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A particle is dropped from height h = 10...

A particle is dropped from height `h = 100 m`, from surface of a planet. If in last `1/2` sec of its journey it covers 19 m. Then value of acceleration due to gravity that planet is :

A

`8 m/s^2`

B

`1/8 m/s^2`

C

`1/4 m/s^2`

D

`2 m/s^2`

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To solve the problem step by step, we will use the equations of motion under uniform acceleration. ### Step 1: Understand the problem A particle is dropped from a height of \( h = 100 \, \text{m} \). We need to find the acceleration due to gravity \( g \) on the planet, given that the particle covers \( 19 \, \text{m} \) in the last \( \frac{1}{2} \) second of its fall. ### Step 2: Define the variables Let: - \( g \) = acceleration due to gravity on the planet (what we need to find) - \( t \) = total time taken to fall from height \( h \) - The distance covered in the last \( \frac{1}{2} \) second is \( s_{last} = 19 \, \text{m} \). ### Step 3: Use the equations of motion 1. The total distance fallen in time \( t \) is given by: \[ h = \frac{1}{2} g t^2 \] Therefore, we can write: \[ 100 = \frac{1}{2} g t^2 \quad \text{(1)} \] 2. The distance fallen in the last \( \frac{1}{2} \) second can be calculated using the formula: \[ s_{last} = s(t) - s(t - \frac{1}{2}) \] where \( s(t) = \frac{1}{2} g t^2 \) and \( s(t - \frac{1}{2}) = \frac{1}{2} g (t - \frac{1}{2})^2 \). Thus, we have: \[ s_{last} = \frac{1}{2} g t^2 - \frac{1}{2} g (t - \frac{1}{2})^2 \] Simplifying gives: \[ s_{last} = \frac{1}{2} g \left[ t^2 - (t^2 - t + \frac{1}{4}) \right] = \frac{1}{2} g \left[ t - \frac{1}{4} \right] \] Setting \( s_{last} = 19 \): \[ 19 = \frac{1}{2} g \left[ t - \frac{1}{4} \right] \quad \text{(2)} \] ### Step 4: Solve the equations From equation (1): \[ g = \frac{200}{t^2} \quad \text{(3)} \] Substituting equation (3) into equation (2): \[ 19 = \frac{1}{2} \left(\frac{200}{t^2}\right) \left[ t - \frac{1}{4} \right] \] This simplifies to: \[ 19 = 100 \left(\frac{t - \frac{1}{4}}{t^2}\right) \] Rearranging gives: \[ 19 t^2 = 100 \left(t - \frac{1}{4}\right) \] Expanding and rearranging: \[ 19 t^2 = 100t - 25 \] \[ 19 t^2 - 100t + 25 = 0 \] ### Step 5: Use the quadratic formula Using the quadratic formula \( t = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} \): Here, \( a = 19, b = -100, c = 25 \): \[ t = \frac{100 \pm \sqrt{(-100)^2 - 4 \cdot 19 \cdot 25}}{2 \cdot 19} \] Calculating the discriminant: \[ 10000 - 1900 = 8100 \] Thus, \[ t = \frac{100 \pm 90}{38} \] Calculating the two possible values: 1. \( t = \frac{190}{38} = 5 \) 2. \( t = \frac{10}{38} = \frac{5}{19} \) (not physically meaningful as time cannot be negative) ### Step 6: Calculate \( g \) Substituting \( t = 5 \) into equation (3): \[ g = \frac{200}{5^2} = \frac{200}{25} = 8 \, \text{m/s}^2 \] ### Final Answer The acceleration due to gravity on the planet is \( g = 8 \, \text{m/s}^2 \). ---

To solve the problem step by step, we will use the equations of motion under uniform acceleration. ### Step 1: Understand the problem A particle is dropped from a height of \( h = 100 \, \text{m} \). We need to find the acceleration due to gravity \( g \) on the planet, given that the particle covers \( 19 \, \text{m} \) in the last \( \frac{1}{2} \) second of its fall. ### Step 2: Define the variables Let: - \( g \) = acceleration due to gravity on the planet (what we need to find) ...
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