Porisma

Original question & working

Two launch angles for an approaching target · source reference

Not printed in supplied question · Question pp. 4 · Working pp. 16, 17

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The working and teaching notes are included in the interactive lesson.

Use degree mode for this model. The approaching target travels towards the origin, so its distance decreases.

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Printed question

The diagram shows the trajectory of a cannonball fired off from an origin OO with an initial speed of v m s−1v\,\mathrm{m\,s^{-1}} and at an angle of θ∘\theta^\circ above the ground. At time tt seconds, its position can be modelled by x=(vcos⁡θ)tx=(v\cos\theta)t, y=(vsin⁡θ)t−5t2y=(v\sin\theta)t-5t^2, where xx m is horizontal distance with respect to OO and yy m is vertical distance with respect to ground level.

(i) Find the horizontal distance, dd m, that a cannonball would have travelled by the time it hits the ground. Leave your answer in terms of vv and θ\theta. [4]

Use v=200v=200 to answer the remaining parts. An approaching target is travelling at a constant speed of 10 m s−110\,\mathrm{m\,s^{-1}} along the ground. A cannonball is fired towards it when it is 3000 m away. You may assume its height is negligible.

(ii) Show that in order to hit the target, the possible angles at which the cannonball should be fired are 22.7∘22.7^\circ and 69.5∘69.5^\circ. [2]

(iii) Explain at which angle the cannonball should be fired in order to hit the target earlier. [2]

(iv) Given θ=22.7\theta=22.7, find the angle that the tangent to the trajectory makes with the horizontal when x=370x=370. [4]

Printed working

(i) To determine the range consider y=0y=0: (vsin⁡θ)t−5t2=0⇒t[vsin⁡θ−5t]=0(v\sin\theta)t-5t^2=0\Rightarrow t[v\sin\theta-5t]=0.

t=0t=0 is rejected as the starting point; otherwise vsin⁡θ−5t=0⇒t=vsin⁡θ/5v\sin\theta-5t=0\Rightarrow t=v\sin\theta/5.

At this time x=dx=d, so d=(vcos⁡θ)(vsin⁡θ/5)=v2sin⁡θcos⁡θ/5d=(v\cos\theta)(v\sin\theta/5)=v^2\sin\theta\cos\theta/5.

(ii) Time for cannonball to hit ground equals time for target to reach impact:

vsin⁡θ5=3000−d10⇒2vsin⁡θ=3000−v2sin⁡θcos⁡θ5.\frac{v\sin\theta}{5}=\frac{3000-d}{10}\Rightarrow2v\sin\theta=3000-\frac{v^2\sin\theta\cos\theta}{5}.

Given v=200v=200, (200)2sin⁡θcos⁡θ/5+400sin⁡θ=3000(200)^2\sin\theta\cos\theta/5+400\sin\theta=3000. GC gives 22.7∘22.7^\circ or 69.5∘69.5^\circ (1 d.p.; shown).

(iii) Since t=vsin⁡θ/5t=v\sin\theta/5 and vsin⁡22.7∘/5<vsin⁡69.5∘/5v\sin22.7^\circ/5<v\sin69.5^\circ/5 for v>0v>0, fire at 22.7∘22.7^\circ to hit earlier.

(iv) x=(200cos⁡22.7∘)tx=(200\cos22.7^\circ)t, y=(200sin⁡22.7∘)t−5t2y=(200\sin22.7^\circ)t-5t^2. Thus dx/dt=184.51dx/dt=184.51, dy/dt=77.181−10tdy/dt=77.181-10t, dy/dx=(77.181−10t)/184.51dy/dx=(77.181-10t)/184.51.

When x=370x=370, 184.51t=370⇒t=2.0053184.51t=370\Rightarrow t=2.0053; dy/dx=(77.181−10(2.0053))/184.51=0.30962dy/dx=(77.181-10(2.0053))/184.51=0.30962.

Let required angle be α\alpha: tan⁡α=0.30962⇒α=17.2∘\tan\alpha=0.30962\Rightarrow\alpha=17.2^\circ (1 d.p.).

Teacher notes

When the cannonball hits ground, y=0y=0.

Time =distance/speed=\text{distance}/\text{speed}. The same flight time is the target’s travel time over distance 3000−d3000-d.

Answer key

(i) v2sin⁡θcos⁡θ/5v^2\sin\theta\cos\theta/5. (iii) 22.7∘22.7^\circ. (iv) 17.2∘17.2^\circ (1 d.p.). No examination attribution is printed for this group.

Native diagrams

Original trajectory schematic: O, θ°, x and y, cannonball(x,y), Ground. Solution schematic: trajectory, approaching target(10m/s), d m, 3000 m and Ground.