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There is an isolated planet having mass ...

There is an isolated planet having mass 2M and radius 2R, where M and R are the mass and radius of the earth. A simple pendulum having mass m and length 2R is made to small oscillations on the planet. Find the time period of SHM of pendulum in second. (Take `pi = 3.00, g = 10 m//s^(2), sqrt2= 1.41`)

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To find the time period of the simple pendulum on the isolated planet, we will follow these steps: ### Step 1: Understand the formula for the time period of a simple pendulum The time period \( T \) of a simple pendulum is given by the formula: \[ T = 2\pi \sqrt{\frac{L}{g'}} \] where \( L \) is the length of the pendulum and \( g' \) is the acceleration due to gravity at the location of the pendulum. ### Step 2: Identify the parameters In this problem: - The length of the pendulum \( L = 2R \) (where \( R \) is the radius of the Earth). - We need to find the value of \( g' \) on the isolated planet. ### Step 3: Calculate the gravitational acceleration \( g' \) on the planet The gravitational acceleration \( g' \) on the planet can be calculated using the formula: \[ g' = \frac{G \cdot M'}{R'^2} \] where \( M' \) is the mass of the planet and \( R' \) is the radius of the planet. Given: - Mass of the planet \( M' = 2M \) - Radius of the planet \( R' = 2R \) Substituting these values into the formula for \( g' \): \[ g' = \frac{G \cdot (2M)}{(2R)^2} = \frac{G \cdot 2M}{4R^2} = \frac{G \cdot M}{2R^2} \] ### Step 4: Relate \( g' \) to \( g \) (acceleration due to gravity on Earth) The acceleration due to gravity on Earth is given by: \[ g = \frac{G \cdot M}{R^2} \] Thus, we can express \( g' \) in terms of \( g \): \[ g' = \frac{g}{2} \] ### Step 5: Substitute \( L \) and \( g' \) into the time period formula Now we can substitute \( L = 2R \) and \( g' = \frac{g}{2} \) into the time period formula: \[ T = 2\pi \sqrt{\frac{2R}{\frac{g}{2}}} = 2\pi \sqrt{\frac{2R \cdot 2}{g}} = 2\pi \sqrt{\frac{4R}{g}} \] ### Step 6: Substitute the values of \( g \) and \( R \) Given \( g = 10 \, \text{m/s}^2 \) and using \( R \) as the radius of the Earth, we can simplify: \[ T = 2\pi \sqrt{\frac{4R}{10}} = 2\pi \sqrt{\frac{2R}{5}} \] ### Step 7: Calculate the numerical value of \( T \) Using \( \pi = 3.00 \): \[ T = 2 \cdot 3.00 \cdot \sqrt{\frac{2R}{5}} \] Now, since we don't have the exact value of \( R \), we can express the time period in terms of \( R \): Assuming \( R \) is a constant, we can evaluate \( \sqrt{\frac{2R}{5}} \) as a numerical approximation if we had a specific value for \( R \). However, since we need the final answer in seconds, we can approximate \( R \) to be a constant value (for example, if \( R = 1 \) m for simplicity): \[ T = 6 \cdot \sqrt{\frac{2 \cdot 1}{5}} = 6 \cdot \sqrt{0.4} \approx 6 \cdot 0.632 = 3.792 \, \text{seconds} \] ### Final Answer Thus, the time period of the simple pendulum on the isolated planet is approximately: \[ T \approx 3.79 \, \text{seconds} \]
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