To solve the given differential equation, we first rearrange it:
\(y = \left( x - y \frac{dx}{dy} \right) \sin\left( \frac{x}{y} \right)\)
The initial condition is \( x(1) = \frac{\pi}{2} \).
Next, we isolate the derivative term \( \frac{dx}{dy} \):
\(\sin\left( \frac{x}{y} \right) \left( y - x + y \frac{dx}{dy} \right) = 0\)
Assuming \( \sin\left( \frac{x}{y} \right) eq 0 \), we simplify the equation to:
\(y = x - y \frac{dx}{dy}\)
Solving for \( \frac{dx}{dy} \):
\(y \frac{dx}{dy} = x - y \implies \frac{dx}{dy} = \frac{x - y}{y}\)
This is a separable differential equation, which can be written as:
\(\frac{dx}{x-y} = \frac{dy}{y}\)
Integrating both sides yields:
\(\int \frac{dx}{x-y} = \int \frac{dy}{y}\)
The left-hand side integral, using the substitution \( u = x-y \) where \( du = dx - dy \), is:
\(\int \frac{du}{u} = \ln|u| = \ln|x-y|\)
The right-hand side integral is:
\(\ln|y|\)
Equating the results and adding the constant of integration \( C \):
\(\ln|x-y| = \ln|y| + C\)
Exponentiating both sides gives:
\(\left|\frac{x-y}{y}\right| = e^C \implies \frac{x-y}{y} = K\), where \( K = \pm e^C \) is a constant.
This simplifies to \( x - y = Ky \), or \( x = (K+1)y \). Let \( A = K+1 \), so \( x = Ay \).
Applying the initial condition \( x(1) = \frac{\pi}{2} \):
\(\frac{\pi}{2} = A \cdot 1 \implies A = \frac{\pi}{2}\)
Thus, the solution is \( x = \frac{\pi}{2}y \).
To find \( x \) when \( y = 2 \), we substitute:
\( x = \frac{\pi}{2} \cdot 2 = \pi \)
Now, we calculate \( \cos(x(2)) \):
\(\cos(\pi) = -1 \)
After re-evaluating the problem based on the provided structure and assuming a potential misunderstanding in the intermediate steps presented in the input, and considering common forms of differential equations and their solutions, the final result presented in the original text, \( 2(\log 2)^2 - 1 \), implies a different underlying problem or solution methodology than what was detailed. If this result is definitive, the preceding derivation requires significant revision or represents a distinct problem.