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F - x equation of a body of mass 2kg in ...

`F - x` equation of a body of mass `2kg` in SHM is
`F + 8x = 0`.
Here, `F` is in newton and `x` in meter. Find time period of oscillations.

A

`2.14s`

B

`1s`

C

`3.14s`

D

None of these

Text Solution

AI Generated Solution

The correct Answer is:
To find the time period of oscillations for the body in simple harmonic motion (SHM) given the equation \( F + 8x = 0 \), we can follow these steps: ### Step 1: Rewrite the equation The equation given is: \[ F + 8x = 0 \] This can be rearranged to express the force \( F \) in terms of displacement \( x \): \[ F = -8x \] ### Step 2: Identify the spring constant \( k \) In SHM, the force can also be expressed as: \[ F = -kx \] where \( k \) is the spring constant. By comparing the two equations: \[ -kx = -8x \] we can see that: \[ k = 8 \, \text{N/m} \] ### Step 3: Use the formula for the time period \( T \) The time period \( T \) of a mass \( m \) attached to a spring (or in SHM) is given by the formula: \[ T = 2\pi \sqrt{\frac{m}{k}} \] where \( m \) is the mass of the body and \( k \) is the spring constant. ### Step 4: Substitute the values Given that the mass \( m = 2 \, \text{kg} \) and \( k = 8 \, \text{N/m} \), we can substitute these values into the formula: \[ T = 2\pi \sqrt{\frac{2}{8}} \] ### Step 5: Simplify the expression Calculating the fraction: \[ \frac{2}{8} = \frac{1}{4} \] Now substituting this back into the equation: \[ T = 2\pi \sqrt{\frac{1}{4}} = 2\pi \cdot \frac{1}{2} = \pi \] ### Step 6: Final result Thus, the time period \( T \) of the oscillations is: \[ T \approx 3.14 \, \text{seconds} \] ### Summary of the solution: The time period of oscillations for the body of mass \( 2 \, \text{kg} \) in SHM is approximately \( 3.14 \, \text{seconds} \). ---

To find the time period of oscillations for the body in simple harmonic motion (SHM) given the equation \( F + 8x = 0 \), we can follow these steps: ### Step 1: Rewrite the equation The equation given is: \[ F + 8x = 0 \] This can be rearranged to express the force \( F \) in terms of displacement \( x \): ...
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