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Draft BCPhysics11-4 Edvantage Interactive.pdf - BC Science ...
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The time intervals on both sides of the equation are the same because both forces<br />
act over the same interval of time. So the equation can be simplified to:<br />
m B v B = – m A v A<br />
Therefore, m A v A + m B v B = 0<br />
or p A + p B = 0<br />
Other Examples of the Law of Conservation of Momentum<br />
If you have ever played pool or billiards you will be familiar with the law of conservation<br />
of momentum. When the cue ball, or white ball, hits another ball, momentum is<br />
conserved. For example, if all the momentum is transferred from the cue ball to the<br />
billiard ball, the cue ball will stop and the billiard ball will move.<br />
Sample Problem 4.4.1 — Conservation of Momentum<br />
A railway car of mass 6.0 × 10 3 kg is coasting along a track with a velocity of 5.5 m/s when suddenly a 3.0 × 10 3 kg<br />
load of sulphur is dumped into the car. What is its new velocity?<br />
What to think about<br />
1. What do I know about the problem?<br />
2. What am I trying to solve?<br />
3. What formula applies to this situation?<br />
4. Find the final velocity v 2 .<br />
How to Do It<br />
The momentum of the railway car will not change<br />
because of the law of conservation of momentum.<br />
Let initial mass be m 1 and initial velocity be v 1 .<br />
The final mass of the railway car will be m 2 and the<br />
final velocity v 2 .<br />
Solve for the final velocity v 2 .<br />
m 1 v 1 = m 2 v 2<br />
(6.0 × 103 kg)(5.5 m/s) = (6.0 × 103 kg +<br />
3.0 × 103 kg)(v2 )<br />
33 × 103 kg•m/s = (9.0 × 103 kg)(v2 )<br />
v2 = 33 103 kg•m/s<br />
9.0 103 kg<br />
184 Chapter 4 Newton’s Laws of Motion — DRAFT © <strong>Edvantage</strong> <strong>Interactive</strong> 2011 ISBN 978-0-9864778-3-6