For a rolling solid sphere, the acceleration \(a\) down an inclined plane can be calculated using the formula that accounts for both the translation and rotation of the sphere:
\[a = \frac{5}{7} g \sin(\theta)\]
where \(\theta\) is the angle of inclination and \(g\) is the acceleration due to gravity. Here, \(\theta = 30^\circ\) and \(g = 9.8 \, \text{m/s}^2\). Plugging in the values:
\[a = \frac{5}{7} \times 9.8 \times \sin(30^\circ) = \frac{5}{7} \times 9.8 \times 0.5 = 3.5 \, \text{m/s}^2\]
This result shows that the rolling motion includes not just the translational kinetic energy but also rotational kinetic energy, which slows the acceleration compared to sliding without rotation.
| LIST I | LIST II | ||
|---|---|---|---|
| A. | Bipolar npn transistor operate in the cut-off mode. | I. The base-emitter is reverse biased and | |
| B. | Bipolar npn transistor operate in the saturation mode. | II. Both the base-emitter and base | |
| C. | Bipolar npn transistor operate in the inverse active mode. | III. The base-emitter is forward biased | |
| D. | Bipolar npn transistor operate in the forward active mode. | IV. Both the base-emitter and bas |
| LIST I | LIST II |
|---|---|
| A. Maxwell's First Equation | I. Modified Ampere's Law |
| B. Maxwell's Second Equation | II. Faraday's Laws of Electromagnetic Induction |
| C. Maxwell's Third Equation | III. Gauss Law in Electrostatics |
| D. Maxwell's Fourth Equation | IV. Gauss Law in Magnetostatics |