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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, $0 < \theta < \frac{\pi}{2}$, with an ... 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, $L^2 = 2V^2t^2(1 - \sin \theta) - 2aVt \cos \theta + a^2$.

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Answer

To find the distance LL between the two particles, we can use the equations of motion. The position of Particle 1 at time tt is given by: x1=Vtcosθx_1 = Vt \cos \theta
y1=Vtsinθ12gt2y_1 = Vt \sin \theta - \frac{1}{2}gt^2

For Particle 2, we have: x2=ax_2 = a
y2=Vt12gt2.y_2 = Vt - \frac{1}{2}gt^2.

The distance LL between the two particles can be expressed as: L=(x1x2)2+(y1y2)2.L = \sqrt{(x_1 - x_2)^2 + (y_1 - y_2)^2}.
Substituting the expressions for x1x_1, x2x_2, y1y_1, and y2y_2 into this equation, we can simplify and show that: L2=2V2t2(1sinθ)2aVtcosθ+a2.L^2 = 2V^2t^2(1 - \sin \theta) - 2aVt \cos \theta + a^2.

Step 2

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

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Answer

To minimize the distance LL, we need to differentiate L2L^2 with respect to tt and set the derivative equal to zero. We find:

d(L2)dt=0.\frac{d(L^2)}{dt} = 0.

Solving for tt gives: t=acosθ2V(1sinθ).t = \frac{a \cos \theta}{2V(1 - \sin \theta)}.

Next, substituting this value back into the expression for L2L^2 yields: Lmin2=a24(1sinθ),L_{min}^2 = \frac{a^2}{4}(1 - \sin \theta),
therefore, Lmin=a21sinθ.L_{min} = \frac{a}{2} \sqrt{1 - \sin \theta}.

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 establish that Particle 1 is ascending when the minimum distance occurs, we evaluate the velocity of Particle 1: Vy=Vsinθgt.V_y = V \sin \theta - gt.

Substituting the expression for tt gives: Vy=Vsinθgacosθ2V(1sinθ).V_y = V \sin \theta - g \frac{a \cos \theta}{2V(1 - \sin \theta)}.

If we require Vy>0V_y > 0, we must show: V>acosθ2sinθ(1sinθ),V > \frac{a \cos \theta}{\sqrt{2}\sin \theta(1 - \sin \theta)},
which confirms that Particle 1 is still ascending.

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