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I have observed this phenomenon as well but it seems
to be mainly an issue with beads or shapes with small holes. The bead magnetizes from the inside out. Larger "toroids" with sizeable center holes don't magnetize as easily. This make sense physics-wise since Ampere's law says H is inversely proportional to radius. Rick N6RK "J M Noeding" wrote in message ... Reposted due to changed URL Hi have noted the following measurement (from LA7MI) forAmidon FB43-4301, and wonder if someone knows more available data for actual ferrite- and iron-powder cores to be used in transmitters? For a Amidon FB43-4301 the inductance drops by 50% for 1.2At. 3At for 75% reduction. One should keep the DC-current below the value of 0.5A to keep the reduction below 0.5. In the example above this rule is used, but the best is to use push-pull arrangement and the DC magnitation is kept to a minimum level. The inductance reduction is stored and the effect is called remanence, cores used for direct current should have air-gap Will write a page - http://www.noding.com/la8ak/12345/n12.htm (changed URL) for constructing RF power amplifier based on an article written by LA7MI and distributed to a local London radio club in 1992 73 Jan-Martin LA8AK http://home.online.no/~la8ak/c.htm |
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