electricalmachinery blogspot.com

Electrical Machinery

Wednesday, January 18, 2012. Now lets put a resistor, capacitor and inductor in series. At any given time, the voltage across the three components in series, v. T, is the sum of these. The current it we shall keep sinusoidal, as before. The voltage across the resistor, v. T, is in phase with the current. That across the inductor, v. T, is 90 ahead and that across the capacitor, v. T, is 90 behind. So Pythagoras now gives us. 1ωC Substituting and taking the common factor I gives. And φ on the.

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Electrical Machinery

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Wednesday, January 18, 2012. Now lets put a resistor, capacitor and inductor in series. At any given time, the voltage across the three components in series, v. T, is the sum of these. The current it we shall keep sinusoidal, as before. The voltage across the resistor, v. T, is in phase with the current. That across the inductor, v. T, is 90 ahead and that across the capacitor, v. T, is 90 behind. So Pythagoras now gives us. 1ωC Substituting and taking the common factor I gives. And φ on the.

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This web page electricalmachinery.blogspot.com states the following, "Wednesday, January 18, 2012." We saw that the webpage said " Now lets put a resistor, capacitor and inductor in series." It also said " At any given time, the voltage across the three components in series, v. T, is the sum of these. The current it we shall keep sinusoidal, as before. The voltage across the resistor, v. T, is in phase with the current. That across the inductor, v. T, is 90 ahead and that across the capacitor, v. T, is 90 behind. So Pythagoras now gives us. 1ωC Substituting and taking the common factor I gives."

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