The Concept of Resonance

Atoms resonate. Oceans resonate. Your vocal chords resonate. The Tacoma Narrows bridge (Figure 1.2) used to resonate in high winds. Vibrating, periodic phenomena abound in nature, especially within high-speed digital electronics.

Figure 1.2. The Tacoma Narrows bridge in Washington State, known locally as "Galloping Gertie," heaving under the influence of heavy winds.

graphics/01fig02.gif

The technical requirements for resonance are simple. First, there must be two or more reservoirs for the storage of some amount of energy E along with a relatively loss-free mechanism for exchanging the energy between them. Such a system almost always harbors one or more modes of oscillatory behavior whereby the total stored system energy can slosh back and forth among the various storage modes.

Second, there must be a source of external power coupled into (at least) one of the reservoirs. The coupling mechanism must be capable of delivering power P into the system without unduly disturbing the resonant behavior.

Third, the external stimulation must excite the periodic resonant behavior you wish to excite. Otherwise, the system won't start resonating. In technical terms, this means that for linear systems the spectral power density of the source must overlap with the natural resonant frequency (or frequencies) of the system. For nonlinear phenomena, this spectral condition is usually helpful but not always required (see [2] ).

Resonant systems may be characterized by their quality factor, Q . The Q measures the reluctance of a system to give up its naturally stored energy. A system with high Q tends to resonate, or ring, for many cycles. A system with low Q damps quickly.

The value of Q is technically defined as the ratio of energy stored to the average energy dissipated per radian of oscillation. The range of Q values typically encountered in digital electronics ranges from less than unity (no resonance) to more than 10 6 (a highly resonant crystal oscillator).

Let's do a specific example. Consider the simple RLC resonator depicted in Figure 1.3. It is representative of a short, unterminated pcb connection with a heavy capacitive load at the receiver. The resistor R SERIES represents the output impedance of the driving gate. In such a circuit, for a single resistance in series with the resonant elements, the Q equals

Equation 1.11

graphics/01equ11.gif

 

Figure 1.3. A short, unterminated pcb trace with a heavy capacitive load resembles this simple LC series-resonant circuit.

graphics/01fig03.gif

We'll assume in this example the Q is greater than one. Drive this circuit with a periodic waveform, and let the sine wave frequency match the natural frequency of oscillation. Assume the driver rise/fall times are just fast enough to perform this function, so the driving signal looks pretty sinusoidal. From these conditions we may derive the output amplitude of the voltage across the capacitive load. It may surprise you to find that the output amplitude can grow quite large.

A Child s Playground Swing Set

A child's swing set possesses at least two main reservoirs for energy storage. The first reservoir is the gravitational potential energy of the child in proportion to the child's height above the earth and also in proportion to the child's mass. At the peak of each swing cycle, when the child is lifted maximally above the ground and the swing momentarily stops moving, most of the energy in the system is stored as the gravitational potential energy of the child's mass.

The other reservoir is the kinetic energy of the child's motion in proportion to the square of the child's velocity and also in proportion to the child's mass. At the nadir of each cycle, when the child is nearest the ground and moving the fastest , most of the energy in the system is stored as the kinetic energy of the child's motion.

The chains and supporting structure of the swing provide a low-loss mechanism for energy to flow back and forth between these two modes as the child swings up, down, and back again. A well-designed swing will exhibit a natural resonant frequency in the neighborhood of 0.25 Hz.

To operate the system in a continuous fashion, there must be a source of power. Presumably, this is your arm (or maybe your foot ). Look carefully at this interaction. Once you get the child in motion, you need to touch the child for only a small fraction of each cycle . This is of prime importance to the operation of the system. It prevents your presence from unduly disturbing the resonant behavior. Were you to grab hold of the swing continuously, running back and forth along with the child, the swing would merely follow the motion of your arms. If you had arms like Arnold Schwarzenegger, it would be difficult if not impossible to detect any resonant behavior in the swing itself. Technically speaking, in that circumstance your arms would have overpowered the natural forces within the system, defeating the resonance. Highly resonant systems are usually weakly coupled to their driving elements.

The last point worth noting in this example is that (for linear systems) the frequency of excitation must reasonably match the natural frequency of oscillation of the swing. When my daughter was 3 years old, she was strong enough to push a swing but did not comprehend that it mattered at what rate the swing was pushed . Her early attempts to entertain her playmates were met with the disappointment of occasionally getting bashed by the swing. Today, at the age of 10, she intuitively grasps the idea that to maximize the power delivered to the swing, the rate of excitation must match the rate of natural oscillation. If she grows up to learn calculus, I shall be able to explain to her why this must be so.

To begin the analysis, break down the driving signal into two components : a steady-state DC offset and a sinusoid at frequency f . The amplitude of the DC offset is V CC /2 (that's the average value of the output). The amplitude of the fundamental frequency is also V CC /2. When added to the DC offset, this brings the peak excursions just up to V CC and down to zero. We will do the DC and AC analyses separately.

The DC analysis for this circuit is easy. Since input and output are connected with an inductor , the average value of the output must equal the average value of the input. Therefore, the DC component of the output waveform is precisely V CC /2.

The AC analysis for this circuit is not too hard either. It may be derived using an energy-balance equation. This equation will balance the energy delivered to the circuit during one radian of oscillation with the energy dissipated within the circuit over the same period.

Once the circuit has reached steady-state operation, the power delivered to the circuit per radian of oscillation is P /2 p f . The amount of energy dissipated per radian of oscillation (from the definition of Q ) is E/Q . These two quantities must balance:

Equation 1.12

graphics/01equ12.gif

 

where

P is the power delivered to the circuit,

 

E is the total energy stored within the circuit, and

 

Q is the quality factor for the resonator, equal to graphics/019equ01.gif .

You are driving the circuit at its resonant frequency, and you know that the input impedance of a perfect series LC resonator operated at its resonant frequency is zero. Therefore, the AC voltage at point (B) in the circuit must be zero. That implies that the full AC driving voltage of ± V CC /2 must appear across resistor R SERIES . The power P delivered to the circuit must therefore equal ½( V CC /2) 2 / R SERIES .

We also know that the total energy E sloshes back and forth between the inductor and the capacitor. At the peak of the output voltage, all the energy is retained within the capacitor , and none in the inductor (the current through L at this moment is zero). If the AC component of the output swings from + V OUT to - V OUT , the energy E stored within the capacitor at the peaks must equal graphics/019equ02.gif .

Substituting all into equation [1.12], we can now write an energy-balance equation in terms of the AC input amplitude V CC /2 and the AC output amplitude V OUT .

Equation 1.13

graphics/01equ13.gif

 

Rearranging terms,

Equation 1.14

graphics/01equ14.gif

 

Recognizing that graphics/020equ01.gif ,

Equation 1.15

graphics/01equ15.gif

 

Combining the C terms on the right-hand side,

Equation 1.16

graphics/01equ16.gif

 

Finally, recognizing for a series-resonant circuit the definition of graphics/020equ02.gif ,

Equation 1.17

graphics/01equ17.gif

 

And taking a square root of both sides,

Equation 1.18

graphics/01equ18.gif

 

We see that the amplification factor for this circuit, that is, the ratio of the AC output amplitude to the amplitude of the AC fundamental in the driving signal, equals the circuit Q . Therein lies the importance of Q . It defines ( roughly ) the amount of amplification that may occur within a resonant circuit. Note that the complete output waveform is a superposition of the DC response V CC /2 and the amplified AC signal. The preceding analysis applies only when Q >> 1.

Now let's move on to a different problem. Figure 1.4 provides some useful approximations for the maximum degree of overshoot expected when a resonant circuit is driven by a step input .

Figure 1.4. The higher the Q, the greater the overshoot.

graphics/01fig04.gif

As illustrated in Figure 1.4, the higher the Q , the greater the overshoot. For Q of 1/2 or below the circuit is over-damped and no visible overshoot occurs. Values of Q greater than 1/2 create overshoot. These approximations apply to any resonant circuit that has unit response at DC and is possessed of only one main resonance, at a frequency well below the knee frequency of the driving step source, with a Q greater than one.

An excessive value of R SERIES pushes the Q below 1/2, giving the circuit a sluggish , overdamped response. The overdamped response in such a circuit is dominated by the action of the resistor R SERIES charging the capacitor. Given particular values of L and C , the best choice of R SERIES for digital applications is usually whatever value forces Q closest to unity. That gives the best risetime without undue amounts of overshoot. In other applications, such as the feedback filter for a control system, one might strive for a Q somewhat below 1/2.

Occasionally you will encounter an LC tank circuit driven by a current source and loaded by some parallel resistance. For a single resistance in parallel with the resonant elements, the Q equals

Equation 1.19

graphics/01equ19.gif

 

For any LC resonator that includes series and parallel elements, the inverses of the Q 's add

Equation 1.20

graphics/01equ20.gif

 

Distributed transmission lines also harbor resonant modes. As in all resonance problems, they are caused by multiple reservoirs of energy coupled together with a low-loss mechanism.

To understand the energy reservoir formations along a transmission line, imagine a line driven with a specific risetime t r . Every point p n along the line is surrounded by a quantity of dielectric medium that serves as a storage repository for electric field energy. It is also surrounded by a magnetically permeable medium that serves as a storage repository for magnetic field energy. In circuit terms, the voltage and current at point p n form two independent circuit variables , each of which can serve as an energy storage reservoir. Therefore, every transmission line has at least two energy storage reservoirs.

Furthermore, if two points p n and p m along the line are separated by a delay greater than t r , then over a scale of time commensurate with one rising edge, they each represent distinct, uncoupled, independent energy storage reservoirs. The longer the line, the more independent reservoirs exist and the more possibilities develop for resonant behavior.

Common strategies for combating resonance in transmission lines are threefold. Combinations of the three techniques are often employed.

  1. Shrink the line until it is very short, with a delay much shorter than a rising edge. This couples together all the voltages and all the currents along the line so that they can no longer independently vary without influencing each other. Any reasonable real-valued impedance at one end of the line will then fix the global relationship between the voltage and current, nailing them inextricably together. If done properly, the line will be reduced to a system that for all practical purposes possesses only one energy reservoir and therefore cannot resonate.
  2. Terminate the transmission line at one end, the other, or both, using a resistance equal to the characteristic impedance of the line. The termination absorbs part of the power within line, effectively reducing the circuit Q to a very low value. Low- Q circuits cannot resonate.
  3. Add sufficient distributed loss along the transmission line to control the Q . This can be done by selecting the conductor geometry and materials such that the skin-effect resistance is sufficient to do the job or by manipulating the dielectric losses of the substrate.

POINT TO REMEMBER

  • Low- Q , dissipative circuits can't resonate. This is a desirable feature for a digital transmission path .


Fundamentals

Transmission Line Parameters

Performance Regions

Frequency-Domain Modeling

Pcb (printed-circuit board) Traces

Differential Signaling

Generic Building-Cabling Standards

100-Ohm Balanced Twisted-Pair Cabling

150-Ohm STP-A Cabling

Coaxial Cabling

Fiber-Optic Cabling

Clock Distribution

Time-Domain Simulation Tools and Methods

Points to Remember

Appendix A. Building a Signal Integrity Department

Appendix B. Calculation of Loss Slope

Appendix C. Two-Port Analysis

Appendix D. Accuracy of Pi Model

Appendix E. erf( )

Notes



High-Speed Signal Propagation[c] Advanced Black Magic
High-Speed Signal Propagation[c] Advanced Black Magic
ISBN: 013084408X
EAN: N/A
Year: 2005
Pages: 163

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