Kinematics problem from JEE advanced

The speed of a projectile when it is at its greatest height is 2 5 \sqrt{\frac{2}{5}} times its speed at half the maximum height. Find the angle of projection (in degrees).


The answer is 60.

This section requires Javascript.
You are seeing this because something didn't load right. We suggest you, (a) try refreshing the page, (b) enabling javascript if it is disabled on your browser and, finally, (c) loading the non-javascript version of this page . We're sorry about the hassle.

3 solutions

Gokul Kumar
Jun 24, 2015

Initial speed of the projectile = U.; Horizontal component = Ux, Vertical compnent = Uy

Angle of inclination with the horizontal = angle of projection = θ Ux = U cos θ and Uy = U sin θ => U² = (Ux)² + (Uy)²

When it is at any height h : Speed = V ; Horizontal component = Vx, Vertical component = Vy Vx = Ux , => (Vx)² = (Ux)² ; (Vy)² = (Uy)² - 2gh

V² = (Vx)² + (Vy)² = (Ux)² + (Uy)² - 2gh = U² - 2gh ......... (1)

At maximum height : h = H and V = V1 , => (V1)² = U² - 2g H ...... (2)

At half the maximum height : h = H/2 and V = V2, => (V2)² = U² - gH ........ (3)

As per the question, (V1)² / (V2)² = (U² - 2gH) / (U² - gH) = (2 / 5) => 5U² - 10gH = 2U² - 2gH => 3U² = 8gH => U² = (8gH / 3) ........ (4)

Again, at maximum height, (V1)x = Ux = U cos θ and (V1)y = 0 => (V1)² = U² cos² θ = U² - 2gH [ from (2) ] => U² ( 1 - cos² θ ) = 2gH = U² sin² θ = 2gH ......... (5)

Dividing (5) by (4) , sin² θ = (2*3) / 8 = 6/8 = 3/4 => sin θ = √3 / 2 , => θ = 60 deg

Sorry but according to your solution :

(V1)² / (V2)² = (U² - 2gH) / (U² - gH) = (2 / 5) (as you have written)

so this means that the speed of a projectile when it is at its greatest height is (2/5)^0.5 times its speed at half the maximum height., instead of (2^0.5)/5 as you have written. Pls take care while writing questions.

Shivam Saxena - 5 years, 11 months ago

Log in to reply

oh ya srry

Gokul Kumar - 5 years, 11 months ago

Log in to reply

Np . It happens all the time :)

Shivam Saxena - 5 years, 11 months ago

Could you use the Latex please..., It will make your solution more interesting

Resha Dwika Hefni Al-Fahsi - 5 years, 3 months ago
Romeo Gomez
Nov 19, 2018

The vectorial equation of the particle is r ( t ) = v 0 cos θ i + v 0 sin θ t 1 2 g t 2 j , r(t)=v_0\cos \theta \textbf{i}+v_0\sin \theta t-\frac{1}{2}gt^2\textbf{j}, the speed is r ( t ) ||r'(t)|| at time t t .\ So the greatest height comes when t = v 0 sin θ g , t=\frac{v_0 \sin \theta}{g}, let's denote the greatest high with t m a x t_{max} r ( t m a x ) = v 0 2 sin θ cos θ g i + v 0 2 sin 2 θ 2 g j , r(t_{max})=\frac{v_0^2\sin \theta \cos \theta}{g}\textbf{i}+\frac{v_0^2\sin^2 \theta }{2g}\textbf{j}, so the half of the greatest heigh is H a l f H e i g h t = v 0 2 sin 2 θ 4 g , HalfHeight=\frac{v_0^2\sin^2 \theta }{4g}, we just need to find when r ( t ) = H a l f H e i g h t r(t)=HalfHeight and that occurs when \ t m a x h a l f = ( 1 2 2 ) v 0 sin θ g t_{maxhalf}=(1-\frac{\sqrt{2}}{2})\frac{v_0\sin \theta }{g} . Now we can replace the value of t m a x h a l f t_{maxhalf} in the speed r ( t m a x h a l f ) = v 0 1 + cos 2 θ 2 , ||r'(t_{maxhalf})||=v_0\sqrt{\frac{1+\cos^2 \theta}{2}}, but the speed of the projectile when it is at its greatest height is 2 5 \sqrt{\frac{2}{5}} times its speed at half of the maximum height. So we get the equation v 0 cos θ = 2 5 v 0 1 + cos 2 θ 2 v_0\cos \theta=\sqrt{\frac{2}{5}}v_0\sqrt{\frac{1+\cos^2 \theta}{2}}

cos θ = 1 + cos 2 θ 5 \cos \theta=\sqrt{\frac{1+\cos^2 \theta}{5}}

cos 2 θ = 1 + cos 2 θ 5 \cos^2\theta=\frac{1+\cos^2 \theta}{5} 5 cos 2 θ = 1 + cos 2 θ 5\cos^2\theta=1+\cos^2 \theta cos 2 θ = 1 4 \cos^2\theta=\frac{1}{4} cos θ = 1 2 \cos\theta=\frac{1}{2} so θ = 6 0 \boxed{\theta=60^\circ}

Venkatesh K
Jun 30, 2015

In this question, if the factor is 2 5 \frac{\sqrt{2}}{5} , then On solving , we get sin θ \sin \theta = 46 7 \frac{\sqrt{46}}{7} . If the multiplying factor is 2 / 5 \sqrt{2/5} , then we get value of θ \theta as 60.

Yes, I just realised this.This is how I did it using the method of conservation of mechanical energy, but would like to know if my approach is correct:

Let θ be the angle the launch speed vector makes with the horizontal, A the point at which the projectile is launched, B the greatest height of projection from the level of projection, O the mid point between the levels on which A and B are located, u its speed at A, x its speed at O, (u cosθ) its speed at B and v its speed at any given point of its trajectory.

(u cosθ)= √ (2/5)x

Δv² between A and B= u²-(u cosθ)²

Δv² between A and O= u²-x²= u²-(5/2)(u cosθ)²

Δv² between A and B= 2(Δv² between A and O)

So u²-(u cosθ)²= 2[u²-(5/2)(u cosθ)²]

u²-(u cosθ)²= 2u²-5(u cosθ)²

4u²(cosθ)²= u²

Since u≠ 0, we can divide both sides of the last equation by u², giving us:

4(cosθ)²= 1

(cosθ)²= 1/4

cosθ= 1/2 [-1/2 is not considered since θ is an acute angle]

Thus, θ= arccos(1/2)= 60°.

Is this how this problem could be approached?

Aran Pasupathy - 5 years, 11 months ago

0 pending reports

×

Problem Loading...

Note Loading...

Set Loading...