To address this issue, a foundational understanding of distance and displacement within simple harmonic motion (SHM) is required.
Step 1: Determine the Number of Oscillations
Given a time period \( T = 2 \) seconds, the number of complete oscillations, \( n \), in 12.5 seconds is calculated as:
\(n = \frac{12.5}{2} = 6.25\)
Step 2: Define Distance and Displacement
In SHM, distance (\( D \)) represents the total path length traversed, whereas displacement (\( d \)) signifies the net change in position from the initial to the final point.
Step 3: Calculate Total Distance (D)
The particle completes 6 full oscillations and an additional 0.25 of an oscillation. The distance covered in one complete oscillation is four times the amplitude, as the particle moves from one extreme to the other and back:
\( D_{\text{one oscillation}} = 4 \times \text{Amplitude} = 4 \times 1 \, \text{cm} = 4 \, \text{cm} \)
Therefore, the total distance for 6 complete oscillations plus 0.25 of an oscillation is:
\(D = 6 \times 4 \, \text{cm} + (0.25 \times 4 \, \text{cm}) = 24 \, \text{cm} + 1 \, \text{cm} = 25 \, \text{cm}\)
Step 4: Calculate Displacement (d)
Following 6 full oscillations, the particle returns to its starting point, resulting in zero displacement for this portion. During the subsequent 0.25 oscillation, the particle moves from the equilibrium position to an extreme point:
\( d = \text{Amplitude} = 1 \, \text{cm} \)
Step 5: Compute the Ratio \( \frac{D}{d} \)
The ratio of the total distance to the displacement is:
\(\frac{D}{d} = \frac{25 \, \text{cm}}{1 \, \text{cm}} = 25\)
Consequently, the ratio \( \frac{D}{d} \) equals 25.
A particle is subjected to simple harmonic motions as: $ x_1 = \sqrt{7} \sin 5t \, \text{cm} $ $ x_2 = 2 \sqrt{7} \sin \left( 5t + \frac{\pi}{3} \right) \, \text{cm} $ where $ x $ is displacement and $ t $ is time in seconds. The maximum acceleration of the particle is $ x \times 10^{-2} \, \text{m/s}^2 $. The value of $ x $ is: