Concept:
The swing equation governs the electromechanical rotor dynamics of a synchronous machine during transient disturbances. It balances the input mechanical power, output electromagnetic power, and accelerating power. Mathematically, the swing equation is expressed as:
\[
\frac{H}{\pi f} \frac{d^2\delta}{dt^2} = P_m - P_e
\]
where $H$ is the inertia constant, $f$ is the system frequency, $\delta$ is the rotor power angle, $P_m$ is the mechanical shaft power input, and $P_e$ is the electrical power output.
Step 1: Analyze the order of the differential equation.
The swing equation contains the term $\frac{d^2\delta}{dt^2}$, which represents the second derivative of the rotor angle $\delta$ with respect to time $t$. This means it is mathematically classified as a second-order differential equation.
Step 2: Determine if the equation is linear or non-linear.
The electrical power output $P_e$ of a cylindrical rotor synchronous generator is given by the power-angle relation:
\[
P_e = P_{max} \sin\delta
\]
Substituting this expression back into the structural swing equation yields:
\[
\frac{H}{\pi f} \frac{d^2\delta}{dt^2} = P_m - P_{max} \sin\delta
\]
The presence of the transcendental function $\sin\delta$ introduces a fundamental non-linearity to the system. The variable $\delta$ cannot be separated linearly, making the differential equation non-linear.
Thus, the swing equation is a non-linear, second-order differential equation. This corresponds to Option (B).