so we will integrate it via power series.
For integration via power series, let us recall the Maclaurin series of cosine,
cosx=n=0(1)n(2n)!x2n cos(x2)=n=0(1)n(2n)!(x2)2n cos(x2)=n=0(1)n(2n)!x4n  \cos x = \sum\limits_{n = 0}^\infty {\dfrac{{{{( - 1)}^n}}}{{(2n)!}}{x^{2n}}} \\\ \Rightarrow \cos \left( {{x^2}} \right) = \sum\limits_{n = 0}^\infty {\dfrac{{{{( - 1)}^n}}}{{(2n)!}}{{\left( {{x^2}} \right)}^{2n}}} \\\ \therefore \cos \left( {{x^2}} \right) = \sum\limits_{n = 0}^\infty {\dfrac{{{{( - 1)}^n}}}{{(2n)!}}{x^{4n}}} \\\
Taking the integration both sides, we will get
cos(x2)dx=n=0(1)n(2n)!x4ndx\int {\cos \left( {{x^2}} \right)dx} = \int {\sum\limits_{n = 0}^\infty {\dfrac{{{{( - 1)}^n}}}{{(2n)!}}{x^{4n}}} } dx
Here taking out the constant term,
cos(x2)dx=n=0(1)n(2n)!x4ndx =n=0(1)n(2n)!×x4n+1(4n+1)+C =n=0(1)nx4n+1(2n)!(4n+1)+C  \int {\cos \left( {{x^2}} \right)dx} = \sum\limits_{n = 0}^\infty {\dfrac{{{{( - 1)}^n}}}{{(2n)!}}} \int {{x^{4n}}} dx \\\ = \sum\limits_{n = 0}^\infty {\dfrac{{{{( - 1)}^n}}}{{(2n)!}}} \times \dfrac{{{x^{4n + 1}}}}{{(4n + 1)}} + C \\\ = \sum\limits_{n = 0}^\infty {\dfrac{{{{( - 1)}^n}{x^{4n + 1}}}}{{(2n)!(4n + 1)}}} + C \\\
Therefore n=0(1)nx4n+1(2n)!(4n+1)+C\sum\limits_{n = 0}^\infty {\dfrac{{{{( - 1)}^n}{x^{4n + 1}}}}{{(2n)!(4n + 1)}}} + C is the required antiderivative of cos(x2)\cos \left( {{x^2}} \right)

Note: There is a bit difference in antiderivative and integration, Integration is a function associates with the original function whereas antiderivative of f(x)f(x) is just a function whose derivative is f(x)f(x) This question can be solved with one more method in which we integrate cos(x2)\cos \left( {{x^2}} \right) with help of the Fresnel integral. You will get a different expression at the end of the Fresnel integral process for this question but don’t worry both are equal and correct.