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The Experimental and Historical Foundations of Electricity - Unicamp

The Experimental and Historical Foundations of Electricity - Unicamp

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7.10 Can Two Bodies Electrified with Charges<br />

<strong>of</strong> the Same Sign Attract One Another?<br />

Experiment 7.23<br />

WerepeatExperiment6.5(Figure6.7). Butnowthenegativestrawismoved<br />

even closer to the strip <strong>of</strong> the negatively charged electroscope. We observe that<br />

for distances smaller or equal to a certain value, <strong>of</strong> the order <strong>of</strong> 2 to 4 cm, the<br />

strip is no longer repelled by the straw, being attracted by it. <strong>The</strong> strip touches<br />

the straw <strong>and</strong> remains attached to it.<br />

Experiment 7.24<br />

We repeat Experiments 4.7 <strong>and</strong> 5.23 (Figures 4.18 <strong>and</strong> 5.27). But now<br />

the negative straw is moved even closer to the negative disk <strong>of</strong> the pendulum.<br />

We observe that the inclination <strong>of</strong> the pendulum from the vertical increases<br />

when the distance between the straw <strong>and</strong> the pendulum goes from 15 to 5 cm,<br />

approximately. This shows that the intensity <strong>of</strong> the repulsive force increases<br />

when the distance between them decreases in this range.<br />

However, for distances less than or equal to certain value, <strong>of</strong> the order <strong>of</strong> 5<br />

cm, there is no longer a repulsion between the negative straw <strong>and</strong> the negative<br />

disk. At these small distances they attract one another. <strong>The</strong> disk touches the<br />

negative straw a second time <strong>and</strong> is again repelled by it.<br />

After 2 or 3 <strong>of</strong> these contacts between the negative straw <strong>and</strong> the disk <strong>of</strong> the<br />

pendulum, the same phenomena are once more observed, but over somewhat<br />

different distances. When the disk has a greater degree <strong>of</strong> electrification, the<br />

repulsion between the disk <strong>and</strong> the negative straw can be observed at a distance<br />

larger than before, <strong>of</strong> the order <strong>of</strong> some 20 cm. <strong>The</strong> intensity <strong>of</strong> the repulsive<br />

force increases when this distance is decreased between 20 cm <strong>and</strong> a lower limit<br />

<strong>of</strong> 2 or 3 cm. When the distance between the straw <strong>and</strong> the disk has a value<br />

less than or equal to this lower limit, there is again an attraction between them,<br />

<strong>and</strong> the ACR mechanism comes into play.<br />

<strong>The</strong>se experiments can be understood on the basis <strong>of</strong> the principles discovered<br />

so far.<br />

Let us suppose that a body �, an insulator, has been charged negatively by<br />

friction. It is close to a neutral body ��, a conductor, which has no net charge.<br />

<strong>The</strong>re will be an attractive force between them. This attractive force is due to<br />

the polarization <strong>of</strong> body �� in the presence <strong>of</strong> body �, as in Figure 7.29. We<br />

represent their attractive force by �� > 0 (Figure 7.32 (a)). We now electrify<br />

body �� with a charge <strong>of</strong> the same sign as the charge <strong>of</strong> the attracting body<br />

�. This can be done, for instance, by the ACR mechanism. This will generate<br />

a new force between them. It is repulsive <strong>and</strong> it will be represented here by<br />

�� < 0. In Figure 7.32 (b) we present this new force <strong>of</strong> repulsion, disregarding<br />

the previous attractive force due to the polarization <strong>of</strong> the conductor. <strong>The</strong> new<br />

negative charge on the conductor is represented in the middle <strong>of</strong> body �� only<br />

202

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