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The displacement of an oscillating parti...

The displacement of an oscillating particle varies with time (in seconds ) according to the equation `y=(cm)= sin ((pi)/(2))(t/2 + 1/3)` The maximum acceleration of the particle is approximately

A

`5.21 cm //s^(2)`

B

`3.62 cm //s^(2)`

C

`1.81 cm //s^(2)`

D

`0.62 cm //s^(2)`

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The correct Answer is:
To find the maximum acceleration of the oscillating particle given the displacement equation \( y = \sin\left(\frac{\pi}{2}\left(\frac{t}{2} + \frac{1}{3}\right)\right) \), we can follow these steps: ### Step 1: Identify the Displacement Equation The displacement of the particle is given by: \[ y = \sin\left(\frac{\pi}{2}\left(\frac{t}{2} + \frac{1}{3}\right)\right) \] ### Step 2: Simplify the Displacement Equation We can rewrite the argument of the sine function: \[ y = \sin\left(\frac{\pi}{4}t + \frac{\pi}{6}\right) \] This shows that the angular frequency \( \omega \) can be identified from the term multiplying \( t \). ### Step 3: Determine the Angular Frequency \( \omega \) From the equation \( y = \sin\left(\frac{\pi}{4}t + \frac{\pi}{6}\right) \), we can see that: \[ \omega = \frac{\pi}{4} \, \text{radians/second} \] ### Step 4: Identify the Amplitude \( A \) The amplitude \( A \) of the oscillation is the coefficient in front of the sine function. Here, the amplitude is: \[ A = 1 \, \text{cm} \] ### Step 5: Calculate the Maximum Acceleration \( A_{max} \) The maximum acceleration \( A_{max} \) of a simple harmonic oscillator is given by the formula: \[ A_{max} = \omega^2 \cdot A \] Substituting the values we found: \[ A_{max} = \left(\frac{\pi}{4}\right)^2 \cdot 1 \] Calculating this gives: \[ A_{max} = \frac{\pi^2}{16} \, \text{cm/s}^2 \] ### Step 6: Approximate the Value Now we can calculate \( \frac{\pi^2}{16} \): \[ \pi \approx 3.14 \implies \pi^2 \approx 9.86 \] Thus, \[ A_{max} \approx \frac{9.86}{16} \approx 0.61625 \, \text{cm/s}^2 \] Rounding this gives approximately: \[ A_{max} \approx 0.62 \, \text{cm/s}^2 \] ### Final Answer The maximum acceleration of the particle is approximately: \[ \boxed{0.62 \, \text{cm/s}^2} \]
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