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A body falls freely from the top of a to...

A body falls freely from the top of a tower. It covers 36% of the total height in the lkast second before striking the ground level. The height of the tower is

A

50 m

B

75 m

C

100 m

D

125 m

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To solve the problem of a body falling freely from the top of a tower and covering 36% of the total height in the last second before striking the ground, we can follow these steps: ### Step-by-Step Solution: 1. **Define Variables**: Let the total height of the tower be \( H \). According to the problem, the body covers 36% of the total height in the last second. Therefore, the distance covered in the last second is: \[ d = 0.36H \] 2. **Calculate Distance Covered Before the Last Second**: The distance covered before the last second (i.e., in \( T - 1 \) seconds) is: \[ d' = H - d = H - 0.36H = 0.64H \] 3. **Use the Equation of Motion**: The distance covered in \( T - 1 \) seconds can be expressed using the second equation of motion: \[ d' = \frac{1}{2} g (T - 1)^2 \] Substituting \( d' \): \[ 0.64H = \frac{1}{2} g (T - 1)^2 \] 4. **Express Total Height Using Time \( T \)**: The total height \( H \) can also be expressed using the second equation of motion for \( T \) seconds: \[ H = \frac{1}{2} g T^2 \] 5. **Substitute \( H \) in the Distance Equation**: Substitute \( H \) from the previous equation into the distance equation: \[ 0.64 \left(\frac{1}{2} g T^2\right) = \frac{1}{2} g (T - 1)^2 \] Simplifying this gives: \[ 0.32 g T^2 = \frac{1}{2} g (T^2 - 2T + 1) \] 6. **Cancel \( g \) and Rearrange**: Since \( g \) is common on both sides, we can cancel it: \[ 0.32 T^2 = \frac{1}{2} (T^2 - 2T + 1) \] Multiplying through by 2 to eliminate the fraction: \[ 0.64 T^2 = T^2 - 2T + 1 \] Rearranging gives: \[ 0 = T^2 - 2T + 1 - 0.64 T^2 \] \[ 0 = 0.36 T^2 - 2T + 1 \] 7. **Multiply by 100 to Simplify**: To eliminate decimals, multiply the entire equation by 100: \[ 36 T^2 - 200 T + 100 = 0 \] 8. **Use the Quadratic Formula**: Applying the quadratic formula \( T = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} \): Here, \( a = 36 \), \( b = -200 \), and \( c = 100 \): \[ T = \frac{200 \pm \sqrt{(-200)^2 - 4 \cdot 36 \cdot 100}}{2 \cdot 36} \] \[ T = \frac{200 \pm \sqrt{40000 - 14400}}{72} \] \[ T = \frac{200 \pm \sqrt{25600}}{72} \] \[ T = \frac{200 \pm 160}{72} \] This gives two possible values for \( T \): \[ T = \frac{360}{72} = 5 \quad \text{(valid time)} \] \[ T = \frac{40}{72} \quad \text{(not valid since time cannot be negative)} \] 9. **Calculate the Height of the Tower**: Now that we have \( T = 5 \) seconds, we can find the height \( H \): \[ H = \frac{1}{2} g T^2 \] Assuming \( g = 10 \, \text{m/s}^2 \): \[ H = \frac{1}{2} \cdot 10 \cdot (5^2) = \frac{1}{2} \cdot 10 \cdot 25 = 125 \, \text{meters} \] ### Final Answer: The height of the tower is \( 125 \, \text{meters} \). ---

To solve the problem of a body falling freely from the top of a tower and covering 36% of the total height in the last second before striking the ground, we can follow these steps: ### Step-by-Step Solution: 1. **Define Variables**: Let the total height of the tower be \( H \). According to the problem, the body covers 36% of the total height in the last second. Therefore, the distance covered in the last second is: \[ d = 0.36H ...
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