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6.3 Projection at Any Angle

6.3 Projection at Any Angle

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Question 43

In this question, use g=9.8 m s−2g = 9.8 \text{ m s}^{-2}g=9.8 m s−2.

A rescue flare is projected from a point at sea level with an initial speed of 28 m s−128 \text{ m s}^{-1}28 m s−1 at an angle of elevation θ\thetaθ. The flare is modelled as a particle moving freely under gravity.

The flare reaches a maximum vertical height of HHH metres.

a.

Show that

H=40sin⁡2θ H = 40 \sin^2 \theta H=40sin2θ
[3]
b.

Hence, given that the launch angle is constrained such that 0∘≤θ≤60∘0^\circ \le \theta \le 60^\circ0∘≤θ≤60∘, determine the maximum possible value of HHH.

[2]
c.

A technician suggests that a heavier flare will always reach a lower maximum vertical height when launched with the same initial speed and angle. State whether the technician is correct, giving a reason for your answer.

[1]
Markscheme

6.3 Projection at Any Angle Questions

  1. A Level
  2. /Maths
  3. /6.3 Projection at Any Angle

57 exam-style questions on Edexcel A Level Maths 6.3 Projection at Any Angle. Each one has a worked solution and a mark scheme showing where the marks go.

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