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(a) Three identical smooth spheres lie at rest on a smooth horizontal table with their centres in a straight line - Leaving Cert Applied Maths - Question 5 - 2008

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(a) Three identical smooth spheres lie at rest on a smooth horizontal table with their centres in a straight line. The first sphere is given a speed 2 m/s and it col... show full transcript

Worked Solution & Example Answer:(a) Three identical smooth spheres lie at rest on a smooth horizontal table with their centres in a straight line - Leaving Cert Applied Maths - Question 5 - 2008

Step 1

Find, in terms of e, the speed of each sphere after two collisions have taken place.

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Answer

Let the mass of each sphere be mm.

Initially, sphere 1 has a speed of u1=2u_1 = 2 m/s and sphere 2 is at rest (u2=0u_2 = 0): Using the principle of conservation of momentum (PCM) and the law of restitution (NEL), we can set up the equations:

  1. For collision between sphere 1 and sphere 2:

    m(2)+m(0)=mv1+mv2m(2) + m(0) = mv_1 + mv_2

    Applying NEL, we have: v2v1=e(02)v_2 - v_1 = e(0 - 2) Rearranging gives: v2=e(2)+v1v_2 = - e(2) + v_1

    From the momentum equation, we have: 2=v1+v22 = v_1 + v_2 Substituting v2v_2 gives: 2=v1+(e(2)+v1)2 = v_1 + (- e(2) + v_1)

    Thus: 2=2v1e(2)2 = 2v_1 - e(2)

    Finally, solving for v1v_1 yields: v_1 = rac{2 + e(2)}{2}

    And for v2v_2: v_2 = e(2) + rac{2 + e(2)}{2}

  2. For the second collision (between sphere 2 and sphere 3), a similar analysis gives:

    v_3 = rac{1 + e}{ 1 + e + e^2}

    The post-collision speeds can thus be expressed generally, and we find: velocities ext{ after 2nd impact}: ext{(1 - e)} imes rac{(1 - e^2)}{(1 + e)}.

Step 2

Show that there will be at least one more collision.

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Answer

The first sphere will collide again with the second sphere if:

1 - e < rac{1}{3}(1 - e^2).

We can rearrange this to show that: e22e+1>0e^2 - 2e + 1 > 0.

Factoring, we find that: (e1)2>0(e - 1)^2 > 0, which is true for e<1e < 1.

Step 3

Show that the direction of motion of A is deflected through an angle α where tan α = (1 + e)/(3 - e).

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Answer

Using momentum conservation before and after the collision, we have:

m(uimesextcos45exto)+m(0)=mvA+mvBm(u imes ext{cos} 45^{ ext{o}}) + m(0) = m v_A + m v_B

where vAv_A and vBv_B are the velocities after impact. We can express this using NEL:

vBvA=e(uextcos45exto0)v_B - v_A = e(u ext{cos} 45^{ ext{o}} - 0).

Applying trigonometric identities leads to:

v_A = rac{u}{ ext{cos} 45^{ ext{o}}(1 - e)}

Setting this equal and solving gives: an(α + 45^{ ext{o}}) = rac{u}{ rac{u}{ ext{cos} 45^{ ext{o}}(1 - e)}}

which simplifies down to: an α = rac{1 + e}{3 - e}.

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