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ELH129M010AQ1 Datasheet(PDF) 19 Page - Kemet Corporation |
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ELH129M010AQ1 Datasheet(HTML) 19 Page - Kemet Corporation |
19 / 26 page ![]() 19 © KEMET Electronics Corporation • P.O. Box 5928 • Greenville, SC 29606 (864) 963-6300 • www.kemet.com A4018_ELH • 2/10/2016 Snap-In Aluminum Electrolytic Capacitors – ELH Series, +85ºC Impedance (Z) Impedance of an electrolytic capacitor results from a circuit formed by the following individual equivalent series components: C o R e L C e C o R e L C e C o = Aluminum oxide capacitance (surface and thickness of the dielectric) R e = Resistance of electrolyte and paper mixture (other resistances not depending on the frequency are not considered: tabs, plates, etc.) C e = Electrolyte soaked paper capacitance L = Inductive reactance of the capacitor winding and terminals Impedance of an electrolytic capacitor is not a constant quantity that retains its value under all conditions; it changes depending on frequency and temperature. Impedance as a function of frequency (sinusoidal waveform) for a certain temperature can be represented as follows: Co Re L Ce 0.1 1 10 100 1000 10000 0.1 1 10 100 1000 Z [ohm] F [KHz] B C A 1/ω ω ω ω Co Re 1/ω ω ω ω Ce ωL • Capacitive reactance predominates at low frequencies • With increasing frequency, capacitive reactance Xc = 1/ωC o decreases until it reaches the order of magnitude of electrolyte resistance R e(A) • At even higher frequencies, resistance of the electrolyte predominates: Z = R e (A - B) • When the capacitor’s resonance frequency is reached (ω 0), capacitive and inductive reactance mutually cancel each other 1/ωC e = ωL, ω0 = C√1/LCe • Above this frequency, inductive reactance of the winding and its terminals (XL = Z = ωL) becomes effective and leads to an increase in impedance Generally speaking, it can be estimated that C e ≈ 0.01 Co. |
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