cert_exam:tech_radio_op_1:b:freq:h-conductor_skin_effect
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| cert_exam:tech_radio_op_1:b:freq:h-conductor_skin_effect [2019/12/30 00:33] – [出題履歴] fu | cert_exam:tech_radio_op_1:b:freq:h-conductor_skin_effect [2019/12/30 23:50] (current) – fu | ||
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| ======平面波の導体中への表皮厚さ====== | ======平面波の導体中への表皮厚さ====== | ||
| - | | + | 高周波になるにつれて、導線の表皮しか電流が流れなくなる |
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| + | 表皮厚さ$\sigma$は | ||
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| + | $\sigma = \frac{1}{\sqrt{\pi f \mu \rho}}$ | ||
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| + | $\mu$: | ||
| + | $\rho$: | ||
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| + | * 表皮厚さは導電率が大きくなるほど、薄くなる | ||
| + | * 表皮厚さが厚くなるほど、減衰定数は小さくなる(表皮厚さが暑いと減衰しにくい) | ||
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| + | 減衰定数:減少の様子が独立変数 x の関数として exp (-αx) の形になるとき,定数αを減衰定数という。 | ||
| ===== 出題履歴 ===== | ===== 出題履歴 ===== | ||
cert_exam/tech_radio_op_1/b/freq/h-conductor_skin_effect.1577633583.txt.gz · Last modified: by fu · Currently locked by: 74.7.241.13,172.18.0.1
