Solveeit Logo

Question

Question: A projectile is projected with velocity of 40 m/s at an angle $\theta$ with the horizontal. If $R$ b...

A projectile is projected with velocity of 40 m/s at an angle θ\theta with the horizontal. If RR be the horizontal range covered by the projectile and after tt seconds, its inclination with horizontal becomes zero, then the value of cotθ\cot \theta is [Take, g=10g=10 m/s2^2]

A

R20t2\frac{R}{20t^2}

B

R10t2\frac{R}{10t^2}

C

5Rt2\frac{5R}{t^2}

D

Rt2\frac{R}{t^2}

Answer

R20t2\frac{R}{20t^2}

Explanation

Solution

The projectile is projected with an initial velocity u=40u = 40 m/s at an angle θ\theta with the horizontal.

The velocity components are ux=ucosθ=40cosθu_x = u \cos \theta = 40 \cos \theta and uy=usinθ=40sinθu_y = u \sin \theta = 40 \sin \theta.

The acceleration due to gravity is g=10g = 10 m/s2^2 downwards.

The inclination of the projectile with the horizontal becomes zero at the highest point of its trajectory. The vertical component of velocity is zero at this point.

Let tt be the time taken to reach the highest point. The vertical velocity at time tt is given by vy(t)=uygtv_y(t) = u_y - gt.

At tt, vy(t)=0v_y(t) = 0.

So, 0=usinθgt0 = u \sin \theta - gt

usinθ=gtu \sin \theta = gt

Substituting u=40u = 40 and g=10g = 10:

40sinθ=10t40 \sin \theta = 10t

sinθ=10t40=t4\sin \theta = \frac{10t}{40} = \frac{t}{4} (Equation 1)

The horizontal range RR is the horizontal distance covered by the projectile when it returns to the initial height. The time taken for this is the total time of flight, which is twice the time taken to reach the highest point.

Total time of flight T=2tT = 2t.

The horizontal range is given by R=ux×TR = u_x \times T.

R=(ucosθ)×(2t)R = (u \cos \theta) \times (2t)

Substituting u=40u = 40:

R=(40cosθ)×(2t)R = (40 \cos \theta) \times (2t)

R=80tcosθR = 80t \cos \theta (Equation 2)

We need to find the value of cotθ\cot \theta. We know that cotθ=cosθsinθ\cot \theta = \frac{\cos \theta}{\sin \theta}.

From Equation 1, we have sinθ=t4\sin \theta = \frac{t}{4}.

From Equation 2, we have cosθ=R80t\cos \theta = \frac{R}{80t}.

Now, we can find cotθ\cot \theta:

cotθ=cosθsinθ=R80tt4\cot \theta = \frac{\cos \theta}{\sin \theta} = \frac{\frac{R}{80t}}{\frac{t}{4}}

cotθ=R80t×4t\cot \theta = \frac{R}{80t} \times \frac{4}{t}

cotθ=4R80t2\cot \theta = \frac{4R}{80t^2}

cotθ=R20t2\cot \theta = \frac{R}{20t^2}