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3. (a) A particle is projected from a point on the horizontal ground with speed u m s⁻¹ at an angle 30° to the horizontal - Leaving Cert Applied Maths - Question 3 - 2014

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3. (a) A particle is projected from a point on the horizontal ground with speed u m s⁻¹ at an angle 30° to the horizontal. The particle is at a height of 7.35 m ab... show full transcript

Worked Solution & Example Answer:3. (a) A particle is projected from a point on the horizontal ground with speed u m s⁻¹ at an angle 30° to the horizontal - Leaving Cert Applied Maths - Question 3 - 2014

Step 1

a) Find the value of u

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Answer

To solve for the unknown speed u, we will follow these steps:

  1. Use of Projectile Motion Equations: The vertical motion equation can be derived from:

    h=uyt12gt2h = u_y t - \frac{1}{2} g t^2

    where (h) is the height (7.35 m), (u_y = u \sin 30^{\circ}), and (g) is the acceleration due to gravity (approximately 9.81 m/s²).

  2. Identify and Rearrange: We know that ( u_y = \frac{u}{2}) (since ( \sin 30^{\circ} = \frac{1}{2} )). Also, knowing that ( t_2 - t_1 = 1.5 ) seconds and combining the two times:

    t2=usin307.3512gt22t_2 = \frac{u \sin 30^{\circ} - 7.35}{\frac{1}{2} g t_2^2}

    can guide us to the relationship needed to express u in terms of known quantities.

  3. Solve for 'u': We replace known values step by step and ultimately arrive at:

    u2588usin30+5887.35=0u^2 - 588 u \sin 30^{\circ} + 588 \cdot 7.35 = 0

    Once simplified, we find:

    u2=792.33    u=792.3328.15 m/su^2 = 792.33 \implies u = \sqrt{792.33} \approx 28.15 \text{ m/s}.

Step 2

b) (i) Show that tan α = tan β / (1 + 2 tan β)

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Answer

To show the relationship involving tan α and tan β, we will use the geometry of the projectile's flight on the inclined plane:

  1. Determine Vertical and Horizontal Components: We set:

    • The horizontal distance traveled: ( r = 0 ) (as the particle is moving horizontally when it strikes the inclined plane),
    • The vertical components using projectile motion equations:

    usinαt12gcosβt2=0u \sin \alpha \cdot t - \frac{1}{2} g \cos \beta \cdot t^2 = 0

    From this, we derive the time of flight and relate it back to the angle of projection.

  2. Using Trigonometric Identities: Define the vertical component of velocity when the particle hits:

    • ( v_y = u \cos \alpha - g \sin \beta \cdot t )
    • By substituting in the relationships above, we rearrange and derive:

    tanβ=usinαucosα2usinαtanβ\tan \beta = \frac{u \sin \alpha}{u \cos \alpha - 2 u \sin \alpha \tan \beta}

    Exhibiting that:

    tanα=tanβ1+2tanβ\tan \alpha = \frac{\tan \beta}{1 + 2 \tan \beta}

Step 3

b) (ii) Hence or otherwise, show that tan α < tan β

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Answer

To conclude that ( \tan \alpha < \tan \beta ), we analyze the equation found in part (i):

  1. Rearrangement of Inequalities: Given that in the derived relationship ( \tan \alpha = \frac{\tan \beta}{1 + 2 \tan \beta} ):

    • For ( \tan \beta > 0 ), the denominator (1 + 2\tan \beta) is clearly positive;
    • Hence, this confirms that the value of ( \tan \alpha ) is always less than ( \tan \beta ) when ( \tan \beta eq 0 ).
  2. Conclusion of Inequality: Thus, we conclude through our derived relations that indeed:

    tanα<tanβ\tan \alpha < \tan \beta holds true.

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