Quartz Crystal Theory of Operation (77 KB)
Quartz Crystal Design Notes (92 KB)
Quartz Crystal Theory of Operation and Design Notes
Oscillator Theory of Operation
Quartz Crystal Theory of Operation and Design Notes
Quartz Crystal Theory of Operation (77 KB)
Quartz Crystal Design Notes (92 KB)
Quartz crystal units serve as the controlling element of oscillator circuits
by conversion of mechanical vibrations to electrical current at a specific
frequency. This is accomplished by means of the "Piezoelectric"
effect. Piezoelectricity is electricity created by pressure. In a piezoelectric
material, the application of mechanical pressure along an axis will result in
the creation of an electrical charge along an axis at right angles to the first.
In some materials, the obverse piezoelectric effect is found, which means that
the imposition of an electric field on the ends of an axis will result in a
mechanical deflection along an axis at right angles to the first. Quartz is
uniquely suited, in terms of mechanical, electrical and chemical properties, for
the manufacture of frequency control devices. Quartz crystal units which
oscillate within certain frequency and temperature ranges have been developed
over the years. Figure 1 shows the location of specific elements within a quartz
stone.
Figure 1
The elements as shown above vibrate in various modes, the most important of
which are the extensional, flexural and shear. The mode of vibration determines
the maximum frequency, stability vs. temperature, and resistance of a given
element. The various modes of vibration are shown in Figure 2, while a
comparison of the various frequency stabilities vs temperature are shown in
Figure 3.
Figure 2
Figure 3
Of the various elements, the "AT" cut has become the most popular
as it is available at relatively high frequencies, exhibits excellent frequency
vs temperature stability and is widely available at reasonable cost. The
frequency vs. temperature capabilities of the "AT" cut crystal unit
are illustrated in Figure 4.
Figure 4
Fundamental vs. Overtone
This is of concern primarily when specifying the "AT" cut crystal
unit. These units increase in frequency as the thickness of the resonator plate
is diminished. At some point, typically around 30MHz, the plate becomes too thin
for efficient processing. As the "AT" will resonate at odd integer
multiples of the fundamental frequency, it is necessary to specify the desired
order of overtone when ordering higher frequency crystals.
Drive Level
Drive level is the amount of power dissipated by the crystal. Drive level is
usually specified in terms of micro or milliwatts, with a typical value being
100 microwatts.
Series vs. Parallel
"Series" resonant crystals are intended for use in circuits which
contain no reactive components in the oscillator feedback loop.
"Parallel" resonant crystals are intended for use in circuits which
contain reactive components (usually capacitors) in the oscillator feedback
loop. Such circuits depend on the combination of the reactive components and the
crystal to accomplish the phase shift necessary to start and maintain
oscillation at the specified frequency. Basic depictions of two such circuits
are shown below.
Figure 5
Load Capacitance
This refers to capacitance external to the crystal, contained within the
feedback loop of the oscillator circuit. If the application requires a
"parallel" resonant crystal, the value of load capacitance must be
specified. If the application requires a "series" resonant crystal,
load capacitance is not a factor and need not be specified. Load capacitance is
the amount of capacitance measured or computed across the crystal terminals on
the PCB.
Frequency Tolerance
Frequency tolerance refers to the allowable deviation from nominal, in parts per
million (PPM), at a specific temperature, usually +25ƒC.
Frequency Stability
Frequency stability refers to the allowable deviation, in parts per million
(PPM), over a specified temperature range. Deviation is referenced to the
measured frequency at +25ƒC.
Aging
Aging refers to the cumulative change in frequency experienced by a crystal unit
over time. Factors affecting aging are excessive drive level, various thermal
effects, wire fatigue and frictional wear. Circuit design incorporating low
operating ambients and minimum drive level will reduce the aging rate.
Pullability
Pullability refers to the change in frequency of a crystal unit, either from the
natural resonant frequency (Fr) to a load resonant frequency (FL), or from one
load resonant frequency to another. See Figure 6. The amount of pullability
exhibited by a given crystal unit at a given value of load capacitance is a
function of the shunt capacitance (Co) and the motional capacitance (C1) of the
crystal unit.
Figure 6
Equivalent Circuit
The equivalent circuit, shown in Figure 7, is an electrical depiction of the
quartz crystal unit when operating at a frequency of natural resonance. The Co,
or shunt capacitance, represents the capacitance of the crystal electrodes plus
the capacitance of the holder and leads. R1, C1, and L1 compose the
"motional arm" of the crystal and are referred to as the motional
parameters. The motional inductance (L1), represents the vibrating mass of the
crystal unit. The motional capacitance (C1), represents the elasticity of the
quartz and the resistance (R1), represents bulk losses occurring within the
quartz.
Figure 7
Impedance/Reactance Curve
A crystal has two frequencies of zero phase, as illustrated in Figure 8. The
first, or lower of the two, is the Series Resonant Frequency, denoted as (fs).
At this point, the crystal appears resistive in the circuit, impedance is at a
minimum and current flow is maximum. As the frequency is increased beyond the
point of series resonance, the crystal appears inductive in the circuit. When
the reactances of the motional inductance and shunt capacitance cancel, the
crystal is at the Frequency of Anti-resonance, denoted as (fa). At this point,
impedance is maximized and current flow is minimized.
Figure 8
Quality Factor (Q)
The "Q" value of a crystal unit is a measure of the units relative
quality, or efficiency of oscillation. The maximum attainable stability of a
crystal unit is dependent on the "Q" value. In Figure 8 above, the
separation between the series and parallel frequencies is called the bandwidth.
The smaller the bandwidth, the higher the "Q" value, and the steeper
the slope of the reactance. Changes in the reactance of external circuit
components have less effect (less "pullability") on a high
"Q" crystal, therefore such a part is more stable.
Calculation of Load Capacitance
If the circuit configuration is as shown in Figure 5 for the parallel version,
the load capacitance may be calculated by means of the following equation:
| CL = | CL1 * CL2 CL1 + CL2 | + Cstray |
Cstray includes the pin to pin input and output capacitance of the microprocessor chip at the Crystal 1 and Crystal 2 pins, plus any parasitic capacitances. As a rule of thumb, Cstray may be assumed to equal 5.0 pF. Therefore, if CL1 = CL2 = 50pF, CL = 30pF.
Trim Sensitivity
Trim sensitivity is a measure of the incremental fractional frequency change for
an incremental change in the value of the load capacitance. Trim sensitivity (S)
is expressed in terms of PPM/pF and is calculated by the following equation:
| S = | C1 * 1000000 2 * Ct2 |
Where (Ct) is the sum of Co and CL.
Solder Reflow of Surface Mount Devices
Mounting of SMD units is typically accomplished by means of solder reflow, in
Figure 9 either by infrared heat or by vapor phase. The following graphs depict
the recommended times and temperatures for each of the two methods:
Figure 9
Useful Crystal Equations
Oscillator Theory of Operation
Oscillator
Theory of Operation (83 KB)
Crystal controlled oscillators may be considered as consisting of an amplifier and a feedback network that selects a part of the amplifier output and returns it to the amplifier input. A generalized depiction of such a circuit is shown below.
Figure 1.0
In order for an oscillator circuit to operate, two (2) conditions must be met: (A) The loop power gain must be equal to unity. (B) The loop phase shift must be equal to 0, 2Pi, 4Pi, etc. radians.
The power fed back to the input of the amplifier must be adequate to supply the oscillator output, the amplifier input, and to overcome circuit losses.
The exact frequency at which an oscillator will operate is dependent on the loop phase angle shifts within the oscillator circuit. Any net change in phase angle will result in a change in the output frequency. As the usual goal of an oscillator is to provide a frequency that is essentially independent of variables, some means of minimizing the net phase shift must be employed. Perhaps the best, and certainly the most common means of minimizing the net phase shift is to use a quartz crystal unit in the feedback loop.
The impedance of a quartz crystal changes so dramatically with changes in the applied frequency that all other circuit components can be considered as being of essentially constant reactance. Therefore, when a crystal unit is used in the feedback loop of an oscillator, the frequency of the crystal unit will adjust itself so that the crystal unit presents a reactance which satisfies the loop phase requirements. A depiction of the reactance vs. frequency of a quartz crystal unit is shown below.
Figure 2.0
As is apparent from Figure 2.0, a quartz crystal unit has two frequencies of zero phase. The first, or lower of the two, is the series resonant frequency, usually abbreviated as Fs. The second, or higher of the two frequencies of zero phase is the parallel, or anti-resonant frequency, usually abbreviated as Fa. Both the series and parallel resonant frequencies appear resistive in an oscillator circuit. At the series resonant point, the resistance is minimal and the current flow is maximal.
At the parallel point, the resistance is maximal and the current flow is minimal. Therefore, the parallel resonant frequency, Fa, should never be used as the controlling frequency of an oscillator circuit.
A quartz crystal unit can be made to oscillate at any point along the line between the series and parallel resonant points by the inclusion of reactive components (usually capacitors) in the feedback loop of the oscillator circuit. In such a case, the frequency of oscillation will be higher than the series resonant frequency but lower than the parallel resonant frequency. Because of the fact that the frequency resulting from the addition of capacitance is higher than the series resonant frequency, it is usually called the parallel frequency, though it is lower than the true parallel frequency.
Just as there are two frequencies of zero phase associated with a quartz crystal unit, there are two primary oscillator circuits. These circuits are generally described by the type of crystal unit to be used, namely ìseriesî or ìparallel.î
SERIES CIRCUIT:
A series resonant oscillator circuit uses a crystal which is designed to operate
at its natural series resonant frequency. In such a circuit, there will be no
capacitors in the feedback loop. Series resonant oscillator circuits are used
primarily because of their minimal component count. These circuits may, however,
provide feedback paths other than through the crystal unit. Therefore, in the
event of crystal failure, such a circuit may continue to oscillate at some
arbitrary frequency. A depiction of a basic series resonant oscillator circuit
is given below.
Figure 3.0
As is apparent from Figure 3.0, a series resonant oscillator circuit provides no means of adjusting the output frequency, should adjustment be required. In the above circuit, resistor R1 is used to bias the inverter and to cause it to operate in its linear region. This resistor also provides negative feedback to the inverter. Capacitor C1 is a coupling capacitor, used to block DC voltage. Resistor R2 is used to bias the crystal unit. This resistor strongly influences the drive current seen by the crystal unit, therefore care must be taken that too small a value is not chosen. Crystal unit Y1 is a series resonant crystal unit, specified to operate at the desired frequency and with the desired frequency tolerance and stability.
PARALLEL CIRCUIT:
A parallel resonant oscillator circuit uses a crystal unit which is designed to
operate with a specified value of load capacitance. This will result in a
crystal frequency which is higher than the series resonant frequency but lower
than the true parallel resonant frequency. These circuits do not provide paths
other than through the crystal unit to complete the feedback loop. In the event
of crystal unit failure, the circuit will not continue to oscillate. A basic
depiction of a parallel resonant circuit is given below.
Figure 4.0
This circuit uses a single inverter, with two capacitors in the feedback loop. These capacitors comprise the ìload capacitanceî and together with the crystal unit, establish the frequency at which the oscillator will operate. As the value of the load capacitance is changed, so is the output frequency of the oscillator. Therefore, this circuit does provide a convenient means of adjusting the output frequency, should adjustment be required.
The resistors R1 and R2 serve the same functions as detailed for the series resonant circuit shown in Figure 3.0. The two load capacitors, CL1 and CL2, serve to establish the frequency at which the crystal unit and therefore the oscillator will operate. Crystal unit Y1 is a parallel resonant crystal unit, specified to operate with a specified value of load capacitance, at the desired frequency and with the desired frequency tolerance and stability.
LOAD CAPACITANCE:
Reference has been made to a ìspecified value of load capacitance.î Load
capacitance may be defined as ìthat value of capacitance, either measured or
calculated, present in the oscillator circuit, across the connection points of
the crystal.î In the case of a series resonant circuit, there is no capacitance
present between the connecting points of the crystal unit and therefore, load
capacitance need not be specified for a series resonant crystal unit. In the
case of a parallel resonant oscillator circuit, capacitance is present. As a
direct measurement of this capacitance is impractical, it is usually necessary
to calculate the value. The calculation of the value of the load capacitance is
done with the following equation:
| CL = | CL1 * CL2 CL1 + CL2 | + CS (1) |
Where CL1 and CL2 are the load capacitors and CS is the circuit stray capacitance, usually 3.0 to 5.0 pF.
It must be noted that changes in the value of the load capacitance will result in changes in the output frequency of the oscillator. Therefore, if precise frequency control is required, then a precise specification of load capacitance is required. To illustrate, assume that a crystal unit is specified to operate at a frequency of 20.000MHz with a load capacitance of 20.0 pF. Assume that the crystal unit is then placed in a circuit which presents a value of 30.0 pF. The frequency of the crystal unit will then be lower than the specified value. Conversely, should the circuit in question present a value of 10.0 pF, the frequency will be higher than the specified value. The relationship between frequency and load capacitance is shown below.
Figure 5.0
DRIVE LEVEL:
The "drive level" is the power dissipated by the crystal unit while
operating. The power is a function of the applied current, and is usually
expressed in terms of Milliwatts or Microwatts. Crystal units are specified as
having certain maximum values of drive level, which change as functions of the
frequency and mode of operation. It is well to consult with the crystal unit
vendor as to the maximum value of drive level allowed for a particular crystal
unit. Exceeding the maximum drive level for a given crystal unit may result in
unstable operation, increased aging rates, and in some cases, catastrophic
damage. The drive level may be calculated by the following equation:
POWER = (Irms2 * R) (2)
Where I is the rms current through the crystal unit and R is the maximum resistance value of the specific crystal unit in question. Equation (2) is simply ìOhms lawî for power.
Measurement of the actual drive level in an operating oscillator circuit may be accomplished by temporarily inserting a resistor in series with the crystal unit. The resistor must be of the same ohmic value as the crystal unit. The voltage drop across the resistor may then be read and the current and power dissipation calculated. The resistor must then be removed. As an alternative means of measuring the drive level, a current probe may be used at the output lead of the crystal unit, if space permits.
FREQUENCY VS MODE:
The frequency of a quartz crystal unit is limited by the physical dimensions of
the vibrating quartz element. In some cases, the limiting dimension(s) are the
length and width. In the case of the most popular crystal unit, the ìATî cut
crystal unit, the limiting dimension is the thickness of the vibrating quartz
element. As the thickness is diminished, the frequency is increased. At some
point, usually around 30.000MHz, the thickness of the quartz plate becomes too
thin for processing.
Should it be desired to develop an oscillator at a frequency higher than the limiting frequency, advantage must be taken of the fact that quartz crystal units will oscillate at odd integer multiples of their ìfundamentalî frequency. We may define the ìfundamentalî frequency as ìthat frequency which naturally occurs at a given set of mechanical dimensions.î Therefore, if a crystal unit has a fundamental frequency of 10.0MHz, it can also be made to oscillate at 3, 5, 7, etc. times the fundamental. That is, the unit will oscillate at 30.0, 50.0, 70.0, etc. MHz. These multiples of the fundamental frequency are called ìovertonesî and are identified by the integer of multiplication, as in the ìthird overtoneî, the ìfifth overtoneî, etc. When use at an overtone frequency is required, the crystal unit must be specified to operate at the desired frequency and on the desired overtone. One should never attempt to order a fundamental mode crystal unit and then operate it at an overtone frequency. This is so due to the fact that the crystal manufacturing processes differ for fundamental and overtone crystal units.
In many cases, the characteristics of the integrated circuit used in a particular oscillator design dictate that the fundamental frequency of the crystal unit be suppressed in order to ensure operation at the desired frequency and on the desired overtone. In such cases, it is usually necessary to modify the oscillator circuit. One method of modification is to add a ìtankî circuit, consisting of an inductor and a capacitor. These modifications are shown in Figure 6.0 and 7.0
Figure 6.0
Figure 6.0 depicts the modification of a series resonant circuit while Figure 7.0 depicts the modification of a parallel resonant circuit.
Figure 7.0
In both cases, the tank circuit is tuned to resonate at some frequency between the fundamental and the desired frequency. This results in the unwanted frequency being shunted to ground, leaving only the desired frequency being present at the output of the oscillator.
DESIGN CONSIDERATIONS:
For good operation of an oscillator circuit, certain design considerations
should be followed. In all cases, it is recommended that parallel traces be
avoided in order to reduce circuit stray capacitance. All traces should be kept
as short as possible and components should be isolated in order to prevent
coupling. Ground planes should be used to isolate signals.
NEGATIVE RESISTANCE:
For optimum performance, an oscillator circuit must be designed in such a way as
to enhance ìnegative resistance,î which is sometimes called the ìoscillation
allowance.î Evaluation of the amount of negative resistance in a given circuit
is accomplished by temporarily installing a variable resistor in series with the
crystal unit. The resistor should be set initially at its lowest setting,
preferably close to zero ohms. The oscillator is then started and the output
monitored on an oscilloscope. The variable resistor is then adjusted so that
resistance is increased while the output is continuously monitored. At some
value of resistance, oscillation will be stopped. At this point, the variable
resistor is measured to determine the ohmic value at which oscillation ceased.
To this value, the maximum resistance of the crystal unit, as specified by the
vendor, must be added. The total ohmic resistance is deemed to be the ìnegative
resistanceî or the ìoscillation allowance.î For good, reliable circuit
operation, it is recommended that the negative resistance be a minimum of five
times the specified maximum resistance value of the crystal unit.
Values of negative resistance exceeding five times the maximum resistance of the crystal unit are better yet. As negative resistance tends to decrease at elevated temperatures, it is recommended that the test be performed at the highest temperature of the operating range.
FOX Electronics, 5570 Enterprise Parkway, Fort Myers, FL 33905, Phone: 941-693-0099, Fax: 941-693-1554