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M7.5

Model motion under gravity in a vertical plane using vectors; projectiles.

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Projectiles

Worked answers and methods for M7.5 on Edexcel A-level Maths 9MA0.

Definition

Specification M7.5: model motion under gravity in a vertical plane using vectors; projectiles. A projectile is modelled as a particle moving freely under gravity, so its horizontal acceleration is zero and its vertical acceleration is gg downwards.

Explanation

  • Resolve the initial velocity into ucos⁡αu\cos\alpha horizontally and usin⁡αu\sin\alpha vertically, then treat the two directions separately with the constant-acceleration formulae: horizontally x=ucos⁡α tx=u\cos\alpha\,t; vertically y=usin⁡α t−12gt2y=u\sin\alpha\,t-\tfrac12gt^2 with upwards positive. Eliminating tt gives the equation of the path, y=xtan⁡α−gx22u2cos⁡2αy=x\tan\alpha-\dfrac{gx^2}{2u^2\cos^2\alpha}, which is derived every time it is used, never quoted.
  • Time of flight to the same level comes from y=0y=0; range from substituting that time into xx; greatest height from the vertical velocity being zero, 0=(usin⁡α)2−2gh0=(u\sin\alpha)^2-2gh, while the horizontal velocity is unchanged there.
  • Speed at any instant combines both components by Pythagoras.
  • State the value of gg used, 9.89.8 unless told otherwise, and give answers to two or three significant figures.
  • Limitations of the model that score are air resistance, spin, wind, size and shape of the object, and treating gg as constant.
A projectile is resolved into horizontal ucos⁡θu\cos\theta and vertical usin⁡θu\sin\theta components.

Worked example

1.

A ball is projected from a point OO on horizontal ground with speed 2020 m s−1^{-1} at an angle of 30∘30^\circ above the horizontal. The ball is modelled as a particle moving freely under gravity. Find the horizontal distance from OO to the point where the ball first hits the ground.

(4)

(Total for Question 1 is 4 marks)

Working

  1. 1.Resolve the initial velocity: horizontally 20cos⁡30∘=10320\cos30^\circ=10\sqrt3 m s−1^{-1}, vertically 20sin⁡30∘=1020\sin30^\circ=10 m s−1^{-1}.
  2. 2.Vertically, taking upwards as positive, s=ut+12at2s=ut+\tfrac12at^2 with s=0s=0: 0=10t−4.9t20=10t-4.9t^2, so t=104.9=2.04t=\dfrac{10}{4.9}=2.04 s.
  3. 3.Horizontally there is no acceleration: x=103×104.9=35.3x=10\sqrt3\times\dfrac{10}{4.9}=35.3 m.

Answer: 3535 m (to 2 s.f.); 35.335.3 m to 3 s.f.

Mark scheme

Mark scheme for question 1
QuestionSchemeMarks
1.Vertical motion with s=0s=0: 0=20sin⁡30∘ t−12(9.8)t20=20\sin30^\circ\,t-\tfrac12(9.8)t^2M1
t=104.9t=\dfrac{10}{4.9} or 2.042.04 sA1
Horizontal motion x=20cos⁡30∘×x=20\cos30^\circ\times their ttM1
3535 or 35.335.3 mA1
Notes
M1: Condone sign errors; g=9.8g=9.8 used
A1: awrt 35

(4 marks)

Common mistakes

  • Don't use a same-level horizontal-range formula for a projectile that lands at a different vertical level.
  • Don't use the full launch speed in both directions instead of resolving it into horizontal and vertical components.

Mark-scheme wording to use

  • “Using horizontal motion, s = ut, with 35 resolved … M1 … x = 35cos α × t … A1 … Using vertical motion, s = ut + (1/2)at², with 35 resolved … M1 … y = 35sin α × t − (1/2)gt² … A1 … Eliminate t : y = 35sin α × x/(35cos α) − (1/2)g(x/(35cos α))² … DM1 … A1* Given answer correctly obtained, with at least one further line of working with trig ratios and g = 9.8 explicitly seen or 4.9 oe used for 0.5g” — Pearson 9MA0, June 2024 Paper 32, Q5(a)
  • “M1 ALT 1: Use of y = 0 in equation of path and solve for x. … (OA = )120 (m) … A1 cao” — Pearson 9MA0, June 2024 Paper 32, Q5(b)
  • “B1 Any single correct answer. Acceptable answer: the inaccuracy of using 9.8 m s⁻² for g or wind or weather effects or the spin of the stone or the size (or shape or surface area) of the stone oe or the stone is still modelled as a particle … Unacceptable answers: The model (it) does not take account of: the mass or weight of the stone … air resistance.” — Pearson 9MA0, June 2024 Paper 32, Q5(e)

What the examiner wants

The path derived from components, with g=9.8g=9.8 visible. The June 2024 Paper 32 report says the final mark of the show-that required 9.89.8 to be seen used explicitly, that quoting the general trajectory equation and substituting the angle achieved no credit, and that some found the greatest height but gave 6060, the xx-value, instead of 22.522.5.

Exam tip

Resolve the initial velocity first, use zero vertical displacement for same-level flight, and keep horizontal acceleration zero.

Worked practice

Q1
Tier 1 · Easy

1.

A particle is projected vertically upwards at 14.7 m s−114.7\,\text{m s}^{-1}. Using g=9.8 m s−2g=9.8\,\text{m s}^{-2}, find the time taken to reach its greatest height and the height gained.

(4)

(Total for Question 1 is 4 marks)

Mark scheme

Mark scheme for question 1
QuestionSchemeMarks
1
  • Time =1.5 s=1.5\,\text{s}
  • Height gained =11.025 m=11.025\,\text{m}
4
Notes
Taking upwards as positive, v=u−gtv=u-gt. At greatest height v=0v=0, so 0=14.7−9.8t0=14.7-9.8t and t=1.5 st=1.5\,\text{s}. Then v2=u2+2asv^2=u^2+2as gives 0=14.72−2(9.8)s0=14.7^2-2(9.8)s, so s=11.025 ms=11.025\,\text{m}.

(4 marks)

Q2
Tier 2 · Standard

2.

A ball is projected horizontally at 12 m s−112\,\text{m s}^{-1} from a point 25 m25\,\text{m} above level ground. Using g=9.8 m s−2g=9.8\,\text{m s}^{-2} and ignoring air resistance, find the time taken to reach the ground and the horizontal distance travelled, each to 3 significant figures.

(4)

(Total for Question 2 is 4 marks)

Mark scheme

Mark scheme for question 2
QuestionSchemeMarks
2
  • Time =2.26 s=2.26\,\text{s}
  • Horizontal distance =27.1 m=27.1\,\text{m}
4
Notes
Vertically the initial velocity is zero, so 25=12(9.8)t225=\tfrac12(9.8)t^2. Hence t=50/9.8=2.2587… st=\sqrt{50/9.8}=2.2587\ldots\,\text{s}, which is 2.26 s2.26\,\text{s} to 3 significant figures. Horizontal velocity remains 12 m s−112\,\text{m s}^{-1}, so the horizontal distance is 12t=27.105… m12t=27.105\ldots\,\text{m}, or 27.1 m27.1\,\text{m} to 3 significant figures. Keep the unrounded tt on your calculator for that multiplication rather than retyping a rounded value.

(4 marks)

Q3
Tier 3 · Hard

3.

From a point 5 m5\,\text{m} above horizontal ground, a projectile is launched with velocity (12i+5j) m s−1(12\mathbf{i}+5\mathbf{j})\,\text{m s}^{-1}. Take j\mathbf{j} vertically upwards and use g=10 m s−2g=10\,\text{m s}^{-2}. Find the Cartesian equation of its path, the horizontal distance to its first impact with the ground, and its speed on impact.

(8)

(Total for Question 3 is 8 marks)

Mark scheme

Mark scheme for question 3
QuestionSchemeMarks
3
  • y=5+512x−5144x2y=5+\dfrac{5}{12}x-\dfrac{5}{144}x^2
  • Horizontal distance =6(1+5) m=6(1+\sqrt5)\,\text{m}
  • Impact speed =269 m s−1=\sqrt{269}\,\text{m s}^{-1}
8
Notes
x=12tx=12t and y=5+5t−5t2y=5+5t-5t^2. Substituting t=x/12t=x/12 gives y=5+5x/12−5x2/144y=5+5x/12-5x^2/144. At impact, 5+5t−5t2=05+5t-5t^2=0, so t=(1+5)/2t=(1+\sqrt5)/2 and x=12t=6(1+5) mx=12t=6(1+\sqrt5)\,\text{m}. The impact velocity is 12i+(5−10t)j=12i−55j12\mathbf{i}+(5-10t)\mathbf{j}=12\mathbf{i}-5\sqrt5\mathbf{j}, so its speed is 122+(55)2=269 m s−1\sqrt{12^2+(5\sqrt5)^2}=\sqrt{269}\,\text{m s}^{-1}.

(8 marks)

Q4
Tier 1 · Easy

4.

A particle is projected at 17 m s−117\,\text{m s}^{-1} at an angle θ\theta above the horizontal, where sin⁡θ=817\sin\theta=\dfrac{8}{17}. Find the horizontal and vertical components of its initial velocity.

(2)

(Total for Question 4 is 2 marks)

Mark scheme

Mark scheme for question 4
QuestionSchemeMarks
4
  • Horizontal component =15 m s−1=15\,\text{m s}^{-1}
  • Vertical component =8 m s−1=8\,\text{m s}^{-1} upwards
2
Notes
Since θ\theta is acute, cos⁡θ=15/17\cos\theta=15/17. Therefore the components are 17cos⁡θ=15 m s−117\cos\theta=15\,\text{m s}^{-1} horizontally and 17sin⁡θ=8 m s−117\sin\theta=8\,\text{m s}^{-1} vertically upwards.

(2 marks)

Q5
Tier 2 · Standard

5.

A particle is projected from a point in a vertical plane. After 1.5 s1.5\,\text{s} its velocity is (14i−2.7j) m s−1(14\mathbf{i}-2.7\mathbf{j})\,\text{m s}^{-1}, where i\mathbf{i} and j\mathbf{j} are horizontal and vertically upward unit vectors respectively. Assume that air resistance is negligible and take the downward acceleration as 9.8 m s−29.8\,\text{m s}^{-2}. Find its initial speed and its angle of projection above the horizontal. Give both answers to 3 significant figures.

(4)

(Total for Question 5 is 4 marks)

Mark scheme

Mark scheme for question 5
QuestionSchemeMarks
5
  • Initial speed =18.4 m s−1=18.4\,\text{m s}^{-1}
  • Angle of projection =40.6∘=40.6^\circ
4
Notes
Horizontal velocity is constant, so the initial horizontal component is 1414. Vertically, −2.7=uy−9.8(1.5)-2.7=u_y-9.8(1.5), giving uy=12u_y=12. Hence the initial speed is 142+122=285=18.4 m s−1\sqrt{14^2+12^2}=2\sqrt{85}=18.4\,\text{m s}^{-1} to 3 significant figures. The angle is tan⁡−1(12/14)=40.6∘\tan^{-1}(12/14)=40.6^\circ to 3 significant figures.

(4 marks)

Q6
Tier 3 · Hard

6.

A particle is projected from horizontal ground with velocity (18i+24j) m s−1(18\mathbf{i}+24\mathbf{j})\,\text{m s}^{-1}, where i\mathbf{i} and j\mathbf{j} are horizontal and vertically upward unit vectors respectively. Assume that air resistance is negligible and use a constant downward acceleration of 9.8 m s−29.8\,\text{m s}^{-2}. The particle passes twice through the horizontal level 20 m20\,\text{m} above the point of projection. Find the exact horizontal distance between these two positions and the exact speed at the later position.

(6)

(Total for Question 6 is 6 marks)

Mark scheme

Mark scheme for question 6
QuestionSchemeMarks
6
  • Horizontal distance =3604649 m=\dfrac{360\sqrt{46}}{49}\,\text{m}
  • Later speed =2127 m s−1=2\sqrt{127}\,\text{m s}^{-1}
6
Notes
The vertical displacement is y=24t−4.9t2y=24t-4.9t^2. Setting y=20y=20 gives 9.8t2−48t+40=09.8t^2-48t+40=0, whose roots differ by 482−4(9.8)(40)/9.8=2184/9.8=2046/49\sqrt{48^2-4(9.8)(40)}/9.8=2\sqrt{184}/9.8=20\sqrt{46}/49. Horizontal speed is constant at 18 m s−118\,\text{m s}^{-1}, so the horizontal separation is 18(2046/49)=36046/49 m18(20\sqrt{46}/49)=360\sqrt{46}/49\,\text{m}. At the later crossing the vertical velocity is −184=−246 m s−1-\sqrt{184}=-2\sqrt{46}\,\text{m s}^{-1}, so the speed is 182+(246)2=508=2127 m s−1\sqrt{18^2+(2\sqrt{46})^2}=\sqrt{508}=2\sqrt{127}\,\text{m s}^{-1}.

(6 marks)

Q7
Tier 2 · Standard

7.

A particle is projected with velocity (15i+12j) m s−1(15\mathbf{i}+12\mathbf{j})\,\text{m s}^{-1}, where i\mathbf{i} is horizontal and j\mathbf{j} is vertically upwards. A vertical wall is 30 m30\,\text{m} horizontally from the point of projection. Model the particle as moving freely under gravity and ignore air resistance. Take g=9.8 m s−2g=9.8\,\text{m s}^{-2}. Find the height of the particle above the point of projection when it reaches the wall and find its velocity at that instant.

(5)

(Total for Question 7 is 5 marks)

Mark scheme

Mark scheme for question 7
QuestionSchemeMarks
7
  • Height =4.4 m=4.4\,\text{m}
  • Velocity =(15i−7.6j) m s−1=(15\mathbf{i}-7.6\mathbf{j})\,\text{m s}^{-1}
5
Notes
Horizontal motion gives 30=15t30=15t, so the particle reaches the wall when t=2 st=2\,\text{s}. Its vertical displacement is 12(2)−12(9.8)(22)=4.4 m12(2)-\tfrac12(9.8)(2^2)=4.4\,\text{m}. The horizontal velocity remains 15 m s−115\,\text{m s}^{-1} and the vertical velocity is 12−9.8(2)=−7.6 m s−112-9.8(2)=-7.6\,\text{m s}^{-1}, giving the stated velocity vector.

(5 marks)

Q8
Tier 3 · Hard

8.

A particle is projected from horizontal ground and passes through the point 13 m13\,\text{m} horizontally and 16.1 m16.1\,\text{m} vertically above the point of projection after 1 s1\,\text{s}. Model the particle as moving freely under gravity and ignore air resistance. Take g=9.8 m s−2g=9.8\,\text{m s}^{-2}. Find its initial velocity. Hence find its greatest height and its horizontal distance from the point of projection when it returns to the ground, giving the distance to 3 significant figures. Use unrounded values in your working.

(6)

(Total for Question 8 is 6 marks)

Mark scheme

Mark scheme for question 8
QuestionSchemeMarks
8
  • Initial velocity =(13i+21j) m s−1=(13\mathbf{i}+21\mathbf{j})\,\text{m s}^{-1}
  • Greatest height =22.5 m=22.5\,\text{m}
  • Horizontal distance =55.7 m=55.7\,\text{m}
6
Notes
Horizontal motion gives 13=ux(1)13=u_x(1), so ux=13 m s−1u_x=13\,\text{m s}^{-1}. Vertically, 16.1=uy(1)−12(9.8)(12)16.1=u_y(1)-\tfrac12(9.8)(1^2), so uy=21 m s−1u_y=21\,\text{m s}^{-1}. At greatest height, 0=212−2(9.8)H0=21^2-2(9.8)H, giving H=22.5 mH=22.5\,\text{m}. The non-zero solution of 0=21t−4.9t20=21t-4.9t^2 is t=30/7 st=30/7\,\text{s}, so the horizontal distance is 13(30/7)=390/7=55.714… m13(30/7)=390/7=55.714\ldots\,\text{m}, which is 55.7 m55.7\,\text{m} to 3 significant figures.

(6 marks)

Q9
Tier 3 · Hard

9.

A particle is projected from a point with speed 14 m s−114\,\text{m s}^{-1} at an angle θ\theta above the horizontal, where 0<θ<90∘0<\theta<90^\circ. It passes through a point 20 m20\,\text{m} horizontally from and 5 m5\,\text{m} below the point of projection. Model the particle as moving freely under gravity, ignore air resistance and take g=9.8 m s−2g=9.8\,\text{m s}^{-2}. Show that 2tan⁡2θ−4tan⁡θ+1=02\tan^2\theta-4\tan\theta+1=0. Hence find all possible exact values of θ\theta in the stated interval. Give all numerical answers exactly.

(6)

(Total for Question 9 is 6 marks)

Mark scheme

Mark scheme for question 9
QuestionSchemeMarks
9
  • 2tan⁡2θ−4tan⁡θ+1=02\tan^2\theta-4\tan\theta+1=0
  • θ=tan⁡−1(1−22)\theta=\tan^{-1}(1-\dfrac{\sqrt2}{2}) or θ=tan⁡−1(1+22)\theta=\tan^{-1}(1+\dfrac{\sqrt2}{2})
6
Notes
Write x=14cos⁡θ tx=14\cos\theta\,t and y=14sin⁡θ t−4.9t2y=14\sin\theta\,t-4.9t^2. Eliminating tt gives y=xtan⁡θ−[9.8x2/(2(14)2)]sec⁡2θy=x\tan\theta-[9.8x^2/(2(14)^2)]\sec^2\theta. At x=20x=20 the coefficient is 1010, so −5=20T−10(1+T2)-5=20T-10(1+T^2) where T=tan⁡θT=\tan\theta. This simplifies to 2T2−4T+1=02T^2-4T+1=0, giving T=1±2/2T=1\pm\sqrt2/2. Both values are positive, so both inverse-tangent values lie in the stated interval.

(6 marks)

Q10
Tier 3 · Hard

10.

The vectors i\mathbf{i} and j\mathbf{j} are horizontal and vertically upward unit vectors respectively. A particle is projected from the origin with velocity (8i+15j) m s−1(8\mathbf{i}+15\mathbf{j})\,\text{m s}^{-1}. It first strikes a plane whose cross-section has equation y=x/2y=x/2. Model the particle as moving freely under gravity, ignore air resistance and take g=9.8 m s−2g=9.8\,\text{m s}^{-2}. Find the exact time of impact, the distance measured along the plane from the origin to the impact point, and the exact speed of impact. Give all numerical answers exactly.

(6)

(Total for Question 10 is 6 marks)

Mark scheme

Mark scheme for question 10
QuestionSchemeMarks
10
  • Impact time =11049 s=\dfrac{110}{49}\,\text{s}
  • Distance along the plane =440549 m=\dfrac{440\sqrt5}{49}\,\text{m}
  • Impact speed =113 m s−1=\sqrt{113}\,\text{m s}^{-1}
6
Notes
x=8tx=8t and y=15t−4.9t2y=15t-4.9t^2. At the plane, 15t−4.9t2=(8t)/2=4t15t-4.9t^2=(8t)/2=4t. Besides t=0t=0, this gives t=11/4.9=110/49 st=11/4.9=110/49\,\text{s}. The impact coordinates are (880/49,440/49)(880/49,440/49), so the distance from the origin along the plane is (880/49)2+(440/49)2=4405/49 m\sqrt{(880/49)^2+(440/49)^2}=440\sqrt5/49\,\text{m}. The impact velocity is 8i+[15−9.8(110/49)]j=8i−7j8\mathbf{i}+[15-9.8(110/49)]\mathbf{j}=8\mathbf{i}-7\mathbf{j}, with speed 113 m s−1\sqrt{113}\,\text{m s}^{-1}.

(6 marks)

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