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Parents Pricing Home Leaving Cert Applied Maths Projectiles A particle is projected from point P, as shown in the diagram, with initial speed 82 m s⁻¹ at an angle of $ heta = an^{-1}(rac{40}{9})$ to the horizontal, where tan $ heta = rac{40}{9}$
A particle is projected from point P, as shown in the diagram, with initial speed 82 m s⁻¹ at an angle of $ heta = an^{-1}(rac{40}{9})$ to the horizontal, where tan $ heta = rac{40}{9}$ - Leaving Cert Applied Maths - Question 3 - 2019 Question 3
View full question A particle is projected from point P, as shown in the diagram, with initial speed 82 m s⁻¹ at an angle of $ heta = an^{-1}(rac{40}{9})$ to the horizontal, where ta... show full transcript
View marking scheme Worked Solution & Example Answer:A particle is projected from point P, as shown in the diagram, with initial speed 82 m s⁻¹ at an angle of $ heta = an^{-1}(rac{40}{9})$ to the horizontal, where tan $ heta = rac{40}{9}$ - Leaving Cert Applied Maths - Question 3 - 2019
Find (i) the initial velocity of the particle in terms of i and j Only available for registered users.
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The initial velocity can be broken down into its horizontal and vertical components using trigonometric functions:
Horizontal component: u_x = u imes ext{cos}( heta) = 82 imes rac{9}{ ext{sqrt}(9^2 + 40^2)}
Vertical component: u_y = u imes ext{sin}( heta) = 82 imes rac{40}{ ext{sqrt}(9^2 + 40^2)}
Hence, the initial velocity in vector form is:
e x t b f u = u x e x t b f i + u y e x t b f j extbf{u} = u_x extbf{i} + u_y extbf{j} e x t b f u = u x e x t b f i + u y e x t b f j
Where, e x t b f u = 82 e x t c o s ( h e t a ) e x t b f i + 82 e x t s i n ( h e t a ) e x t b f j extbf{u} = 82 ext{cos}( heta) extbf{i} + 82 ext{sin}( heta) extbf{j} e x t b f u = 82 e x t cos ( h e t a ) e x t b f i + 82 e x t s in ( h e t a ) e x t b f j .
Find (ii) the velocity of the particle after 5 seconds of motion in terms of i and j Only available for registered users.
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To find the velocity after 5 seconds, we use the components found previously:
The horizontal component remains constant: v_x = u_x = 82 imes rac{9}{ ext{sqrt}(9^2 + 40^2)}
The vertical component changes due to gravity: v y = u y − g t = u y − 9.8 i m e s 5 v_y = u_y - gt = u_y - 9.8 imes 5 v y = u y − g t = u y − 9.8 im es 5
Thus, the velocity vector at t = 5 seconds is:
e x t b f v = v x e x t b f i + v y e x t b f j extbf{v} = v_x extbf{i} + v_y extbf{j} e x t b f v = v x e x t b f i + v y e x t b f j
Find (iii) the displacement of Q from P in terms of i and j Only available for registered users.
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The displacement can be found by considering the horizontal distance traveled and the vertical height of point Q.
Horizontal distance ( d x ) (d_x) ( d x ) traveled in 17 seconds: d_x = u_x imes t = 82 imes rac{9}{ ext{sqrt}(9^2 + 40^2)} imes 17
Vertical distance ( d y ) (d_y) ( d y ) will equal the height difference: d y = h d_y = h d y = h .
Thus, the displacement in vector form is:
e x t D i s p l a c e m e n t = d x e x t b f i + d y e x t b f j ext{Displacement} = d_x extbf{i} + d_y extbf{j} e x t D i s pl a ce m e n t = d x e x t b f i + d y e x t b f j
Find (iv) the value of h, given that the particle lands at R after 17 seconds of motion. Only available for registered users.
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At t = 17 seconds, we set up equations for the horizontal and vertical motions:
Horizontal motion: 54 = u x i m e s 17 54 = u_x imes 17 54 = u x im es 17
Vertical motion: h - 30 = u_y imes t - rac{1}{2} g t^2
Solving both will give us the value of h.
Find (v) the time for which the particle is not passing over a building. Only available for registered users.
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We analyze the vertical motion:
The particle reaches its peak height at t_{ ext{peak}} = rac{u_y}{g} .
Then it starts descending.
To find the time it remains above the height of the building:
Set the height equal to the height of the building and solve for time.
Thus, we can determine the intervals of time when the particle is above the building.
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