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A body dropped from the top of a tower c...

A body dropped from the top of a tower covers 7/16 of the total height in the last second of its fall. The time of fall is

A

`2sec`

B

`4sec`

C

`1sec`

D

`((50)/(7))sec`

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To solve the problem, we need to find the time of fall \( t \) for a body dropped from the top of a tower, given that it covers \( \frac{7}{16} \) of the total height in the last second of its fall. ### Step 1: Understand the problem Let the total height of the tower be \( h \). The body is dropped from the top, so the initial velocity \( u = 0 \). The distance covered in the last second of the fall is given as \( \frac{7}{16} h \). ### Step 2: Use the equations of motion The distance covered in \( t \) seconds is given by the equation: \[ h = ut + \frac{1}{2}gt^2 \] Since \( u = 0 \), this simplifies to: \[ h = \frac{1}{2}gt^2 \] ### Step 3: Distance covered in the last second The distance covered in the last second (from \( t-1 \) to \( t \)) can be expressed as: \[ \text{Distance in last second} = h - \text{Distance covered in } (t-1) \text{ seconds} \] The distance covered in \( t-1 \) seconds is: \[ h_{t-1} = \frac{1}{2}g(t-1)^2 \] Thus, the distance covered in the last second is: \[ \text{Distance in last second} = h - h_{t-1} = \frac{1}{2}gt^2 - \frac{1}{2}g(t-1)^2 \] ### Step 4: Set up the equation Now we can set up the equation based on the information that the distance covered in the last second is \( \frac{7}{16}h \): \[ \frac{1}{2}gt^2 - \frac{1}{2}g(t-1)^2 = \frac{7}{16}h \] Substituting \( h = \frac{1}{2}gt^2 \) into the equation gives: \[ \frac{1}{2}gt^2 - \frac{1}{2}g(t-1)^2 = \frac{7}{16} \left(\frac{1}{2}gt^2\right) \] ### Step 5: Simplify the equation Expanding \( (t-1)^2 \): \[ (t-1)^2 = t^2 - 2t + 1 \] Thus, \[ \frac{1}{2}gt^2 - \frac{1}{2}g(t^2 - 2t + 1) = \frac{7}{32}gt^2 \] This simplifies to: \[ \frac{1}{2}g(2t - 1) = \frac{7}{32}gt^2 \] Cancelling \( g \) (assuming \( g \neq 0 \)): \[ t - \frac{1}{2} = \frac{7}{16}t^2 \] ### Step 6: Rearranging the equation Rearranging gives: \[ \frac{7}{16}t^2 - t + \frac{1}{2} = 0 \] Multiplying through by 16 to eliminate the fraction: \[ 7t^2 - 16t + 8 = 0 \] ### Step 7: Solve the quadratic equation Using the quadratic formula \( t = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} \): Here \( a = 7, b = -16, c = 8 \): \[ t = \frac{16 \pm \sqrt{(-16)^2 - 4 \cdot 7 \cdot 8}}{2 \cdot 7} \] Calculating the discriminant: \[ t = \frac{16 \pm \sqrt{256 - 224}}{14} = \frac{16 \pm \sqrt{32}}{14} = \frac{16 \pm 4\sqrt{2}}{14} \] Simplifying gives: \[ t = \frac{8 \pm 2\sqrt{2}}{7} \] ### Step 8: Finding the positive root Since time cannot be negative, we take the positive root: \[ t = \frac{8 + 2\sqrt{2}}{7} \] Calculating this gives approximately \( t \approx 4 \) seconds. ### Conclusion The time of fall \( t \) is approximately \( 4 \) seconds.

To solve the problem, we need to find the time of fall \( t \) for a body dropped from the top of a tower, given that it covers \( \frac{7}{16} \) of the total height in the last second of its fall. ### Step 1: Understand the problem Let the total height of the tower be \( h \). The body is dropped from the top, so the initial velocity \( u = 0 \). The distance covered in the last second of the fall is given as \( \frac{7}{16} h \). ### Step 2: Use the equations of motion The distance covered in \( t \) seconds is given by the equation: \[ ...
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RESONANCE ENGLISH-DAILY PRACTICE PROBLEM-DPP No.11
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