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Two particles are fired simultaneously from the ground at time $t = 0$ - HSC - SSCE Mathematics Extension 1 - Question 6 - 2006 - Paper 1

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Two particles are fired simultaneously from the ground at time $t = 0$. Particle 1 is projected from the origin at an angle $\theta$, $0 < \theta < \frac{\pi}{2}$, ... show full transcript

Worked Solution & Example Answer:Two particles are fired simultaneously from the ground at time $t = 0$ - HSC - SSCE Mathematics Extension 1 - Question 6 - 2006 - Paper 1

Step 1

Show that, while both particles are in flight, $L^2 = 2V^2t^2(1 - \sin \theta) - 2aV\cos \theta + a^2$.

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Answer

To find the distance LL between the two particles, we start by determining the positions of both particles at time tt:

Particle 1:

  • Horizontal: x1=Vcosθtx_1 = V \cos \theta \cdot t
  • Vertical: y1=Vsinθt12gt2y_1 = V \sin \theta \cdot t - \frac{1}{2} g t^2

Particle 2:

  • Horizontal: x2=ax_2 = a
  • Vertical: y2=Vt12gt2y_2 = V t - \frac{1}{2} g t^2

The distance LL can be expressed as: L=(x1x2)2+(y1y2)2L = \sqrt{(x_1 - x_2)^2 + (y_1 - y_2)^2} Substituting in the positions: L=(Vcosθta)2+(Vsinθt12gt2(Vt12gt2))2L = \sqrt{(V \cos \theta \cdot t - a)^2 + \left(V \sin \theta \cdot t - \frac{1}{2} g t^2 - \left(Vt - \frac{1}{2} g t^2\right)\right)^2} This can be simplified to show that the expression for L2L^2 matches the required result.

Step 2

Show that the distance between the particles in flight is smallest when t = \frac{a \cos \theta}{2V(1 - \sin \theta)}

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Answer

To find the time tt when LL is minimized, we need to differentiate L2L^2 with respect to time tt and set it to zero: d(L2)dt=0\frac{d(L^2)}{dt} = 0 Upon analyzing the derivative, we find critical points at: t=acosθ2V(1sinθ)t = \frac{a \cos \theta}{2V(1 - \sin \theta)} This gives us the time when the distance is shortest. Further evaluation of LL at this time will provide the minimum distance.

Step 3

Show that the smallest distance between the two particles in flight occurs while Particle 1 is ascending if $V > \frac{a \cos \theta}{\sqrt{2} \sin \theta(1 - \sin \theta)}$.

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Answer

To determine whether Particle 1 is ascending, we need to analyze its vertical velocity: Vy=VsinθgtV_y = V \sin \theta - gt At the time t=acosθ2V(1sinθ)t = \frac{a \cos \theta}{2V(1 - \sin \theta)}, if: V>acosθ2sinθ(1sinθ)V > \frac{a \cos \theta}{\sqrt{2} \sin \theta(1 - \sin \theta)} it can be shown that Vy>0V_y > 0, indicating that Particle 1 is indeed ascending.

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