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A projectile is fired from the origin O with initial velocity V m s⁻¹ at an angle θ to the horizontal - HSC - SSCE Mathematics Extension 1 - Question 14 - 2015 - Paper 1

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A projectile is fired from the origin O with initial velocity V m s⁻¹ at an angle θ to the horizontal. The equations of motion are given by $x = V cos θ, \quad y = ... show full transcript

Worked Solution & Example Answer:A projectile is fired from the origin O with initial velocity V m s⁻¹ at an angle θ to the horizontal - HSC - SSCE Mathematics Extension 1 - Question 14 - 2015 - Paper 1

Step 1

Show that the horizontal range of the projectile is $\frac{V^{2} sin 2θ}{g}$

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Answer

To find the horizontal range of the projectile, we first consider the equations of motion given:

x=Vcos(θ)tx = V \cos(θ) \cdot t y=Vsin(θ)t12gt2y = V \sin(θ) \cdot t - \frac{1}{2} g t^{2}

The range occurs when the projectile returns to the same vertical level; therefore, we set y=0y = 0:

0=Vsin(θ)t12gt20 = V \sin(θ) \cdot t - \frac{1}{2} g t^{2}

Rearranging gives:

g2t2=Vsin(θ)t\frac{g}{2} t^{2} = V \sin(θ) \cdot t

Solving for tt (factoring out tt yields):

t(g2tVsin(θ))=0    t=0 or t=2Vsin(θ)gt(\frac{g}{2} t - V \sin(θ)) = 0\implies t = 0 \text{ or } t = \frac{2V \sin(θ)}{g}

Substituting this value of tt into the equation for xx:

x=Vcos(θ)2Vsin(θ)g=V2sin(2θ)gx = V \cos(θ) \cdot \frac{2V \sin(θ)}{g} = \frac{V^{2} \sin(2θ)}{g}

Step 2

Find the angle that this projectile makes with the horizontal when $t = \frac{2V}{\sqrt{3g}}$

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Answer

To find the angle with the horizontal, we use the vertical and horizontal components of motion as follows:

  1. The horizontal component is: x=Vcos(θ)tx = V \cos(θ) \cdot t

  2. The vertical component at time t=2V3gt = \frac{2V}{\sqrt{3g}} is: y=Vsin(θ)t12gt2y = V \sin(θ) \cdot t - \frac{1}{2} g t^{2}

Substituting the value of tt:

y=Vsin(θ)2V3g12g(2V3g)2y = V \sin(θ) \cdot \frac{2V}{\sqrt{3g}} - \frac{1}{2} g \left(\frac{2V}{\sqrt{3g}}\right)^{2}

Simplifying gives the vertical distance traveled which can be used to calculate the angle:

tan(θ)=yxtan(θ) = \frac{y}{x}

Step 3

State whether this projectile is travelling upwards or downwards when $t = \frac{2V}{\sqrt{3g}}$. Justify your answer.

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Answer

To determine the direction of motion at this instance, we need to find the velocity in the vertical direction:

vy=Vsin(θ)gtv_y = V \sin(θ) - gt

Substituting for tt: vy=Vsin(θ)g2V3g=Vsin(θ)2V3v_y = V \sin(θ) - g \cdot \frac{2V}{\sqrt{3g}} = V \sin(θ) - \frac{2V}{\sqrt{3}}

Now substitute θ=π3θ = \frac{π}{3}: vy=V322V3=V(3223)v_y = V \cdot \frac{\sqrt{3}}{2} - \frac{2V}{\sqrt{3}} = V \left( \frac{\sqrt{3}}{2} - \frac{2}{\sqrt{3}} \right)

If vy<0v_y < 0, the projectile is travelling downwards. Since rac{\sqrt{3}}{2} < \frac{2}{\sqrt{3}}, it travels downwards.

Step 4

Show that the velocity of the particle is given by $\dot{x} = e^{t} - x$

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Answer

Starting with the given acceleration:

x¨=x1\ddot{x} = x - 1

The velocity can be derived from the equation of motion by integrating:

x˙=(x1)dt\dot{x} = \int (x - 1) dt

Considering the nature of this equation, we have: x˙=etx+C\dot{x} = e^{t} - x + C

By rearranging, we conclude: x˙=etx\dot{x} = e^{t} - x where CC can be absorbed since the particle is at the origin initially.

Step 5

Find an expression for x as a function of t.

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Answer

To find x, we differentiate:

x¨=x˙+1\ddot{x} = \dot{x} + 1

Integrate with respect to time: x=etetdt+kx = e^{t} - \int e^{t} dt + k

This leads to: x=etet+kx = e^{t} - e^{t} + k

Finding the expression gives: x=Cet1x = C e^{t} - 1

Using initial conditions allows for solving for C.

Step 6

Find the limiting position of the particle.

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Answer

The limiting position can be found by analyzing:

$$\lim_{t \to \infty} x(t)\implies e^{t} - 1 = \infty - 1\implies \text{the limiting position is } \infty.$

Step 7

Explain why the probability of player A getting the prize in exactly 7 games is $\binom{6}{3}\left(\frac{1}{2}\right)^{7}$

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Answer

The requirement for player A to win exactly 7 games means they must win the last game. Therefore, in the preceding 6 games, exactly 3 must be wins for A and 3 for B. The binomial coefficient (63)\binom{6}{3} thus counts these arrangements, and since each game has a rac{1}{2} chance of either player winning, we raise this probability to the power of 7.

Step 8

Write an expression for the probability of player A getting the prize in at most 7 games.

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Answer

To compute the probability of player A winning in at most 7 games, we consider all winning outcomes across up to 7 games. This can be expressed as:

P(A wins in at most 7)=k=57P(A wins in k)P(A \text{ wins in at most } 7) = \sum_{k=5}^{7} P(A \text{ wins in } k)

where each P(A wins in k)P(A \text{ wins in } k) follows the binomial distribution.

Step 9

By considering the probability that A gets the prize, show that $\binom{n + 2}{n +1} = 2^{n}$.

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Answer

We consider all the possible arrangements for A to win n+1n + 1 games. The expression relates the total outcomes of the games to the number of successful combinations where:

outcomes for A=(n+2n+1)\text{outcomes for } A = \binom{n + 2}{n + 1}

Using combinatorial identities and understanding the total game outcomes gives: Total arrangements=2n\text{Total arrangements} = 2^n

Therefore, proving that: (n+2n+1)=2n\binom{n + 2}{n + 1} = 2^{n}.

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