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Cecil, W5DXP wrote:
"Charge is NOT limited to an infinitesimal charged particle, as you imply." True, but charge has a force characteristic. The electron has a charge of -1, or, the value of negative charge carried by an electron is one. A coulomb is (6.281 times 10 to the 18th power) times the charge carried by one electron. A coulomb per second past a particular point is also one ampere. I have long thought that electrical charges, individually, likely have random motions but that an ampere is the net result of more charges moving one way than another. With so many small charges involved in a net substantial charge flow, why shouldn`t charges be moving in two or more directions at once? Best regards, Richard Harrison, KB5WZI |
#2
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![]() Richard Harrison wrote: Cecil, W5DXP wrote: "Charge is NOT limited to an infinitesimal charged particle, as you imply." True, but charge has a force characteristic. The electron has a charge of -1, or, the value of negative charge carried by an electron is one. A coulomb is (6.281 times 10 to the 18th power) times the charge carried by one electron. A coulomb per second past a particular point is also one ampere. I have long thought that electrical charges, individually, likely have random motions but that an ampere is the net result of more charges moving one way than another. With so many small charges involved in a net substantial charge flow, why shouldn`t charges be moving in two or more directions at once? The simplest answer is that charges move in response to the local electric field they experience. That field has only one value at that point, at that instant, and is determined by the superposition of all local electric fields. 73, AC6XG |
#3
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On Tue, 31 Aug 2004 08:50:39 -0700, Jim Kelley
wrote: With so many small charges involved in a net substantial charge flow, why shouldn`t charges be moving in two or more directions at once? The simplest answer is that charges move in response to the local electric field they experience. That field has only one value at that point, at that instant, and is determined by the superposition of all local electric fields. If you presume the simplest answer, it still entails complexity in that this is more correctly called "directed drift" wherein the motion of the chargeS are random within a locality, but in the aggregate and as an average tend in one direction. This sort of dovetails with recent postings by Art speculating about charge accelerating (without needing power mind you) in the circle of a loop antenna. The truth of the matter is that those electrons/holes would never move in a circle, nor even an arc given the short distance of the net migration being very much less than the diameter of a small, small wire (and at any HF frequency, infinitesimal). 73's Richard Clark, KB7QHC |
#4
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Jim Kelley wrote:
The simplest answer is that charges move in response to the local electric field they experience. That field has only one value at that point, at that instant, and is determined by the superposition of all local electric fields. Hi Jim, we missed you. For RF, it is certainly possible for the network charges, at t(x), to be moving in the opposite direction from force exerted by the network electric field (voltage) at t(x). Remember, dQ/dt can have a different sign from the sign of the electric field voltage. This ain't DC. -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
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