Cs,Cp←C0..C4 C₀ = C₁ = ←C₀,Cp C₂ = C₃ = C₄ = ☺ ☺ ☺ Co = Cp = \(C_o=C_0+\ \dots\ +C_{n-1}\) Crp = Cs = \(C_{rp}=\dfrac{1}{\dfrac{1}{C_0}+\ \dots\ +\dfrac{1}{C_{n-1}}}\) Ch = \(C_h=\dfrac{n}{\dfrac{1}{C_0}+\ \dots\ +\dfrac{1}{C_{n-1}}}\) Cm = \(C_m=\sqrt[n]{C_0\cdot\ \dots\ \cdot C_{n-1}}\) Csz = \(C_{sz}=\dfrac{C_0+\ \dots\ +C_{n-1}}{n}\) Cn = \(C_n=\sqrt{\dfrac{{C_0}^2+\ \dots\ +{C_{n-1}}^2}{n}}\)

C1←C0,Cs C₀ = Cs = ← C₀..Cn-1 ☺ C₁ = \(C_1=\dfrac{1}{\dfrac{1}{C_s}-\dfrac{1}{C_0}}\)

C1←C0,Cp C₀ = Cp = ← C₀..Cn-1 ☺ C₁ = \(C_1=C_p-C_0\)

D,Q,Rp←C,f,Rs C = f = Rs = ☺ ☺ D=tan(δ) = \(D=\tan(\delta)=2\cdot\pi\cdot f\cdot C\cdot R_s\) δ = \(\delta=\arctan(D)\) Q = \(Q=\dfrac{1}{D}=\dfrac{1}{2\cdot\pi\cdot f\cdot C\cdot R_s}\) Rp = \(R_p=\dfrac{1}{\left(2\cdot\pi\cdot f\cdot C\right)^2\cdot R_s}\) cos(φ) = \(\cos(\varphi)=\dfrac{R}{|Z|}\)

D,Q,Rs←C,f,Rp C = f = Rp = ☺ ☺ D=tan(δ) = \(D=\tan(\delta)=\dfrac{1}{2\cdot\pi\cdot f\cdot C\cdot R_p}\) δ = \(\delta=\arctan(D)\) Q = \(Q=\dfrac{1}{D}=2\cdot\pi\cdot f\cdot C\cdot R_p\) Rs = \(R_s=\dfrac{1}{\left(2\cdot\pi\cdot f\cdot C\right)^2\cdot R_p}\) cos(φ) = \(\cos(\varphi)=\dfrac{R}{|Z|}\)

C←f,X,Z f = ← C,XC|Z XC = ← C,f Z = *i ← C,f ☺ C =	f←C,X,Z C = ←f,XC|Z XC = ←C,f Z = *i ←C,f ☺ f =
Y,Z←C,f C = ←f,XC|Z f = ←C,XC|Z ☺ Y = \(Y=2\cdot\pi\cdot f\cdot C\cdot\mathrm{i}\) XC = \(X_C=\dfrac{1}{2\cdot\pi\cdot f\cdot C}\) Z = \(Z=-\dfrac{1}{2\cdot\pi\cdot f\cdot C}\cdot\mathrm{i}\)

C,←f,I,U f = ←C,I,U I = ←C,f,U U = ←C,f,I ☺ C = \(C=\dfrac{I}{2\cdot\pi\cdot f\cdot U}\)	f←C,I,U C = ←f,I,U I = ←C,f,U U = ←C,f,I ☺ f = \(f=\dfrac{I}{2\cdot\pi\cdot C\cdot U}\)
I←C,f,U C = ←f,I,U f = ←C,I,U U = ←C,f,I ☺ I = \(I=2\cdot\pi\cdot f\cdot C\cdot U\)	U←C,f,I C = ←f,I,U f = ←C,I,U I = ←C,f,U ☺ U = \(U=\dfrac{I}{2\cdot\pi\cdot f\cdot C}\)

C,E←(Q|I,t),U Q = ←E,U ←C,U ←C,E I = t = U = ←E,Q ←C,Q ←C,E ☺ ☺ C = E =	C,Q←E,U E = ←Q,U ←C,U ←C,Q U = ←E,Q ←C,E ←C,Q ☺ ☺ C = \(C=\dfrac{2\cdot E}{U^2}\) Q = \(Q=\dfrac{2\cdot E}{U}\)
C, U←E, (Q|I,t) E = ←Q,U ←C,U ←C,Q Q = ←E,U ←C,E ←C,U I = t = ☺ C = U =	E, Q←C, U C = ←Q,U ←E,U ←E,Q U = ←E,Q ←C,Q ←C,E ☺ ☺ E = \(E=\dfrac{C\cdot U^2}{2}\) Q = \(Q=C\cdot U\)
E,U←C,(Q|I,t) C = ←Q,U ←E,U ←E,Q Q = ←E,U ←C,U ←C,E I = t = ☺ ☺ E = U =	Q,U←C,E C = ←Q,U ←E,U ←E,Q E = ←Q,U ←C,U ←C,Q ☺ ☺ Q = \(Q=\sqrt{2\cdot C\cdot E}\) U = \(U=\sqrt{\dfrac{E}{2\cdot C}}\)

C←R,t,Ub,UC R = ←C,t,U,U t = ←C,R,U,U Ub = UC = ←C,R.t,U ☺ C↑ = \(C_\uparrow=-\dfrac{t}{R\cdot\ln\left(1-\dfrac{U_C}{U_b}\right)}\) C↓ = \(C_\downarrow=-\dfrac{t}{R\cdot\ln\left(\dfrac{U_C}{U_b}\right)}\)	R←C,t,Ub,UC C = ←R,t,U,U t = ←C,R,U,U Ub = UC = ←C,R,t,U ☺ R↑ = \(R_\uparrow=-\dfrac{t}{C\cdot\ln\left(1-\dfrac{U_C}{U_b}\right)}\) R↓ = \(R_\downarrow=-\dfrac{t}{C\cdot\ln\left(\dfrac{U_C}{U_b}\right)}\)
t←C,R,Ub,UC C = ←R,t,U,U R = ←C,t,U,U Ub = UC = ←C,R,t,U ☺ ☺ t↑ = \(t_\uparrow=-C\cdot R\cdot \ln\left(1-\dfrac{U_C}{U_b}\right)\) t↓ = \(t_\downarrow=-C\cdot R\cdot\ln\left(\dfrac{U_C}{U_b}\right)\)	UC←C,R,t,Ub C = ←R,t,U,U R = ←C,t,U,U t = ←C,R,U,U Ub = ☺ U↑ = \(U_{C\uparrow}=U_b\cdot\left(1-e^{-\dfrac{t}{R\cdot C}}\right)\) U↓ = \(U_{C\downarrow}=U_b\cdot e^{-\dfrac{t}{R\cdot C}}\) |I| = \(|I|=\dfrac{U_b\cdot e^{-\dfrac{t}{R\cdot C}}}{R}\)

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⌂ Index
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Verzió: 2026-03-14 ( 2010-06-24 .. 2025-03-10 18:00:01 UTC )
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