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| United States Patent | 4139826 |
| Link to this page | http://www.wikipatents.com/4139826.html |
| Inventor(s) | Pradal; Bortolo M. (Pittsburgh, PA) |
| Abstract | An overtone oscillator of the feedback type is provided by a transistor, a
crystal resonant at a fundamental frequency and higher odd overtone
frequencies, and a feedback circuit that includes the crystal, a second
transistor connected in cascade with the first transistor and an RC
network. This feedback circuit provides the correct phase shift to achieve
and sustain oscillations at the desired overtone frequency. |
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Title Information  |
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Drawing from US Patent 4139826 |
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Crystal overtone oscillator using cascade connected transistors |
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| Publication Date |
February 13, 1979 |
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| Filing Date |
December 27, 1977 |
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Title Information  |
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References  |
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| Market Size |
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Estimate the gross annual revenues of the relevant market
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| Market Share |
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| Reasonable Royalty |
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Public's "Guesstimation" of Royalty Value
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| Market Size | N/A | [No votes] | | x | Market Share | N/A | [No votes] | | x | Reasonable Royalty | N/A | [No votes] |
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Market Review  |
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Technical Review  |
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Claims  |
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What is claimed is:
1. An overtone crystal oscillator comprising:
a first transistor including a base, emitter and collector electrodes,
a crystal having natural resonances at a fundamental frequency and higher
odd overtone frequencies,
feedback means including a second transistor and said crystal connected in
series between the collector electrode of said first transistor and the
base of said first transistor for providing sufficient gain and phase
shift at a selected overtone frequency to achieve oscillation at the
overtone frequency, said second transistor providing about 180.degree.
additional phase shift at the desired overtone frequency.
means coupled to the electrodes of said first and second transistors for
biasing said first and second transistor as an amplifier,
said biasing means including current negative feedback means for peaking
the gain at the desired overtone frequency.
2. The combination of claim 1 wherein said feedback means further includes
a capacitor and resistor connected in series for peaking the gain and
providing additional phase shift at the desired overtone frequency.
3. The combination of claim 2 wherein said capacitor is an adjustable
capacitor.
4. The combination of claim 3 wherein said adjustable capacitor is a
varactor.
5. The combination of claim 2 wherein said resistor is adjustable.
6. The combination of claim 1 wherein said second transistor has its base
electrode coupled to the collector of said first transistor and its
collector electrode coupled to said crystal.
7. An overtone crystal oscillator comprising:
first and second transistors with the second transistor connected in
cascade to the output of the first transistor,
means for biasing said transistors as amplifiers,
a piezoelectric crystal having natural resonances at the fundamental and
the odd overtone frequencies, an RC network coupled to the base of said
first transistor for peaking the gain and the phase at the desired
overtone frequency, said crystal connected between the collector output of
the second transistor and the RC network for together with the RC network
and the second transistor providing feedback with sufficient gain and
phase shift to the base of the first transistor to achieve oscillation at
the desired overtone frequency,
said biasing means including current negative feedback means for peaking
the gain at the desired overtone frequency. |
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Claims  |
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Description  |
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BACKGROUND OF THE INVENTION
This invention relates generally to oscillators and, more particularly, to
crystal controlled overtone oscillator circuits having means for assuring
that the oscillator operates at a desired overtone frequency.
Overtone oscillators are well known in the prior art. The prior art
overtone oscillators usually have adjustable inductances in the feedback
path to prevent oscillation at lower overtone frequency and achieve the
additional phase shift at the overtone frequency. See for example Irwin et
al U.S. Pat. No. 3,875,533. The use of the inductance in the feedback
introduces a temperature drift since a typical adjustable coil drifts
about 400 ppm (parts per million) per degree celsius. It is therefore
desirable to provide an overtone oscillator without the use of this
feedback coil.
Although overtone oscillators of the negative resistance type as described
in U.S. Pat. No. 3,512,107 of Miyake et al do not use an inductance, such
circuits operate on the negative resistance principle and only at
frequencies below 20 MHz with a narrow operating frequency range. The
negative resistance type oscillator is very sensitive to multiple
oscillation or frequency jumping between fundamental and overtone modes
and/or at crystal spurious frequencies.
SUMMARY OF THE INVENTION
Briefly, an overtone oscillator without using an inductance coil or
operating in the negative resistance region is provided by a first
transistor and a second transistor and a crystal with the second
transistor connected in cascade to the output of the first transistor and
the crystal having a natural resonance at a fundamental frequency
connected between the collector output of the second transistor and the
base input of the first transistor. The second transistor provides
additional gain and phase shift to the base input of the first transistor
to provide oscillation at the desired overtone frequency. The transistors
are biased as amplifiers for providing peaked gain at the desired overtone
frequency.
DESCRIPTION OF DRAWING
The sole FIGURE is a schematic drawing of the oscillator according to one
embodiment of the present invention.
DESCRIPTION OF THE INVENTION
Referring to the FIGURE, a transistor 10 is coupled in cascade with
transistor 11. The collector 10a of transistor 10 is coupled via resistor
13 and an isolating impedance or choke 14 to a D.C. power supply at
terminal 16. Similarly, the collector 11a of transistor 11 is coupled via
resistor 15 to the same D.C. source. The base bias for transistor 10 is
provided by the voltage dividing resistors 17 and 19. Similarly, the D.C.
bias to the base 11b of transistor 11 is provided by voltage dividing
resistors 21 and 23. The emitter 10c of transistor 10 is coupled to ground
or reference potential via resistor 25. This resistor 25 is bypassed by a
capacitor 27. Similarly, the emitter 11c of transistor 11 is coupled thru
a resistor 29 to ground or reference potential and has a bypass capacitor
31 coupled thereacross. The signal at the collector 10a of transistor 10
is coupled via coupling capacitor 33 to the base 11b of transistor 11. The
two cascade connected transistor stages 10 and 11 have current negative
feedback determined by the value of the resistors 25 and 29 and the
capacitances 27 and 31 coupled thereacross. The output signal at the
collector 11a of transistor 11 is coupled via coupling capacitor 49 to the
output terminal 60. Positive feedback for the oscillator is provided via
the crystal 50 to the input terminal of varactor diode 45. Sufficient gain
is provided by the transistor stages 10 and 11 to enable oscillation at
the desired overtone frequency. A resistor 51 is coupled between the anode
terminal of varactor 45 and ground or reference potential. The value of
the resistance of resistor 51 together with the capacitance of the
varactor 45 is adjusted such that at the desired overtone frequency there
is exactly 360.degree. phase shift between the collector of transistor 10
and the input at the base of transistor 10. The value of the capacitance
of varactor 45 is determined by the D.C. voltage applied at the input
terminal 41. Alternatively resistor 51 can be made variable to extend the
tuning range of the circuit and/or to adjust crystal frequency. Cascade
connected transistor 11 provides about an extra 180.degree. phase shift.
The crystal 50 is designed at a selected given fundamental frequency. For
the example this frequency is about 13 MHz. The value of resistor 51
together with the capacitance of varactor 45 is adjusted such that at for
example the third overtone frequency of 39 MHz, there is exactly
360.degree. phase shift. In addition, the capacitance values at the
emitters of transistor stages 10 and 11 -- the values of capacitors 27 and
31 in the FIGURE -- are adjusted such as to provide peaking of the
amplification at the desired overtone frequency and to provide
insufficient gain and lesser phase shift because of the current negative
feedback at the fundamental frequency. Further, the value of the A.C. load
resistances (load resistor 55) are adjusted to provide peaking at the
overtone frequency. Input signals to be modulated are applied to the
oscillator at input terminal 41. These input signals are applied via
resistor 43 to varactor diode 45. These signals are then coupled via
coupling capacitor 47 to the base 10b of transistor 10. For example, in
the above described arrangement when operating a crystal with the
fundamental frequency at 13 MHz, the circuit had the following parameters:
Transistors 10, 11 = 2 N2857
Resistors 17, 21 = 11K .OMEGA.
Resistors 19, 23 = 10K .OMEGA.
Resistor 13 = 1K .OMEGA.
Resistor 15 = 1.5K .OMEGA.
Load resistor 55 = 50 .OMEGA.
For the third overtone resistor 51 = 877.OMEGA. with capacitor 27 being 110
pF.
Resistor 29 = 1K .OMEGA.
Capacitor 31 = 560 pF
Varactor 45 = type KV2002 varactor diode sold by KSW Electronics of
Burlington, Mass., with the D.C. biasing level thereto being +5 D.C. thru
a 100K .OMEGA. resistor 43. The D.C. voltage at the biasing terminal 16 is
+8 V D.C. For the fifth overtone, the resistance of resistor 51 is
selected to be 47 .OMEGA. and the capacitor 27 is 68 pF. A variable
resistor, electronically controlled such as FET transistor, or a manually
adjustable resistor, can replace resistor 51 to tune the desired overtone.
* * * * *
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Description  |
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