A rotating shaft with a mounted rotor behaves dynamically much like a simple spring-mass oscillator, where the shaft acts as the spring (with stiffness \( k \)) and the rotor acts as the suspended mass \( m \). Just as changing either the spring or the mass changes a spring-mass system's natural frequency, changing either the shaft's stiffness or the rotor's mass changes the shaft's critical speed. Checking the options with this analogy:
The spring-mass analogy confirms critical speed is governed jointly by mass and stiffness.
Therefore, the correct answer is mass and stiffness.
| LIST I | LIST II |
| A. Involute Gear | I. Variable Pressure Angle |
| B. Cycloidal Gear | II. Constant Pressure Angle |
| C. Gyroscope | III. Sensitivity |
| D. Governor | IV. Stability |