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A point mass oscillates along the x-axis...

A point mass oscillates along the x-axis according to the law `x=x_(0) cos(omegat-pi//4)`. If the acceleration of the particle is written as `a=Acos(omegat+delta)`, the .

A

`A=x_(0)omega^(2),delta=(3pi)/(4)`

B

`A=x_(0),delta=-(pi)/(4)`

C

`A=x_(0)omega^(2),delta=(pi)/(4)`

D

`A=x_(0)omega^(2),delta=-(pi)/(4)`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to find the acceleration of a point mass oscillating along the x-axis given by the equation: \[ x = x_0 \cos(\omega t - \frac{\pi}{4}) \] We want to express the acceleration in the form: \[ a = A \cos(\omega t + \delta) \] ### Step-by-Step Solution: 1. **Identify the displacement function**: The displacement of the particle is given by: \[ x = x_0 \cos(\omega t - \frac{\pi}{4}) \] 2. **Differentiate to find velocity**: To find the velocity \( v \), we differentiate \( x \) with respect to time \( t \): \[ v = \frac{dx}{dt} = \frac{d}{dt}(x_0 \cos(\omega t - \frac{\pi}{4})) \] Using the chain rule: \[ v = -x_0 \omega \sin(\omega t - \frac{\pi}{4}) \] 3. **Differentiate to find acceleration**: Now, we differentiate the velocity \( v \) to find the acceleration \( a \): \[ a = \frac{dv}{dt} = \frac{d}{dt}(-x_0 \omega \sin(\omega t - \frac{\pi}{4})) \] Again, using the chain rule: \[ a = -x_0 \omega^2 \cos(\omega t - \frac{\pi}{4}) \] 4. **Rewrite the acceleration**: We can rewrite the cosine term using the angle addition formula: \[ a = -x_0 \omega^2 \cos\left(\omega t - \frac{\pi}{4}\right) = x_0 \omega^2 \cos\left(\omega t + \frac{3\pi}{4}\right) \] This is because: \[ \cos(\theta) = -\cos(\theta + \pi) \] 5. **Identify A and δ**: Now, we can compare this with the given form \( a = A \cos(\omega t + \delta) \): \[ A = x_0 \omega^2 \quad \text{and} \quad \delta = \frac{3\pi}{4} \] 6. **Final result**: Therefore, we have: \[ a = x_0 \omega^2 \cos(\omega t + \frac{3\pi}{4}) \] ### Conclusion: From the above steps, we conclude that: - \( A = x_0 \omega^2 \) - \( \delta = \frac{3\pi}{4} \) The correct option is: - \( a = x_0 \omega^2 \) and \( \delta = \frac{3\pi}{4} \) ---

To solve the problem, we need to find the acceleration of a point mass oscillating along the x-axis given by the equation: \[ x = x_0 \cos(\omega t - \frac{\pi}{4}) \] We want to express the acceleration in the form: \[ a = A \cos(\omega t + \delta) \] ...
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