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Starting from the origin a body osillate...

Starting from the origin a body osillates simple harmonicall with a period of 2 s. A fter what time will its kinetic energy be 75% of the total energy?

A

`1/6s`

B

`1/4s`

C

`1/3s`

D

`1/12s`

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To solve the problem step by step, we will analyze the kinetic energy in simple harmonic motion (SHM) and find the time when the kinetic energy is 75% of the total energy. ### Step 1: Understand the relationship between kinetic energy and total energy in SHM In SHM, the total mechanical energy (E) is constant and is given by: \[ E = \frac{1}{2} m \omega^2 A^2 \] where: - \( m \) is the mass of the body, - \( \omega \) is the angular frequency, - \( A \) is the amplitude of the motion. The kinetic energy (KE) at any point in time is given by: \[ KE = \frac{1}{2} m v^2 \] where \( v \) is the velocity of the body. ### Step 2: Express kinetic energy in terms of displacement The velocity \( v \) in SHM can be expressed as: \[ v = \omega \sqrt{A^2 - x^2} \] where \( x \) is the displacement from the mean position. Therefore, the kinetic energy can be rewritten as: \[ KE = \frac{1}{2} m (\omega^2 (A^2 - x^2)) \] ### Step 3: Set up the equation for kinetic energy being 75% of total energy We want to find when the kinetic energy is 75% of the total energy: \[ KE = \frac{3}{4} E \] Substituting the expressions for KE and E, we get: \[ \frac{1}{2} m (\omega^2 (A^2 - x^2)) = \frac{3}{4} \left(\frac{1}{2} m \omega^2 A^2\right) \] ### Step 4: Simplify the equation Cancel out the common terms: \[ A^2 - x^2 = \frac{3}{4} A^2 \] This simplifies to: \[ x^2 = A^2 - \frac{3}{4} A^2 = \frac{1}{4} A^2 \] Thus, we find: \[ x = \frac{A}{2} \] ### Step 5: Find the time corresponding to this displacement The displacement in SHM is given by: \[ x = A \sin(\omega t) \] Substituting \( x = \frac{A}{2} \): \[ \frac{A}{2} = A \sin(\omega t) \] Dividing both sides by \( A \) (assuming \( A \neq 0 \)): \[ \frac{1}{2} = \sin(\omega t) \] ### Step 6: Solve for \( t \) Taking the inverse sine: \[ \omega t = \sin^{-1}\left(\frac{1}{2}\right) \] We know that: \[ \sin^{-1}\left(\frac{1}{2}\right) = \frac{\pi}{6} \] Now, we need to find \( \omega \): \[ \omega = \frac{2\pi}{T} \] Given that the period \( T = 2 \) seconds, we have: \[ \omega = \frac{2\pi}{2} = \pi \] Substituting back: \[ \pi t = \frac{\pi}{6} \] Thus: \[ t = \frac{1}{6} \text{ seconds} \] ### Final Answer The time after which the kinetic energy will be 75% of the total energy is: \[ t = \frac{1}{6} \text{ seconds} \]

To solve the problem step by step, we will analyze the kinetic energy in simple harmonic motion (SHM) and find the time when the kinetic energy is 75% of the total energy. ### Step 1: Understand the relationship between kinetic energy and total energy in SHM In SHM, the total mechanical energy (E) is constant and is given by: \[ E = \frac{1}{2} m \omega^2 A^2 \] where: - \( m \) is the mass of the body, - \( \omega \) is the angular frequency, ...
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