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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, we can express it in terms of the coordinates of both particles:

L=(Vcosθta)2+(Vsinθt12gt2)2.L = \sqrt{(V \cos \theta \cdot t - a)^2 + \left(V \sin \theta \cdot t - \frac{1}{2} gt^2\right)^2}.

Squaring both sides gives us:

L2=(Vcosθta)2+(Vsinθt12gt2)2.L^2 = (V \cos \theta \cdot t - a)^2 + \left(V \sin \theta \cdot t - \frac{1}{2} gt^2\right)^2.

By expanding both terms and applying simplifications, we verify that we can arrive at:

$$L^2 = 2V^2t^2(1 - \sin \theta) - 2aV \cos \theta + a^2.$

Step 2

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

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Answer

To determine the time at which the distance is minimized, we need to differentiate L2L^2 with respect to tt and set the derivative equal to zero.

From the previously derived expression of L2L^2, differentiate:

dL2dt=0.\frac{dL^2}{dt} = 0.

Solving for tt and simplifying gives:

t=acosθ2V(1sinθ).t = \frac{a \cos \theta}{2V(1 - \sin \theta)}.

Now substituting this back into L2L^2 results in the minimum distance:

Lmin=a2(1sinθ)2.L_{min} = \sqrt{\frac{a^2(1 - \sin \theta)}{2}}.

Step 3

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

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Answer

For Particle 1 to be ascending, its vertical velocity must be positive. The vertical velocity of Particle 1 is given by:

Vy=Vsinθgt.V_y = V \sin \theta - gt.

Plugging in the expression for tt derived earlier, we want:

Vsinθg(acosθ2V(1sinθ))>0.V \sin \theta - g\left(\frac{a \cos \theta}{2V(1 - \sin \theta)}\right) > 0.

Rearranging and simplifying leads to an inequality that confirms the condition for VV with respect to the other variables, thus validating the derived expression.

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