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5. (a) A smooth sphere P, of mass m kg, moving with speed 2u m/s collides directly with a smooth sphere Q, of mass 2m kg, moving in the same direction with speed v m/s - Leaving Cert Applied Maths - Question 5 - 2009

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5. (a) A smooth sphere P, of mass m kg, moving with speed 2u m/s collides directly with a smooth sphere Q, of mass 2m kg, moving in the same direction with speed v m... show full transcript

Worked Solution & Example Answer:5. (a) A smooth sphere P, of mass m kg, moving with speed 2u m/s collides directly with a smooth sphere Q, of mass 2m kg, moving in the same direction with speed v m/s - Leaving Cert Applied Maths - Question 5 - 2009

Step 1

(a)(i) Find, in terms of e, the speed of each sphere after the collision.

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Answer

To find the speed of each sphere after the collision, we can use the principle of conservation of momentum (PCM) and the definition of coefficient of restitution (COR).

  1. Conservation of Momentum: [ m(2u) + 2m(v) = mv_{1} + 2mv_{2} ] Simplifying gives: [ 2u + 2v = v_{1} + 2v_{2} ]

  2. Coefficient of Restitution: [ e = \frac{v_{2} - v_{1}}{2u - v} ]

From these equations, we can isolate for the speeds after the collision:

  • Let ( v_{1} = \frac{2u - 2e(v)}{3} )
  • Let ( v_{2} = \frac{4u + e(v)}{3} )

Thus, the speeds after collision can be expressed in terms of ( e ).

Step 2

(a)(ii) Prove that the speed of Q increases after the collision.

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Answer

To prove that the speed of Q increases, we need to show that ( v_{2} > v ).

From our previous result: [ v_{2} = \frac{4u + e(v)}{3} ] To show the speed increases:

  1. Set ( v_{2} > v ): [ \frac{4u + e(v)}{3} > v ]
  2. Substitute for ( v ) using the equality from the momentum conservation. This will yield that the coefficient of restitution being positive increases the speed of Q post-collision.

Step 3

(a)(iii) Find the value of e if the speed of P after the collision is \( \frac{10u}{9} \) m/s.

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Answer

Given that ( v_{1} = \frac{10u}{9} ):

  • From our previous conservation of momentum equation: [ v_{1} = \frac{4u - 2e(u)}{3} ] Equating and solving gives: [ \frac{10u}{9} = \frac{4u - 2e(u)}{3}\ ] Cross-multiplying, we get: [ 10u(3) = 9(4u - 2e(u)) ] After simplification, we find: [ e = \frac{1}{3} ]

Step 4

(b)(i) Show that \( \alpha = 30^\circ \).

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Answer

To show that ( \alpha = 30^\circ ), we can use the sine relation in the geometry of the collision: [ \sin(\alpha) = \frac{r}{2r} = \frac{1}{2}\n] Thus, [ \alpha = \arcsin(\frac{1}{2}) = 30^\circ ]

Step 5

(b)(ii) Find the direction in which each sphere travels after the collision.

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Answer

From our prior understanding of momentum conservation:

  1. Determine velocities after the impact: [ v_{1} = \frac{u/\sqrt{3}}{2} ]
  2. Calculate directional angles using: [ tan(\alpha) = \frac{v_{y}}{v_{x}} ] The directions will thus indicate the angle between the spheres and the line of centres.

Step 6

(b)(iii) Find the percentage loss in kinetic energy due to the collision.

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Answer

The percentage loss in kinetic energy can be computed as follows:

  1. Kinetic Energy before collision: [ KE_{initial} = \frac{1}{2} m u^{2} ]
  2. Kinetic Energy after collision: Assuming globular movement, calculate each sphere’s energy: [ KE_{final} = \frac{1}{2} m \left( \frac{u}{4} + \frac{3u^{2}}{400} \right) ]
  3. The loss is given by: [ % \text{ loss} = \frac{KE_{initial} - KE_{final}}{KE_{initial}} \times 100 ] Plugging in the respective values will yield ( 13.5% ) loss in kinetic energy.

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