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University Physics I - Classical Mechanics, 2019

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52 CHAPTER 3. MOMENTUM AND INERTIA<br />

when two identical objects (presumably, therefore, having the same inertia) collide: if the collision<br />

is head-on (so the motion, before and after, is confined to a straight line), they basically exchange<br />

velocities. For instance, a billiard ball hitting another one will stop dead and the second one will set<br />

off with the same speed as the first one. The toy sometimes called “Newton’s balls” or “Newton’s<br />

cradle” also shows this effect. Intuitively, we understand that what it takes to stop the first ball is<br />

exactly the same as it would take to set the second one in motion with the same velocity.<br />

But what if the objects colliding have different inertias? We expect that the change in their<br />

velocities as a result of the collision will be different: the velocity of the object with the largest<br />

inertia will not change very much, and conversely, the change in the velocity of the object with the<br />

smallest inertia will be comparatively larger. A velocity vs. time graph for the two objects might<br />

look somewhat like the one sketched in Fig. 3.1.<br />

1<br />

1 m/s<br />

2<br />

1.2<br />

1<br />

0.8<br />

1<br />

v (m/s)<br />

0.6<br />

0.4<br />

0.2<br />

2<br />

0<br />

-0.2<br />

-0.4<br />

0 2 4 6 8 10<br />

t (ms)<br />

Figure 3.1: An example of a velocity vs. time graph for a collision of two objects with different inertias.<br />

In this picture, object 1, initially moving with velocity v 1i = 1 m/s, collides with object 2, initially<br />

at rest. After the collision, which here is assumed to take a millisecond or so, object 1 actually<br />

bounces back, so its final velocity is v 1f = −1/3 m/s, whereas object 2 ends up moving to the right<br />

with velocity v 2f =2/3 m/s. So the change in the velocity of object 1 is Δv 1 = v 1f −v 1i = −4/3m/s,<br />

whereas for object 2 we have Δv 2 = v 2f − v 2i =2/3m/s.<br />

It is tempting to use this ratio, Δv 1 /Δv 2 , as a measure of the relative inertia of the two objects,<br />

only we’d want to use it upside down and with the opposite sign: that is, since Δv 2 /Δv 1 = −1/2<br />

we would say that object 2 has twice the inertia of object 1. But then we have to ask: is this a

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