The given Bernoulli’s equation can be written as:
\[
\frac{dy}{dx} = y - y^3.
\]
As \( x \to \infty \), the solution \( y_c(x) \) tends to a steady-state value where \( \frac{dy}{dx} = 0 \). Solving for this steady state, we get:
\[
y - y^3 = 0 \quad \Rightarrow \quad y(1 - y^2) = 0.
\]
Since \( y>0 \), we find that \( y = 1 \). Therefore, as \( x \to \infty \), \( y_c(x) \to 1 \).