Simple Nature - Light and Matter

j / Example 9. In 1 and 2,charges that are visible on thefront surface of the conductor areshown as solid dots; the otherswould have to be seen throughthe conductor, which we imagineis semi-transparent.k / Short-circuiting a battery.Warning: you can burn yourselfthis way or start a fire! If youwant to try this, try making theconnection only very briefly, usea low-voltage battery, and avoidtouching the battery or the wire,both of which will get hot.The lightning rod example 9Suppose you have a pear-shaped conductor like the one in figurej/1. Since the pear is a conductor, there are free charges everywhereinside it. Panels 1 and 2 of the figure show a computer simulationwith 100 identical electric charges. In 1, the charges arereleased at random positions inside the pear. Repulsion causesthem all to fly outward onto the surface and then settle down intoan orderly but nonuniform pattern.We might not have been able to guess the pattern in advance, butwe can verify that some of its features make sense. For example,charge A has more neighbors on the right than on the left, whichwould tend to make it accelerate off to the left. But when welook at the picture as a whole, it appears reasonable that this isprevented by the larger number of more distant charges on its leftthan on its right.There also seems to be a pattern to the nonuniformity: the chargescollect more densely in areas like B, where the surface is stronglycurved, and less densely in flatter areas like C.To understand the reason for this pattern, consider j/3. Two conductingspheres are connected by a conducting wire. Since thewhole apparatus is conducting, it must all be at one voltage. Asshown in problem 37 on p. 550, the density of charge is greateron the smaller sphere. This is an example of a more general factobserved in j/2, which is that the charge on a conductor packsitself more densely in areas that are more sharply curved.Similar reasoning shows why Benjamin Franklin used a sharp tipwhen he invented the lightning rod. The charged stormclouds inducepositive and negative charges to move to opposite ends ofthe rod. At the pointed upper end of the rod, the charge tendsto concentrate at the point, and this charge attracts the lightning.The same effect can sometimes be seen when a scrapof aluminum foil is inadvertently put in a microwave oven. Modernexperiments (Moore et al., Journal of Applied Meteorology 39(1999) 593) show that although a sharp tip is best at starting aspark, a more moderate curve, like the right-hand tip of the pearin this example, is better at successfully sustaining the spark forlong enough to connect a discharge to the clouds.Short circuitsSo far we have been assuming a perfect conductor. What if itis a good conductor, but not a perfect one? Then we can solve for∆V = IR. An ordinary-sized current will make a very small resultwhen we multiply it by the resistance of a good conductor such asa metal wire. The voltage throughout the wire will then be nearlyconstant. If, on the other hand, the current is extremely large, wecan have a significant voltage difference. This is what happens in a524 Chapter 9 Circuits