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Now you start Its a fact that Taylor series can be used to study approximate solutions to non-linear ODEs. Use this fact to
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Solution:-

Given that

The Taylor series of a function is an infinite sum of terms that are expressed in terms of the function's derivatives at a single point.

Given

\frac{d^2x}{dt^2}+\sin x=0

subject to (0) = 0 and x'(0)=x_1\geq 0

Now we are considering fact that Taylor series can be used to steady approximate solutions to non linear ODE's

Let us take

α(t) =Σα, =0

then we get

x'(t)=\sum^\infty_{n=1}na_nt^{n-1}

similarly

x''(t)=\sum^\infty_{n=2}n(n-1)a_nt^{n-2}

By applying

\sin x=x-\frac{x^3}{3!}+\frac{x^5}{5!}+...

Thus we get

\sum^\infty_{n=2}n(n-1)a_nt^{n-2}+\sum^\infty_{n=0}a_nt^n-\frac{(\sum^\infty_{n=0}a_nt^n)^3}{3!}+\frac{(\sum^\infty_{n=0}a_nt^n)^5}{5!}=0we already know that (0) = 0 from equation

then we take a_0=0

Now substitute a_0=0 in the above equation

\sum^\infty_{n=2}n(n-1)a_nt^{n-2}+\sum^\infty_{n=0}a_nt^n-\frac{t^3(\sum^\infty_{n=0}a_nt^{n-1})^3}{6}+\frac{t^5(\sum^\infty_{n=0}a_nt^{n-1})^5}{120}...=0Now considering constant terms as

2(1)a_2=0

x'(0)=x_1=a_1

Now by considering coefficient of t

we have

3(2)a_3+a_1=0

By solving

6a_3+a_1=0

6a_3=-a_1

a_3=-\frac{a_1}{6}

we already know that x_1=a_1 substitute

a_3=\frac{-x_1}{6}

Now considering coefficient of t^2

12a_4+a_2=0

we get

a_2=0,\ \ a_4=0

Now considering coefficient of t^3

20a_5+a_3-\frac{a_1}{6}

then we get

20a_5-\frac{2a_1}{6}=0

a_5=\frac{a_1}{60}

as we know that a_1=x_1 then finally we get

a_5=\frac{x_1}{60}

Now similarly considering coefficient of t^4

30a_6+a_4-\frac{3a^2_1a_2}{6}=0

we already know that a_2=0 and a_4=0

Thus we get

a_6=0

Therefore

x(t)=x_1t-\frac{x_1}{6}t^3+\frac{x_1}{60}t^5...

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