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Aviation Maintenance Technician Handbook–General

FAA-H-8083-30B Version 2023

Chapter 12

Fundamentals of Electricity & Electronics

Formula: 1 ; XC = ; 2πfC

are functions of an AC frequency. Decreasing the frequency decreases the ohmic value of the inductive reactance, but a decrease in frequency increases the capacitive reactance. At some particular frequency, known as the resonant frequency, the reactive effects of a capacitor and an inductor is equal.

Figure 12-137. A circuit containing resistance, inductance, and capacitance.
Figure 12-137. A circuit containing resistance, inductance, and capacitance.

oppose current flow in a circuit. If the value of resistance is small or consists only of the resistance in the conductors, the value of current flow can become very high.

In a circuit where the inductor and capacitor are in series, and the frequency is the resonant frequency, or frequency of resonance, the circuit is said to be “in resonance” and is referred to as a series resonant circuit. The symbol for resonant frequency is Fn.

If, at the frequency of resonance, the inductive reactance is equal to the capacitive reactance, then:

Formula: XL = XC, or ; 1 ; 2πfL = ; 2πfC ; Dividing both sides by 2 fL, ; 1 ; Fn2 = ; (2π) 2LC

Extracting the square root of both sides gives:

Formula: 1 ; Fn = ; 2π LC

Where Fn is the resonant frequency in cps, C is the capacitance in farads, and L is the inductance in henries. With this formula, the frequency at which a capacitor and inductor is resonant can be determined.

To find the inductive reactance of a circuit use:

Formula: XL = 2πfL

The impedance formula used in a series AC circuit must be modified to fit a parallel circuit.

Figure 12-138. AC parallel circuit containing inductance and resistance.
Figure 12-138. AC parallel circuit containing inductance and resistance.

To find the parallel networks of inductance and capacitive reactors, use:

Formula: XL + XC ; X = XL + XC

To find the parallel networks with resistance capacitive and inductance, use:

Formula: R XL XC ; Z = XL 2 XC 2 + (RXL – RXC)2

Since at the resonant frequency XL cancels XC, the current can become very large, depending on the amount of resistance. In such cases, the voltage drop across the inductor or capacitor is often higher than the applied voltage.

Figure 12-139. A parallel AC circuit containing capacitance and resistance.
Figure 12-139. A parallel AC circuit containing capacitance and resistance.