How do I show that a particular solution $y_{1}$ of the ODE $$y''-k^{2}y=R(x)$$ $k\neq0$, is given by $$y_{1}=\frac{1}{k}\int_{0}^{x}R(t)\sinh(k(x-t))dt$$
I really have no idea how to do it.
How do I show that a particular solution $y_{1}$ of the ODE $$y''-k^{2}y=R(x)$$ $k\neq0$, is given by $$y_{1}=\frac{1}{k}\int_{0}^{x}R(t)\sinh(k(x-t))dt$$
I really have no idea how to do it.
The full version of the general solution of the corresponding ODE done by variation of parameters is $y=C_1\sinh kx+C_2\cosh kx+\sinh kx\int_0^x\dfrac{R(x)\cosh kx}{k}dx-\cosh kx\int_0^x\dfrac{R(x)\sinh kx}{k}dx$
Note that the general solution can also rewrite as
$y=C_1\sinh kx+C_2\cosh kx+\dfrac{\sinh kx}{k}\int_0^xR(t)\cosh kt~dt-\dfrac{\cosh kx}{k}\int_0^xR(t)\sinh kt~dt$
$y=C_1\sinh kx+C_2\cosh kx+\dfrac{1}{k}\int_0^xR(t)(\sinh kx\cosh kt-\cosh kx\sinh kt)~dt$
$y=C_1\sinh kx+C_2\cosh kx+\dfrac{1}{k}\int_0^xR(t)\sinh(k(x-t))~dt$
The particular solution part is $y_1=\dfrac{1}{k}\int_0^xR(t)\sinh(k(x-t))~dt$
Hint: You can use the Laplace transform techniques to get this solution.
Added: You can follow the steps:
1) Take the Laplace transform of the ode.
2) Rearrange and solve for $Y(s)$
3) apply the initial conditions if they have been given
4) take the inverse Laplace transform and you need to use the convolution property of the Laplace transform.