- #106
pmb_phy
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The energy of a electric field is proportional to the integral of the square of the E-field over the region that the field doesn't vanish. Following the derivation which leads to that conclusion leads one to believe that what you say is true. However if it were true then this proves to be troublesome. It would seem to imply that the field had no momentum. But if the field has no momentum then the principle of momentum conservation would be violated.Andrew Mason said:You have merely pointed out that a charged particle in an electric field has potential energy. My point was that a static electric field which surrounds a charged mass contains no energy UNLESS you bring another charge into it.
There are various ways to express EM energy, not all of which include the integration mentioned above. As such there are different ways to look at the energy involved. Shadowitz covers this in his EM text.When there is a charge in an electric field, that charge has electric potential and one can think of the energy being stored in the field, with its units being that of kQq/r. When there is no charge q in the electric field created by charge Q, I don't see how the field can have any energy.
To be quite literal - Look at how the association of energy<-> field came to be. One starts with a single point charge and assigns a total potential energy of this isolated system to be zero. One then brings in a charged particle from infinity to a nearby point. The work done will equal the change in the potential energy of the system. It makes no sense to say "The potential energy is at this place..etc". Bring in more charges - there will be more potential energy. Now let the charges become infinitesimal and let the number of them approach infinity. The discrete charge distribution then becomes a continuous charge distribution. Then the potential energy can then be expressed as being proportional to the integral of the square of the E-field over all space. If one then applies this relation to the field of a point charge then the integral diverges. What this means physically is that you tried to assemble a point charge. The work required to do that would be infinite. But now recall what this energy means. We *defined* the energy of a point charge to be zero. Thus it would seem reasonable to hold that the energy associated with the E-field of a point charge is zero.
However I have been unable to justify this assertion since when I attempted to do so it led to other problems (I can't recall exactly but I do remember trouble in doing so).
Pete