# Applications of resonance

So far, the phenomenon of resonance appears to be a useless curiosity, or at most a nuisance to be avoided (especially if series resonance makes for a short-circuit across our AC voltage source!). However, this is not the case. Resonance is a very valuable property of reactive AC circuits, employed in a variety of applications.

One use for resonance is to establish a condition of stable frequency in circuits designed to produce AC signals. Usually, a parallel (tank) circuit is used for this purpose, with the capacitor and inductor directly connected together, exchanging energy between each other. Just as a pendulum can be used to stabilize the frequency of a clock mechanism’s oscillations, so can a tank circuit be used to stabilize the electrical frequency of an AC *oscillator* circuit. As was noted before, the frequency set by the tank circuit is solely dependent upon the values of L and C, and not on the magnitudes of voltage or current present in the oscillations: (Figure )

*Resonant circuit serves as stable frequency source.*

Another use for resonance is in applications where the effects of greatly increased or decreased impedance at a particular frequency is desired. A resonant circuit can be used to “block” (present high impedance toward) a frequency or range of frequencies, thus acting as a sort of frequency “filter” to strain certain frequencies out of a mix of others. In fact, these particular circuits are called *filters*, and their design constitutes a discipline of study all by itself: (Figure )

*Resonant circuit serves as filter.*

In essence, this is how analog radio receiver tuner circuits work to filter, or select, one station frequency out of the mix of different radio station frequency signals intercepted by the antenna.

**REVIEW:**- Resonance can be employed to maintain AC circuit oscillations at a constant frequency, just as a pendulum can be used to maintain constant oscillation speed in a timekeeping mechanism.
- Resonance can be exploited for its impedance properties: either dramatically increasing or decreasing impedance for certain frequencies. Circuits designed to screen certain frequencies out of a mix of different frequencies are called
*filters*.

## Resonance in series-parallel circuits

In simple reactive circuits with little or no resistance, the effects of radically altered mpedance will manifest at the resonance frequency predicted by the equation given earlier. In a parallel (tank) LC circuit, this means infinite impedance at resonance. In a series LC circuit, it means zero impedance at resonance:

However, as soon as significant levels of resistance are introduced into most LC circuits, this simple calculation for resonance becomes invalid. We’ll take a look at several LC circuits with added resistance, using the same values for capacitance and inductance as before: 10 µF and 100 mH, respectively. According to our simple equation, the resonant frequency should be 159.155 Hz. Watch, though, where current reaches maximum or minimum in the following SPICE analyses:

*Parallel LC circuit with resistance in series with L.*

resonant circuit

v1 1 0 ac 1 sin

c1 1 0 10u

r1 1 2 100

l1 2 0 100m

.ac lin 20 100 200

.plot ac i(v1)

.end

*Resistance in series with L produces minimum current at 136.8 Hz instead of calculated 159.2 Hz*

Minimum current at 136.8 Hz instead of 159.2 Hz!

*Parallel LC with resistance in serieis with C.*

Here, an extra resistor (R_{bogus}) is necessary to prevent SPICE from encountering trouble in analysis. SPICE can’t handle an inductor connected directly in parallel with any voltage source or any other inductor, so the addition of a series resistor is necessary to “break up” the voltage source/inductor loop that would otherwise be formed. This resistor is chosen to be a *very* low value for minimum impact on the circuit’s behavior.

resonant circuit

v1 1 0 ac 1 sin

r1 1 2 100

c1 2 0 10u

rbogus 1 3 1e-12

l1 3 0 100m

.ac lin 20 100 400

.plot ac i(v1)

.end

Minimum current at roughly 180 Hz instead of 159.2 Hz!

*Resistance in series with C shifts minimum current from calculated 159.2 Hz to roughly 180 Hz.*

Switching our attention to series LC circuits, (Figure ) we experiment with placing significant resistances in parallel with either L or C. In the following series circuit examples, a 1 Ω resistor (R_{1}) is placed in series with the inductor and capacitor to limit total current at resonance. The “extra” resistance inserted to influence resonant frequency effects is the 100 Ω resistor, R_{2}.

The results are shown in (Figure

*Series LC resonant circuit with resistance in parallel with L.*

resonant circuit

v1 1 0 ac 1 sin

r1 1 2 1

c1 2 3 10u

l1 3 0 100m

r2 3 0 100

.ac lin 20 100 400

.plot ac i(v1)

.end

Maximum current at roughly 178.9 Hz instead of 159.2 Hz!

*Series resonant circuit with resistance in parallel with L shifts maximum current from 159.2 Hz to roughy 180 Hz.*

And finally, a series LC circuit with the significant resistance in parallel with the capacitor. (Figure

The shifted resonance is shown in (Figure

*Series LC resonant circuit with rsistance in parallel with C.*

resonant circuit

v1 1 0 ac 1 sin

r1 1 2 1

c1 2 3 10u

r2 2 3 100

l1 3 0 100m

.ac lin 20 100 200

.plot ac i(v1)

.end

Maximum current at 136.8 Hz instead of 159.2 Hz!

*Resistance in parallel with C in series resonant circuit shifts curreent maximum from calculated 159.2 Hz to about 136.8 Hz.*

The tendency for added resistance to skew the point at which impedance reaches a maximum or minimum in an LC circuit is called *antiresonance*. The astute observer will notice a pattern between the four SPICE examples given above, in terms of how resistance affects the resonant peak of a circuit:

**Parallel (“tank”) LC circuit:**- R in series with L: resonant frequency shifted
*down* - R in series with C: resonant frequency shifted
*up*

**Series LC circuit:**- R in parallel with L: resonant frequency shifted
*up* - R in parallel with C: resonant frequency shifted
*down*

Again, this illustrates the complementary nature of capacitors and inductors: how resistance in series with one creates an antiresonance effect equivalent to resistance in parallel with the other. If you look even closer to the four SPICE examples given, you’ll see that the frequencies are shifted by the *same amount*, and that the shape of the complementary graphs are mirror-images of each other!

Antiresonance is an effect that resonant circuit designers must be aware of. The equations for determining antiresonance “shift” are complex, and will not be covered in this brief lesson. It should suffice the beginning student of electronics to understand that the effect exists, and what its general tendencies are.

Added resistance in an LC circuit is no academic matter. While it is possible to manufacture capacitors with negligible unwanted resistances, inductors are typically plagud with substantial amounts of resistance due to the long lengths of wire used in their construction. What is more, the resistance of wire tends to increase as frequency goes up, due to a strange phenomenon known as the *skin effect* where AC current tends to be excluded from travel through the very center of a wire, thereby reducing the wire’s effective cross-sectional area. Thus, inductors not only have resistance, but *changing, frequency-dependent* resistance at that.

As if the resistance of an inductor’s wire weren’t enough to cause problems, we also have to contend with the “core losses” of iron-core inductors, which manifest themselves as added resistance in the circuit. Since iron is a conductor of electricity as well as a conductor of magnetic flux, changing flux produced by alternating current through the coil will tend to induce electric currents in the core itself (*eddy currents*). This effect can be thought of as though the iron core of the transformer were a sort of secondary transformer coil powering a resistive load: the less-than-perfect conductivity of the iron metal. This effects can be minimized with laminated cores, good core design and high-grade materials, but never completely eliminated.

One notable exception to the rule of circuit resistance causing a resonant frequency shift is the case of series resistor-inductor-capacitor (“RLC”) circuits. So long as *all* components are connected in series with each other, the resonant frequency of the circuit will be unaffected by the resistance. (Figure

The resulting plot is shown in (Figure

*Series LC with resistance in series.*

series rlc circuit

v1 1 0 ac 1 sin

r1 1 2 100

c1 2 3 10u

l1 3 0 100m

.ac lin 20 100 200

.plot ac i(v1)

.end

Maximum current at 159.2 Hz once again!

*Resistance in series resonant circuit leaves current maximum at calculated 159.2 Hz, broadening the curve.*

Note that the peak of the current graph (Figure ) has not changed from the earlier series LC circuit (the one with the 1 Ω token resistance in it), even though the resistance is now 100 times greater. The only thing that has changed is the “sharpness” of the curve. Obviously, this circuit does not resonate as strongly as one with less series resistnce (it is said to be “less selective”), but at least it has the same natural frequency!

It is noteworthy that antiresonance has the effect of dampening the oscillations of free-running LC circuits such as tank circuits. In the beginning of this chapter we saw how a capacitor and inductor connected directly together would act something like a pendulum, exchanging voltage and current peaks just like a pendulum exchanges kinetic and potential energy. In a perfect tank circuit (no resistance), this oscillation would continue forever, just as a frictionless pendulum would continue to swing at its resonant frequency forever. But frictionless machines are difficult to find in the real world, and so are lossless tank circuits. Energy lost through resistance (or inductor core losses or radiated electromagnetic waves or . . .) in a tank circuit will cause the oscillations to decay in amplitude until they are no more. If enough energy losses are present in a tank circuit, it will fail to resonate at all.

Antiresonance’s dampening effect is more than just a curiosity: it can be used quite effectively to eliminate *unwanted* oscillations in circuits containing stray inductances and/or capacitances, as almost all circuits do. Take note of the following L/R time delay circuit: (Figure )

*L/R time delay circuit*

The idea of this circuit is simple: to “charge” the inductor when the switch is closed. The rate of inductor charging will be set by the ratio L/R, which is the time constant of the circuit in seconds. However, if you were to build such a circuit, you might find unexpected oscillations (AC) of voltage across the inductor when the switch is closed. (Figure Why is this? There’s no capacitor in the circuit, so how can we have resonant oscillation with just an inductor, resistor, and battery?

*Inductor ringing due to resonance with stray capacitance.*

All inductors contain a certain amount of stray capacitance due to turn-to-turn and turn-to-core insulation gaps. Also, the placement of circuit conductors may create stray capacitance. While clean circuit layout is important in eliminating much of this stray capacitance, there will always be some that you cannot eliminate. If this causes resonant problems (unwanted AC oscillations), added resistance may be a way to combat it. If resistor R is large enough, it will cause a condition of antiresonance, dissipating enough energy to prohibit the inductance and stray capacitance from sustaining oscillations for very long.

Interestingly enough, the principle of employing resistance to eliminate unwanted resonance is one frequently used in the design of mechanical systems, where any moving object with mass is a potential resonator. A very common application of this is the use of shock absorbers in automobiles. Without shock absorbers, cars would bounce wildly at their resonant frequency after hitting any bump in the road. The shock absorber’s job is to introduce a strong antiresonant effect by dissipating energy hydraulically (in the same way that a resistor dissipates energy electrically).

**REVIEW:**- Added resistance to an LC circuit can cause a condition known as
*antiresonance*, where the peak impedance effects happen at frequencies other than that which gives equal capacitive and inductive reactances. -
Resistance inherent in real-world inductors can contribute greatly to conditions of antiresonance. One source of such resistance is the
*skin effect*, caused by the exclusion of AC current from the center of conductors. Another source is that of*core losses*in iron-core inductors. - In a simple series LC circuit containing resistance (an “RLC” circuit), resistance does
*not*produce antiresonance. Resonance still occurs when capacitive and inductive reactances are equal.