MHB Integral equation by successive approximation 2

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The integral equation $$y(x)= -1+\int_0^x(y(t)-sin(t))dt$$ is simplified to $$y(x)=-2+cos(x)+\int_0^x y(t)dt$$. The method of successive approximation is applied, leading to initial approximations $$y_1(x)=-2+cos(x)-x$$ and $$y_2(x)=-\frac{1}{2}x^2-2x-2+cos(x)+sin(x)$$. A general formula for $$y_n(x)$$ is not derived, but it is noted that the exact solution is $$y(x)= \frac{\sin x + \cos x - 3e^{x}}{2}$$. Each iteration improves the approximation towards this exact solution.
Suvadip
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I have to solve the integral equation $$y(x)= -1+\int_0^x(y(t)-sin(t))dt$$ by the method of successive approximation taking $$y_0(x)=-1$$.

Sol: After simplification the given equation we have
$$y(x)=-2+cos(x)+\int_0^x y(t)dt $$. So comparing it with $$y(x)=f(x)+\lambda\int_0^x k(x,t)y(t))dt$$ we have

$$f(x)=-2+cos(x), \lambda=1, k(x,t)=1$$

Now let us use the relation
$$y_n(x)=f(x)+\lambda\int_0^x k(x,t)y_{n-1}(t))dt$$

Using this relation we have

$$y_1(x)=-2+cos(x)-x, y_2(x)=-\frac{1}{2}x^2-2x-2+cos(x)+sin(x)$$

Using these I am unable to find a general formula for $$y_n(x)$$ from which the required solution $$y(x)$$ can be found using $$y(x)=lim_{n \to \infty} y_n(x)$$

How should I proceed.
 
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Re: integral equation by successive approximation

suvadip said:
I have to solve the integral equation $$y(x)= -1+\int_0^x(y(t)-sin(t))dt$$ by the method of successive approximation taking $$y_0(x)=-1$$.

Sol: After simplification the given equation we have
$$y(x)=-2+cos(x)+\int_0^x y(t)dt $$. So comparing it with $$y(x)=f(x)+\lambda\int_0^x k(x,t)y(t))dt$$ we have

$$f(x)=-2+cos(x), \lambda=1, k(x,t)=1$$

Now let us use the relation
$$y_n(x)=f(x)+\lambda\int_0^x k(x,t)y_{n-1}(t))dt$$

Using this relation we have

$$y_1(x)=-2+cos(x)-x, y_2(x)=-\frac{1}{2}x^2-2x-2+cos(x)+sin(x)$$

Using these I am unable to find a general formula for $$y_n(x)$$ from which the required solution $$y(x)$$ can be found using $$y(x)=lim_{n \to \infty} y_n(x)$$

How should I proceed.

Take into account that the integral equation has the 'exact' solution...

$\displaystyle y(x)= \frac{\sin x + \cos x - 3\ e^{x}}{2} = \frac{\sin x + \cos x}{2} - \frac{3}{2} - \frac{3}{2}\ x - \frac{3}{4}\ x^{2} - \frac{1}{4}\ x^{3} -... - \frac{3}{2\ n!}\ x^{n} - ...\ (1)$

... and at each iteration You obtain a better approximation to (1)...

Kind regards

$\chi$ $\sigma$
 
Here is a little puzzle from the book 100 Geometric Games by Pierre Berloquin. The side of a small square is one meter long and the side of a larger square one and a half meters long. One vertex of the large square is at the center of the small square. The side of the large square cuts two sides of the small square into one- third parts and two-thirds parts. What is the area where the squares overlap?

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