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At a height of 15 m from ground velocity...

At a height of 15 m from ground velocity of a projectile is `v = (10hati+ 10hatj)`. Here `hatj` is vertically upwards and `hati` is along horizontal direction then (g = 10 `ms^(-1)`)

A

particle was projected at an angle of `45^@` with horizontal.

B

time of flight of projectile is 4 s

C

horizontal range of projectile is 100 m

D

maximum height of projectile from ground is 20 m.

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To solve the problem, we need to analyze the projectile motion of the object at a height of 15 m. The velocity at this height is given as \( \vec{v} = 10 \hat{i} + 10 \hat{j} \) m/s, where \( \hat{i} \) is the horizontal direction and \( \hat{j} \) is the vertical direction. The acceleration due to gravity \( g \) is given as \( 10 \, \text{m/s}^2 \). ### Step 1: Identify the components of the velocity The velocity of the projectile at the height of 15 m can be broken down into its horizontal and vertical components: - Horizontal component \( v_x = 10 \, \text{m/s} \) - Vertical component \( v_y = 10 \, \text{m/s} \) ### Step 2: Relate the horizontal component to the initial velocity Since there is no acceleration in the horizontal direction, the horizontal component of the initial velocity \( u \cos \theta \) remains constant throughout the motion: \[ u \cos \theta = v_x = 10 \, \text{m/s} \] ### Step 3: Use the vertical motion equation For the vertical motion, we can use the third equation of motion: \[ v_y^2 = u_y^2 - 2g h \] Where: - \( v_y = 10 \, \text{m/s} \) (final vertical velocity) - \( u_y = u \sin \theta \) (initial vertical velocity) - \( g = 10 \, \text{m/s}^2 \) (acceleration due to gravity) - \( h = 15 \, \text{m} \) (height) Substituting the known values: \[ 10^2 = (u \sin \theta)^2 - 2 \cdot 10 \cdot 15 \] \[ 100 = (u \sin \theta)^2 - 300 \] \[ (u \sin \theta)^2 = 400 \] \[ u \sin \theta = 20 \, \text{m/s} \] ### Step 4: Calculate the angle of projection Now we have both components of the initial velocity: - \( u \cos \theta = 10 \) - \( u \sin \theta = 20 \) We can find the angle of projection \( \theta \) using the tangent function: \[ \tan \theta = \frac{u \sin \theta}{u \cos \theta} = \frac{20}{10} = 2 \] Thus, \[ \theta = \tan^{-1}(2) \] ### Step 5: Calculate the time of flight The time of flight \( T \) can be calculated using the formula: \[ T = \frac{2 u \sin \theta}{g} \] Substituting the known values: \[ T = \frac{2 \cdot 20}{10} = 4 \, \text{s} \] ### Step 6: Calculate the range The range \( R \) can be calculated as: \[ R = u_x \cdot T \] Where \( u_x = u \cos \theta = 10 \, \text{m/s} \): \[ R = 10 \cdot 4 = 40 \, \text{m} \] ### Step 7: Calculate the maximum height The maximum height \( H \) can be calculated using: \[ H = \frac{(u \sin \theta)^2}{2g} \] Substituting the known values: \[ H = \frac{20^2}{2 \cdot 10} = \frac{400}{20} = 20 \, \text{m} \] ### Summary of Results - Angle of projection \( \theta = \tan^{-1}(2) \) - Time of flight \( T = 4 \, \text{s} \) - Range \( R = 40 \, \text{m} \) - Maximum height \( H = 20 \, \text{m} \)

To solve the problem, we need to analyze the projectile motion of the object at a height of 15 m. The velocity at this height is given as \( \vec{v} = 10 \hat{i} + 10 \hat{j} \) m/s, where \( \hat{i} \) is the horizontal direction and \( \hat{j} \) is the vertical direction. The acceleration due to gravity \( g \) is given as \( 10 \, \text{m/s}^2 \). ### Step 1: Identify the components of the velocity The velocity of the projectile at the height of 15 m can be broken down into its horizontal and vertical components: - Horizontal component \( v_x = 10 \, \text{m/s} \) - Vertical component \( v_y = 10 \, \text{m/s} \) ### Step 2: Relate the horizontal component to the initial velocity ...
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