9 Linear Momentum and Collisions
9.3 Conservation of Linear Momentum
Learning Objectives
By the end of this section, you will be able to:
- Explain the meaning of “conservation of momentum”
- Correctly identify if a system is, or is not, closed
- Define a system whose momentum is conserved
- Mathematically express conservation of momentum for a given system
- Calculate an unknown quantity using conservation of momentum
Recall Newton’s third law: When two objects of masses [latex]{m}_{1}[/latex] and [latex]{m}_{2}[/latex] interact (meaning that they apply forces on each other), the force that object 2 applies to object 1 is equal in magnitude and opposite in direction to the force that object 1 applies on object 2. Let:
- [latex]{\mathbf{\overset{\to }{F}}}_{21}=[/latex] the force on [latex]{m}_{1}[/latex] from [latex]{m}_{2}[/latex]
- [latex]{\mathbf{\overset{\to }{F}}}_{12}=[/latex] the force on [latex]{m}_{2}[/latex] from [latex]{m}_{1}[/latex]
Then, in symbols, Newton’s third law says
(Recall that these two forces do not cancel because they are applied to different objects. [latex]{F}_{21}[/latex] causes [latex]{m}_{1}[/latex] to accelerate, and [latex]{F}_{12}[/latex] causes [latex]{m}_{2}[/latex] to accelerate.)
Although the magnitudes of the forces on the objects are the same, the accelerations are not, simply because the masses (in general) are different. Therefore, the changes in velocity of each object are different:
However, the products of the mass and the change of velocity are equal (in magnitude):
It’s a good idea, at this point, to make sure you’re clear on the physical meaning of the derivatives in Figure. Because of the interaction, each object ends up getting its velocity changed, by an amount dv. Furthermore, the interaction occurs over a time interval dt, which means that the change of velocities also occurs over dt. This time interval is the same for each object.
Let‘s assume, for the moment, that the masses of the objects do not change during the interaction. (We’ll relax this restriction later.) In that case, we can pull the masses inside the derivatives:
and thus
This says that the rate at which momentum changes is the same for both objects. The masses are different, and the changes of velocity are different, but the rate of change of the product of m and [latex]\mathbf{\overset{\to }{v}}[/latex] are the same.
Physically, this means that during the interaction of the two objects ([latex]{m}_{1}\,\text{and}\,{m}_{2}[/latex]), both objects have their momentum changed; but those changes are identical in magnitude, though opposite in sign. For example, the momentum of object 1 might increase, which means that the momentum of object 2 decreases by exactly the same amount.
In light of this, let’s re-write Figure in a more suggestive form:
This says that during the interaction, although object 1’s momentum changes, and object 2’s momentum also changes, these two changes cancel each other out, so that the total change of momentum