Some naturally available crystals (such as, quartz) have the property that their resonant frequencies are constant. Hence a crystal is used as the frequency determining element in an oscillator for high frequency stability. Such oscillator is called a crystal oscillator.
CRYSTAL
OSCILLATOR
The
frequency of LC and RC oscillators may change with time, temperature changes,
etc. Hence the frequency of oscillations does not remain constant. Therefore
the LC oscillators are not suitable high frequency stability requirement.
Some
naturally available crystals (such as, quartz) have the property that their
resonant frequencies are constant. Hence a crystal is used as the frequency
determining element in an oscillator for high frequency stability. Such
oscillator is called a crystal oscillator.
When
a piezoelectric proper alternating potential, vibrates mechanically. The
amplitude of these mechanical oscillations maximum when the frequency of the
applied alternating voltage is equal to the natural frequency of the crystal.
The
equivalent electrical circuit of a vibrating piezoelectric crystal is
represented by a series resonant LCR circuit shunted by a capacitance C', as
shown in fig.1.31(b). The inductance L is the electrical equivalent of the mass
of the crystal. The capacitance C is the electrical equivalent of the
mechanical compliance, and the resistance R represents the electrical
equivalent of the mechanical friction.
The capacitance C' represents the
electrostatic capacitance between the mounting electrodes when the crystal is
not vibrating. C' also induces any capacitance due to the crystal holder. The
values of the L, C, R and C' depends upon the crystal cut, its and the nature
of the vibrations involved.
The
series resonance frequency is given by
fs
= ωs / 2л 1/ 2π √LC... (1)
where
fs is called the series resonant frequency. At this frequency the
impedance of the series arm is resistive and has a low value equal to R.
or
The
parallel resonance frequency fp is given by
The
ratio of C'/C is usually several hundred. Hence Eq. (2) can be written
fp=
1 / 2π √ LC....(3)
Thus
the series resonant frequency fs is very close to the parallel
resonant frequency fp. At fp the crystal offers a very
high impedance to the internal circuit.
The
resonant frequencies of a crystal are inversely proportional to the thickness
of the cut and are different cuts. In general crystal can be used in the
frequency range from about 15 kHz to 10 MHz.
A
crystal oscillator circuit is shown in fig.1.32. In this circuit the crystal
operates in its parallel-resonant mode.
Since
the resistance R of a crystal is very small, the Q (Quality factor) of the
crystal is very high.
Hence the frequency stability of the crystal oscillator is also very high.
1.The
Q factor of a crystal is very high of the order 106 compared to that
of an LC circuit and hence, the frequency of crystal is highly stable.
Thus
fr / Q = bandwidth virtually
becomes zero. The circuit frequency depends upon the crystal resonance
frequency alone.
2.
By changing the crystal different frequencies can be achieved.
3.
The frequency drift can be made less than 1 part in 106.
4.
The rate of change of phase shift θ with angular frequency ω (d θ/d ω) is
large, frequency change is very small even if the phase shift of the circuit
changes.
5.
Crystal oscillator does not need a separat tuned circuit. oals at
1.As the crystal has got a very large Q; the crystal
vibrates only at resonant frequency and does not vibrate at the other
frequencies.
2.
If excessive power is applied, the oscillator waveform basin will be distorted.
3.Overheating
causes frequency drift and the crystal being fragile is likely to fail.
4.
A crystal oscillator is used in low power circuits.
•
Crystal oscillators are used in frequency synthesisers, which have
revolutionised the frequency scene in communication equipment. It is now
possible to have complete systems economically.
•
They are used to generate a chromatic sub-carrier or color sub-carrier in TV
receivers.
•They
got wide applications in microprocessors, microcontrollers, embedded systems,
electronics clocks and watches, frequency and time standards, generates in
radio and computer-clock pulse communication equipment.
Physics for Electrical Engineering: Unit I: Dielectric Materials and Insulation : Tag: : Circuit Diagram, Advantages, Disadvantages, Application, uses - Crystal Oscillator
Physics for Electrical Engineering
PH3202 2nd Semester 2021 Regulation | 2nd Semester EEE Dept 2021 Regulation