Chapter 23 Electromagnetic Induction, AC Circuits, and Electrical Technologies
Chapter 23 Electromagnetic Induction, AC Circuits, and Electrical Technologies
23.11 Reactance, Inductive and Capacitive
- Sketch voltage and current versus time in simple inductive, capacitive, and resistive circuits.
- Calculate inductive and capacitive reactance.
- Calculate current and/or voltage in simple inductive, capacitive, and resistive circuits.
Many circuits also contain capacitors and inductors, in addition to resistors and an AC voltage source. We have seen how capacitors and inductors respond to DC voltage when it is switched on and off. We will now explore how inductors and capacitors react to sinusoidal AC voltage.
Inductors and Inductive Reactance
Suppose an inductor is connected directly to an AC voltage source, as shown in [link]. It is reasonable to assume negligible resistance, since in practice we can make the resistance of an inductor so small that it has a negligible effect on the circuit. Also shown is a graph of voltage and current as functions of time.
The graph in [link](b) starts with voltage at a maximum. Note that the current starts at zero and rises to its peak after the voltage that drives it, just as was the case when DC voltage was switched on in the preceding section. When the voltage becomes negative at point a, the current begins to decrease; it becomes zero at point b, where voltage is its most negative. The current then becomes negative, again following the voltage. The voltage becomes positive at point c and begins to make the current less negative. At point d, the current goes through zero just as the voltage reaches its positive peak to start another cycle. This behavior is summarized as follows:
When a sinusoidal voltage is applied to an inductor, the voltage leads the current by one-fourth of a cycle, or by a
90º90º phase angle.
Current lags behind voltage, since inductors oppose change in current. Changing current induces a back emf V=−L(ΔI/Δt)V=−L(ΔI/Δt) size 12{V= – L ( ΔI/Δt ) } {}. This is considered to be an effective resistance of the inductor to AC. The rms current II size 12{I} {} through an inductor LL size 12{L} {} is given by a version of Ohm’s law:
where
VV is the rms voltage across the inductor and XLXL size 12{X rSub { size 8{L} } } {} is defined to be
with ff size 12{f} {} the frequency of the AC voltage source in hertz (An analysis of the circuit using Kirchhoff’s loop rule and calculus actually produces this expression). XLXL size 12{X rSub { size 8{L} } } {} is called the inductive reactance, because the inductor reacts to impede the current. XLXL size 12{X rSub { size 8{L} } } {} has units of ohms (1 H=1 Ω⋅s1 H=1 Ω⋅s, so that frequency times inductance has units of (cycles/s)(Ω⋅s)=Ω(cycles/s)(Ω⋅s)=Ω size 12{ ( “cycles/s” ) ( ` %OMEGA cdot s ) = %OMEGA } {}), consistent with its role as an effective resistance. It makes sense that XLXL size 12{X rSub { size 8{L} } } {} is proportional to LL size 12{L} {}, since the greater the induction the greater its resistance to change. It is al