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2016 Paper 1 Q11
D: 1516.0 B: 1484.7
projectiles range optimisation trigonometric double angle formula quadratic in angle tower maximum range

The point \(O\) is at the top of a vertical tower of height \(h\) which stands in the middle of a large horizontal plain. A projectile \(P\) is fired from \(O\) at a fixed speed \(u\) and at an angle \(\alpha\) above the horizontal. Show that the distance \(x\) from the base of the tower when \(P\) hits the plain satisfies \[ \frac{gx^2}{u^2} = h(1+\cos 2\alpha) + x \sin 2\alpha \,. \] Show that the greatest value of \(x\) as \(\alpha\) varies occurs when \(x=h\tan2\alpha\) and find the corresponding value of \(\cos 2\alpha\) in terms of \(g\), \(h\) and \(u\). Show further that the greatest achievable distance between \(O\) and the landing point is \(\dfrac {u^2}g +h\,\).

Solution: \begin{align*} \rightarrow: && x &= u \cos \alpha t\\ \Rightarrow && t &= \frac{x}{u \cos \alpha}\\ \uparrow: && -h &= u\sin \alpha t- \frac12gt^2 \\ && - h &= x\tan \alpha - \frac12 g \frac{x^2}{u^2}\sec^2 \alpha \\ \Rightarrow && \frac{gx^2}{u^2} &= h(2\cos^2 \alpha) + x2 \tan \alpha \cos^2 \alpha \\ &&&= h(1 + \cos 2 \alpha) + x \sin 2\alpha \\ \frac{\d}{\d \alpha}: && \frac{g}{u^2} 2 x \frac{\d x}{\d \alpha} &= -2h \sin 2 \alpha + 2x \cos 2 \alpha +\frac{\d x}{\d \alpha} \sin 2 \alpha \\ \Rightarrow && \frac{\d x}{\d \alpha} \left ( \frac{2xg}{u^2} - \sin 2 \alpha \right) &= 2\cos 2 \alpha (x -h \tan 2 \alpha) \end{align*} Since the turning point will be a maximum must be \(x = h \tan 2 \alpha\). Therefore, let \(c = \cos 2 \alpha\) \begin{align*} && \frac{gh^2}{u^2} \tan^2 2 \alpha &= h(1 + \cos 2 \alpha) + h \tan 2 \alpha \sin 2 \alpha \\ \Rightarrow && \frac{gh}{u^2}(c^{-2}-1) &= 1+c+\frac{1-c^2}{c} \\ \Rightarrow && \frac{gh(1-c^2)}{u^2c^2} &= \frac{c+c^2+1-c^2}{c}\\ &&&= \frac{1+c}{c} \\ \Rightarrow && \frac{gh(1-c)}{u^2c} &= 1 \\ \Rightarrow && u^2c &= gh(1-c) \\ \Rightarrow && c(u^2+gh) &= gh \\ \Rightarrow && \cos 2 \alpha &= \frac{gh}{u^2+gh} \\ \\ \Rightarrow && d_{max}^2 &= h^2 + h^2 \tan^2 2 \alpha \\ &&&= h^2\sec^2 2 \alpha \\ &&&= h^2 \frac{(u^2+gh)^2}{g^2h^2} \\ &&&= \frac{(u^2+gh)^2}{g^2} \\ &&&= \left (\frac{u^2}{g}+h \right)^2 \\ \Rightarrow && d_{max} &= \frac{u^2}{g}+h \end{align*}

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2016 Paper 2 Q11
D: 1600.0 B: 1484.0
projectiles collision trigonometric identity inequality simultaneous equations angle of elevation tower particle on horizontal surface

  1. Two particles move on a smooth horizontal surface. The positions, in Cartesian coordinates, of the particles at time \(t\) are \((a+ut\cos\alpha \,,\, ut\sin\alpha)\) and \((vt\cos\beta\,,\, b+vt\sin\beta )\), where \(a\), \(b\), \(u\) and \(v\) are positive constants, \(\alpha\) and \(\beta\) are constant acute angles, and \(t\ge0\). Given that the two particles collide, show that \[ u \sin(\theta+\alpha) = v\sin(\theta +\beta)\,, \] where \(\theta \) is the acute angle satisfying \(\tan\theta = \dfrac b a\).
  2. A gun is placed on the top of a vertical tower of height \(b\) which stands on horizontal ground. The gun fires a bullet with speed \(v\) and (acute) angle of elevation \(\beta\). Simultaneously, a target is projected from a point on the ground a horizontal distance \(a\) from the foot of the tower. The target is projected with speed \(u\) and (acute) angle of elevation \(\alpha\), in a direction directly away from the tower. Given that the target is hit before it reaches the ground, show that \[ 2u\sin\alpha (u\sin\alpha - v\sin\beta) > bg\,. \] Explain, with reference to part (i), why the target can only be hit if \(\alpha > \beta\).

Solution:

  1. The particles collide if there exists a time when \begin{align*} && a + ut \cos \alpha &= vt \cos \beta \\ \Rightarrow && t (v \cos \beta-u \cos \alpha) &= a\\ && ut \sin \alpha &= b + vt \sin \beta \\ \Rightarrow && t(u \sin \alpha - v \sin \beta) &= b\\ \Rightarrow && a(u\sin \alpha - v \sin \beta) &= b(v \cos \beta - u \cos \alpha) \\ \Rightarrow && u(a \sin \alpha + b \cos \alpha) &= v (b \cos \beta + a \sin \beta) \\ \Rightarrow && u \sin (\alpha + \theta) &= v \sin (\beta + \theta) \end{align*}
  2. The path of the bullet is \((vt \cos \beta, b + vt \sin \beta -\frac12 g t^2)\). The path of the target is \((a+ut \cos \alpha, ut \sin \alpha - \frac12 g t^2)\). By comparing components as in part (i) and noting the acceleration doesn't change the story, we can see that \(t(u \sin \alpha - v \sin \beta) = b\) and we also need \(u t \sin \alpha - \frac12 gt^2 >0\) or \(u \sin \alpha - \frac12 gt > 0\) \begin{align*} && u \sin \alpha & > \frac12 gt \\ && 2u \sin \alpha & > g \frac{b}{(u \sin \alpha - v \sin \beta)} \\ \Rightarrow && 2u \sin \alpha( u \sin \alpha - v \sin \beta) & > gb \end{align*} Notice we must have \(u \sin \alpha > v \sin \beta\) and \(u \sin (\alpha + \theta) = v \sin (\beta + \theta)\) so \( \frac{\sin \alpha}{\sin (\alpha + \theta)} > \frac{\sin \beta}{\sin (\beta + \theta)}\), but if we consider \(f(t) = \frac{\sin t}{\sin(t+x)}\) we can see \(f'(t) = \frac{\cos t \sin(t + x) - \sin t \cos(t+x)}{\sin^2(t+x)} = \frac{\sin x}{\sin^2(t+x)} > 0\) is increasing, therefore \(\alpha > \beta\).

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