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Owen Duffy wrote in
: .... Some thoughts about inductor loss and self capacitance: Consider and ideal coil (ie lossless, no distributed capacitance) in series with a small ideal resistor to represent its loss, the combination having high Q. Connect it to a constant voltage source at some frequency and observe that the current lags the voltage by almost 90 deg. Now shunt that combination coil+resistor with a small lossless capacitor, and note that the current in the capacitor will be small in magnitude, and leading the applied voltage by 90 degrees. The effect of the capacitor is to reduce the total current, and not change its phase slightly. So the combination of coil & series resistance, & shunt capacitance draws less current and at slightly lower (lagging) phase, so it appears to be a smaller but lossier inductor. A workup at 10MHz of some numbers for a 10uH inductance in series with 10 ohms loss resistance gives Z=10+j628, Q is 62.8. When this is shunted by a 2pf ideal capacitor, the impedance is now 11.8 +j682, Q is 58, apparent inductance is 10.9uH in series with 11.8 ohms of resistance. The small shunt capacitor has increased the apparent inductance, and decreased the Q. Where has this newfound loss come from? The current in the coil's loss resistance is higher than the current from the source, so whilst the two terminal equivalent has a higher impedance, the higher internal current is generating larger loss from the smaller resistance. This is the "circulating current" people are talking about. Owen Note |
#2
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In message , Owen Duffy
writes Owen Duffy wrote in : ... Some thoughts about inductor loss and self capacitance: Consider and ideal coil (ie lossless, no distributed capacitance) in series with a small ideal resistor to represent its loss, the combination having high Q. Connect it to a constant voltage source at some frequency and observe that the current lags the voltage by almost 90 deg. Now shunt that combination coil+resistor with a small lossless capacitor, and note that the current in the capacitor will be small in magnitude, and leading the applied voltage by 90 degrees. The effect of the capacitor is to reduce the total current, and not change its phase slightly. So the combination of coil & series resistance, & shunt capacitance draws less current and at slightly lower (lagging) phase, so it appears to be a smaller but lossier inductor. A workup at 10MHz of some numbers for a 10uH inductance in series with 10 ohms loss resistance gives Z=10+j628, Q is 62.8. When this is shunted by a 2pf ideal capacitor, the impedance is now 11.8 +j682, Q is 58, apparent inductance is 10.9uH in series with 11.8 ohms of resistance. The small shunt capacitor has increased the apparent inductance, and decreased the Q. Where has this newfound loss come from? The current in the coil's loss resistance is higher than the current from the source, so whilst the two terminal equivalent has a higher impedance, the higher internal current is generating larger loss from the smaller resistance. This is the "circulating current" people are talking about. Owen Note Just out of interest, if you increased the inductance to 10.9uH by increasing the number of turns, what effect would it have on the Q? Ian. -- |
#3
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Ian Jackson wrote in
: .... Just out of interest, if you increased the inductance to 10.9uH by increasing the number of turns, what effect would it have on the Q? Ian. Ian, that depends on the type of coil. A very simple view (eg if a toroidal core was used) would be that it would take a (10.9/10)^0.5 increase in turns (4.4%), inductive reactance would increase by 9% and R would increase by 4.4%, Q would increase by 4.4%. I don't really understand the relevance of the questions. Owen |
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