μr =
	dh =	\(l_a/(N+0,5)=l_k/(N+1)\)
	Ah =
	=
=
	la =	\(d_h\cdot(N+0,5)\)
	=
N =				←d,L
☺
L0 =				\(L_0=\dfrac{\mu_r\cdot\mu_0\cdot d_a^2\cdot N^2}{1,7593\cdot l_a+0,50266\cdot d_a}\)
L1 =				\(L_1=\dfrac{\mu_r\cdot\mu_0\cdot d_a^2\cdot N^2}{1,2566\cdot l_a+0,56549\cdot d_a}\)
L2 =				\(L_2=\dfrac{\mu_r\cdot\mu_0\cdot d_a^2\cdot N^2}{1,2767\cdot l_a+0,57454\cdot d_a}\)
L3 =				\(L_3=\mu_r\cdot\mu_0\cdot k\cdot d_a\cdot N^2\) \(0,01\le\dfrac{d_a}{l_a}\le 1\rightarrow k=0,6398\cdot\left(\dfrac{d_a}{l_a}\right)^{0,912}\) \(1\lt\dfrac{d_a}{l_a}\le 100\rightarrow k=0,6517+0,5443\cdot\ln\left(\dfrac{d_a}{l_a}\right)\)
dh =
da =
db =
la =
lk =
lh =				\(l_h=\sqrt{(N\cdot\pi\cdot d_a)^2+l_a^2}\)

\(L_0=\dfrac{d_a\cdot N^2}{0,14\cdot\dfrac{l_a}{d_a}+0,04}\)	[da] = [l] = cm; [L0] = cm	Molnár, Jovitza: Rádiósok könyve, 85. oldal ( reprint 1994. ).
\(L_1=\dfrac{d_a^2\cdot N^2}{100\cdot l_a+45\cdot d_a}\)	[da] = [l] = cm; [L1] = μH	Rádióamatőrök kézikönyve 1978. 1.28.
\(L_2=\dfrac{r_a^2\cdot N^2}{10\cdot l_a+9\cdot r_a}\)	[da] = [l] = inch; [L2] = μH	Wheeler képlet
\(L_3=k\cdot d_a\cdot N^2\) \(0,01\le\dfrac{d_a}{l_a}\le 1\rightarrow k=8,04\cdot 10^{-3}\cdot\left(\dfrac{d_a}{l_a}\right)^{0,912}\) \(1\lt\dfrac{d_a}{l_a}\le 100\rightarrow k=8,19\cdot 10^{-3}+6,84\cdot 10^{-3}\cdot\ln\left(\dfrac{d_a}{l_a}\right)\)	[da] = [l] = cm; [L3] = μH	HE 1993-03-101.

μ₀→

---

⌂ Index
☺
Verzió: 2024-08-22 ( 2010-11-13 .. 2024-05-19 18:07:59 UTC )