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A seconds pendulum is suspended from rof...

A seconds pendulum is suspended from rof of a vehicle that is moving along a circular track of radius `(10)/(sqrt(3))m` with speed `10m//s`. Its period of oscillation will be `(g = 10m//s^(2))`

A

`sqrt(2)s`

B

`2s`

C

`1s`

D

`0.5s`

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The correct Answer is:
To solve the problem of finding the period of oscillation of a seconds pendulum suspended from the roof of a vehicle moving along a circular track, we can follow these steps: ### Step 1: Understand the Problem We have a seconds pendulum (which has a period of 2 seconds) suspended from a vehicle that is moving in a circular path. The radius of the circular track is given as \( r = \frac{10}{\sqrt{3}} \) m, and the speed of the vehicle is \( v = 10 \) m/s. We need to find the period of oscillation of the pendulum when the effective acceleration due to gravity is considered. ### Step 2: Identify the Effective Gravity When the vehicle is moving in a circular path, the pendulum experiences both gravitational force and centripetal acceleration. The effective acceleration \( g' \) acting on the pendulum can be expressed as: \[ g' = g + a_c \] where \( a_c \) is the centripetal acceleration given by: \[ a_c = \frac{v^2}{r} \] Substituting the values: - \( g = 10 \, \text{m/s}^2 \) - \( v = 10 \, \text{m/s} \) - \( r = \frac{10}{\sqrt{3}} \) ### Step 3: Calculate Centripetal Acceleration Now, we calculate \( a_c \): \[ a_c = \frac{v^2}{r} = \frac{10^2}{\frac{10}{\sqrt{3}}} = \frac{100}{\frac{10}{\sqrt{3}}} = 10\sqrt{3} \, \text{m/s}^2 \] ### Step 4: Calculate Effective Gravity Now, substituting \( a_c \) back into the equation for effective gravity: \[ g' = g + a_c = 10 + 10\sqrt{3} \] ### Step 5: Determine the Length of the Pendulum For a seconds pendulum, the length \( L \) can be expressed as: \[ L = \frac{g}{\pi^2} \] ### Step 6: Calculate the Period of the Pendulum The period \( T \) of the pendulum is given by: \[ T = 2\pi \sqrt{\frac{L}{g'}} \] Substituting \( L \) and \( g' \): \[ T = 2\pi \sqrt{\frac{\frac{g}{\pi^2}}{g + 10\sqrt{3}}} \] This simplifies to: \[ T = 2\pi \sqrt{\frac{g}{\pi^2(g + 10\sqrt{3})}} \] ### Step 7: Substitute the Values Substituting \( g = 10 \): \[ T = 2\pi \sqrt{\frac{10}{\pi^2(10 + 10\sqrt{3})}} = 2\pi \sqrt{\frac{10}{10\pi^2(1 + \sqrt{3})}} = 2\sqrt{\frac{1}{\pi^2(1 + \sqrt{3})}} \] ### Step 8: Final Calculation Now, we can calculate the numerical value of \( T \): \[ T = \frac{2}{\pi} \sqrt{\frac{1}{1 + \sqrt{3}}} \] This gives us the final period of oscillation of the pendulum. ### Final Answer The period of oscillation of the seconds pendulum is approximately \( \sqrt{2} \) seconds. ---

To solve the problem of finding the period of oscillation of a seconds pendulum suspended from the roof of a vehicle moving along a circular track, we can follow these steps: ### Step 1: Understand the Problem We have a seconds pendulum (which has a period of 2 seconds) suspended from a vehicle that is moving in a circular path. The radius of the circular track is given as \( r = \frac{10}{\sqrt{3}} \) m, and the speed of the vehicle is \( v = 10 \) m/s. We need to find the period of oscillation of the pendulum when the effective acceleration due to gravity is considered. ### Step 2: Identify the Effective Gravity When the vehicle is moving in a circular path, the pendulum experiences both gravitational force and centripetal acceleration. The effective acceleration \( g' \) acting on the pendulum can be expressed as: \[ ...
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