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A particle is projected with a speed u. ...

A particle is projected with a speed u. If after 2 seconds of projection it is found to be making an angle of `45^@` with the horizontal and `0^@` after 3 sec, then:

A

Angle of projection is `tan^(-1) 3`

B

Angle of projection is `tan^(-1) (1//3)`

C

Speed of projection `= 30 sqrt2m//s`

D

Speed of projection is 30 m/s

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To solve the problem step by step, we will analyze the motion of the particle projected at an angle and use the information given about its velocity at specific times. ### Step 1: Understand the components of motion The particle is projected with an initial speed \( u \) at an angle \( \theta \). The initial velocity can be broken down into horizontal and vertical components: - Horizontal component: \( u_x = u \cos \theta \) - Vertical component: \( u_y = u \sin \theta \) ### Step 2: Analyze the vertical motion at \( t = 3 \) seconds At \( t = 3 \) seconds, the particle is at an angle of \( 0^\circ \) with the horizontal, which means its vertical component of velocity \( v_y \) is \( 0 \): \[ v_y = u_y - g t = 0 \] Substituting \( t = 3 \) seconds: \[ u \sin \theta - g \cdot 3 = 0 \] Rearranging gives: \[ u \sin \theta = 3g \] Using \( g \approx 10 \, \text{m/s}^2 \): \[ u \sin \theta = 30 \, \text{m/s} \quad \text{(1)} \] ### Step 3: Analyze the vertical motion at \( t = 2 \) seconds At \( t = 2 \) seconds, the angle with the horizontal is \( 45^\circ \). The tangent of the angle is given by: \[ \tan(45^\circ) = 1 = \frac{v_y}{u_x} \] The vertical component of velocity at \( t = 2 \) seconds is: \[ v_y = u \sin \theta - g \cdot 2 = u \sin \theta - 20 \] Setting this equal to \( u \cos \theta \) (since \( \tan(45^\circ) = 1 \)): \[ u \sin \theta - 20 = u \cos \theta \] Rearranging gives: \[ u \sin \theta - u \cos \theta = 20 \] Factoring out \( u \): \[ u (\sin \theta - \cos \theta) = 20 \quad \text{(2)} \] ### Step 4: Solve the equations Now we have two equations: 1. \( u \sin \theta = 30 \) 2. \( u (\sin \theta - \cos \theta) = 20 \) From equation (1), we can express \( \sin \theta \): \[ \sin \theta = \frac{30}{u} \] Substituting this into equation (2): \[ u \left(\frac{30}{u} - \cos \theta\right) = 20 \] This simplifies to: \[ 30 - u \cos \theta = 20 \] Thus: \[ u \cos \theta = 10 \quad \text{(3)} \] ### Step 5: Find \( \tan \theta \) Now we have: - From (1): \( u \sin \theta = 30 \) - From (3): \( u \cos \theta = 10 \) Now we can find \( \tan \theta \): \[ \tan \theta = \frac{u \sin \theta}{u \cos \theta} = \frac{30}{10} = 3 \] Thus: \[ \theta = \tan^{-1}(3) \] ### Step 6: Find the initial speed \( u \) To find \( u \), we can use the Pythagorean theorem: \[ u^2 = (u \sin \theta)^2 + (u \cos \theta)^2 \] Substituting the values: \[ u^2 = 30^2 + 10^2 = 900 + 100 = 1000 \] Thus: \[ u = \sqrt{1000} = 10\sqrt{10} \, \text{m/s} \] ### Final Answers - The angle of projection \( \theta = \tan^{-1}(3) \) - The speed of projection \( u = 10\sqrt{10} \, \text{m/s} \)

To solve the problem step by step, we will analyze the motion of the particle projected at an angle and use the information given about its velocity at specific times. ### Step 1: Understand the components of motion The particle is projected with an initial speed \( u \) at an angle \( \theta \). The initial velocity can be broken down into horizontal and vertical components: - Horizontal component: \( u_x = u \cos \theta \) - Vertical component: \( u_y = u \sin \theta \) ### Step 2: Analyze the vertical motion at \( t = 3 \) seconds ...
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