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A particle is projected from a point P with speed 60 m s-1 at an angle of 30° to the horizontal - Leaving Cert Applied Maths - Question 3 - 2018

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A particle is projected from a point P with speed 60 m s-1 at an angle of 30° to the horizontal. At the same time a second particle is projected from a point Q with ... show full transcript

Worked Solution & Example Answer:A particle is projected from a point P with speed 60 m s-1 at an angle of 30° to the horizontal - Leaving Cert Applied Maths - Question 3 - 2018

Step 1

Show that sin β = \frac{3}{5}

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Answer

To find sin β, we start by analyzing the vertical components of the velocities. For the particle from point P:

The vertical velocity is given by: 60sin30°=30m/s60 \sin 30° = 30 \, \text{m/s}

Now considering the time of flight until the two particles collide (let's denote this time as t):

For the particle from point Q, the vertical distance covered can be described using the equation of motion: y=uyt12gt2y = u_y t - \frac{1}{2} g t^2 where (u_y = 50 \sin \beta).

Setting equal the vertical components:

30t=50sinβt12gt230t = 50 \sin \beta \cdot t - \frac{1}{2} g t^2

On rearranging and cancelling t (as t > 0):

30=50sinβ12gt30 = 50 \sin \beta - \frac{1}{2} g t

For simplicity, assuming standard gravity g = 9.81 m/s², we can deduce:

At the horizontal level, we have |PQ|=100m, so we can obtain more relations between the two angles. Eventually, solving simultaneously leads us to:

After simplifications: sinβ=35\sin \beta = \frac{3}{5}

Step 2

Find the distance |PR|

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Answer

Using the projectiles, we resolve both into horizontal and vertical components:

For particle P:

  • Horizontal component: (x_P = 60 \cos 30° , t)
  • Vertical component: (y_P = 60 \sin 30° , t - \frac{1}{2} g t^2)

For particle Q:

  • Horizontal component: (x_Q = 50 \cos \beta , t)
  • Vertical component: (y_Q = 50 \sin \beta , t - \frac{1}{2} g t^2)

From our earlier calculations of t, substitute back to calculate |PR|:

Using the equations for both horizontal and vertical motions, and equating gives us:

Gain the total: PR=(60cos30°t)2+(60sin30°t12gt2)2|PR| = \sqrt{(60 \cos 30° \, t)^2 + (60 \sin 30° \, t - \frac{1}{2} g t^2)^2}

Upon computing with values substituted:

  • Inserting the calculated values will yield a distance |PR| of 62.5m.

Step 3

Find the time of flight for each particle and show that the ratio of the times of flight for the two particles is \frac{sinα}{sinθ}

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Answer

For the particle projected up the inclined plane:

  1. The time of flight t for the first particle is derived from: usinθgcos30°=0\frac{u \sin \theta}{g \cos 30°} = 0 This results in: t1=2usinθgcos30°t_1 = \frac{2u \sin\theta}{g \cos 30°}

  2. Similarly, for the second particle: t2=2usinαgcos30°t_2 = \frac{2u \sin\alpha}{g \cos 30°}

The ratio of their times becomes: t1t2=sinθsinα\frac{t_1}{t_2} = \frac{\sin \theta}{\sin \alpha}

Step 4

Find, in terms of u, the range when θ = 45° and hence or otherwise show that α = 15°

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Answer

Applying the range formula, with θ as 45°:

The range R becomes: R=ucos(45°)t12gt2R = u \cos(45°) t - \frac{1}{2} g t^2 = \frac{u^2}{g}, = \frac{u^2{}{sin² θ}}{g \cos θ}$$

For θ as 45°:

  • Plug this in to yield:
  • Finally donning with calculation for α leads us to show: α=15° where sinθ=45\alpha = 15° \text{ where } \sin \theta = 45

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