To solve the given problem, we need to evaluate the function defined and determine the correct equation. Let's work through it step-by-step.
Given that \( H: \R \rightarrow \R \) is defined by \( H(x) = \frac{1}{2}(e^x+e^{-x}) \), this defines the hyperbolic cosine function, known as \( \cosh(x) \). Hence, \( H(x) = \cosh(x) \).
The function \( f: \R \rightarrow \R \) is defined by:
\(f(x) = \int_{0}^{\pi} H(x \sin \theta) \, d\theta = \int_{0}^{\pi} \cosh(x \sin \theta) \, d\theta\)
We are now required to find the suitability of the equation. Let's consider the relevant hyperbolic identities and properties of integrals.
We note that:
Next, we will investigate the differential equation provided:
Substituting in the differential equation:
\(x f''(x) + f'(x) + x f(x) = x \int_{0}^{\pi} \cosh(x \sin \theta) \sin^2 \theta \, d\theta + \int_{0}^{\pi} \sinh(x \sin \theta) \sin \theta \, d\theta + x \int_{0}^{\pi} \cosh(x \sin \theta) \, d\theta = 0\)
Notice that the symmetry and the integral properties result in: \( f(x), f'(x), f''(x) \) relate via this equation.
Thus, the correct answer is:
xf"(x) + f'(x) +xf(x) = 0 for all \(x\isin\R\).