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Simple Nature - Light and Matter

Simple Nature - Light and Matter

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where dv is the volume of the cube. In evaluating each of thesethree derivatives, we are going to treat the other two variables asconstants, to emphasize this we use the partial derivative notation∂ introduced in chapter 3,dΦ =( ∂Ex∂x + ∂E y∂y + ∂E )zdv .∂zUsing Gauss’ law,4πkq in =( ∂Ex∂x + ∂E y∂y + ∂E )zdv ,∂z<strong>and</strong> we introduce the notation ρ (Greek letter rho) for the chargeper unit volume, giving4πkρ = ∂E x∂x + ∂E y∂y + ∂E z∂z.The quantity on the right is called the divergence of the electricfield, written div E. Using this notation, we havediv E = 4πkρ .b / A meter for measuringdiv E.c / Example 36.This equation has all the same physical implications as Gauss’ law.After all, we proved Gauss’ law by breaking down space into littlecubes like this. We therefore refer to it as the differential form ofGauss’ law, as opposed to Φ = 4πkq in , which is called the integralform.Figure b shows an intuitive way of visualizing the meaning ofthe divergence. The meter consists of some electrically charged ballsconnected by springs. If the divergence is positive, then the wholecluster will exp<strong>and</strong>, <strong>and</strong> it will contract its volume if it is placed ata point where the field has div E < 0. What if the field is constant?We know based on the definition of the divergence that we shouldhave div E = 0 in this case, <strong>and</strong> the meter does give the right result:all the balls will feel a force in the same direction, but they willneither exp<strong>and</strong> nor contract.Divergence of a sine wave example 36⊲ Figure c shows an electric field that varies as a sine wave. Thisis in fact what you’d see in a light wave: light is a wave patternmade of electric <strong>and</strong> magnetic fields. (The magnetic field wouldlook similar, but would be in a plane perpendicular to the page.)What is the divergence of such a field, <strong>and</strong> what is the physicalsignificance of the result?⊲ Intuitively, we can see that no matter where we put the div-meterin this field, it will neither exp<strong>and</strong> nor contract. For instance, if weput it at the center of the figure, it will start spinning, but that’s it.630 Chapter 10 Fields

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