Crystal Oscillators

The circuit shown is a standard oscillator of the Colpitts variety. Similar circuits have been used in many ham radio homebrew transmitters. This particular circuit should function well at frequencies from 1500 kHz to 8000 kHz. For stability, C1 and C2 should be disc or silver mica. C3 and C4 can just be ceramic disc. At lower frequencies, the values of C1 and C2 might need to be increased.

C1: 100 pF ceramic disc or silver mica
C2: 680 pF ceramic disc or silver mica
C3: .01 uF ceramic disc
C4: .001 uF ceramic disc
Q1: 2N3904
R1: 220 K
R2: 1 K
   
Enhanced Crystal Oscillator

Below is another version of the circuit with a couple of enhancements. The variable capacitor between the crystal and ground allows you to adjust the frequency slightly. (More capacitance equals lower frequency.) Q2 serves as a buffer amplifier which stabilizes the circuit and boosts the output power. This circuit was developed independently by another MWA member and uses very different values for R1, C1 and C2 compared to the first circuit on this page; don't let those differences scare you.

R1: 22 K
R2, R6: 1 K
R3: 18 K
R4: 270 K
R5: 470 K
C1, C4, C5: .001 uF
C2: .0033 uF
C3: 20 to 50 pF
Q1, Q2: 2N3904
   

Another common variation of the Colpitts circuit involves adding a resistor parallel to the crystal, as shown below. What's the advantage? I have no idea. The circuit shown has been tested and works fine at frequencies from 1.5 to 20 MHz.

Pierce FET Oscillators

To round out the collection, here's a Pierce oscillator using an FET. The version on the left is from an electronics textbook. The version on the right is from the "Grenade" shortwave pirate radio transmitter designed by "Radio Animal."

VFO

On the right is a drawing for a VFO (Variable Frequency Oscillator) that can replace a crystal oscillator. A VFO would allow you to operate across a range of frequencies, without investing in a lot of crystals.

L1 C1 Min C1 Max C2 C3
µH pF pF pF pF
Frequency Minimum
xxx
Frequency Maximum
xxx
F Delta
xxx

On the drawing, C1 is a small Air-Dielectric Variable Capacitor and would be your main tuning. C2, and C3 set your main tuning range. For temperature stability, those capacitors should be Polystyrene. With the values listed in the drawing, the tuning range will be approximately 1641-1711 kHz tuning range (about 70 KHz). Changing C3 to 100 pF will change the tuning range to 1565-1625 kHz (about 60 KHz). The small calculator above can be used to find out the tuning range for a different set of capacitors.

C1:4 to 20 pF, air-dielectric variable capacitor
(such as Antique Electronic Supply catalog number C-VT20)
C2:100 pF Polystyrene
C3:82 pF Polystyrene
(for approx. 1640-1700 kHz tuning range or
or 100 pF polystyrene (for 1570-1630 kHz tuning range)
C4, C5:1000 pF
C6:.01 uF ceramic disk
C7:50 pF polystyrene
D1:1N914
L1:47 uH inductor
Q1:MPF102
R1:100 K, 1/4 watt
R2:470 ohm, 1/4 watt
RFC:1 millihenry choke
VR1:any 8 or 8.2 volt, 1/2 watt zener diode (such as NTE 5016A)

There are 4 keys to building a stable VFO:

1. Use a regulator IC or a zener diode to regulate the voltage going to the oscillator. Voltage fluctuations produce frequency drift.

2. Build the circuit carefully. Keep component leads short, do your best soldering work, and make sure all the components are physically secure (no wiggling).

3. Choose your inductor and variable capacitor carefully. Air-core inductors are more stable across a range of temperatures than iron-core inductors. Air-dielectric variable capacitors are more stable than mica compression and other types.

4. Put a buffer amplifier between the VFO's output and the rest of the transmitter. Failure to do this makes the VFO vulnerable to being "pulled" by modulation, by changes in antenna loading, etc.

The circuit shown here is a series-tuned Clapp oscillator. Unlike the parallel LC tanks seen in many oscillators, this one has the LC components in series. Similar VFOs have been used successfully in many ham radio transmitters and receivers.

PLL
Buffer Amplifiers
C1:0.01 uF
C2:0.1 uF
R1:27 K
R2:5600
R3:22 ohms
R4:270

A buffer amp can be inserted between the oscillator and the rest of a transmitter circuit. The buffer not only increases the power of the signal but also prevents the oscillator frequency from being affected by modulation, changes in antenna loading, etc.

Above is the simplest buffer amp we could dig up. It is designed to work with a 9 volt power supply.


Q1, Q22N2222A2N3904
R110047
R21 K1 K
R310 K10 K
R4220010 K
R510 K22 K
R6330330
C1.1 uF.1 uF
C2.01 uF.01 uF

Above is a deluxe buffer amp that uses a pair of bipolar transistors. Some of the resistor values are a little different depending on whether it is built with 3904's or 2222's.

Simple Modulators for Solid-State Transmitters

Simple AM modulators work by varying the amount of power flowing through the transistor which is serving as the RF output amplifier. By imposing an audio waveform on the power supply, amplitude modulation is achieved.

Rather than giving detailed examples, this page gives simplified schematics, followed by links to circuits that actually use the various techniques.

An external audio amp sends its output to the 8-ohm side of an 8-to-1000 ohm (or similar) audio transformer. The other winding of the transformer is inserted in the power supply going to the final RF amp transistor. The audio transformer must be rated to handle the level of power going through it. An inadequate transformer will produce a bad-sounding signal. In some cases it takes a lot of searching and experimentation to find the best transformer.

Simple Modulators for Solid-State Transmitters - technique #2-A

A lightly amplified audio signal is fed to the base of an NPN transistor. This transistor is inserted into the power supply going to the RF amp transistor. A choke between the two transistors keeps RF out of the power supply and audio circuitry. The RF choke must be rated to handle the level of current going through it.

Simple Modulators for Solid-State Transmitters - technique #2-B

A line-level audio signal is fed to an audio amplifier I.C. The output of this chip is used as a power supply for the RF amp transistor.

This circuit is physically smaller and lighter than designs that use a modulation transformer. The audio quality is good.

Simple Modulators for Solid-State Transmitters - technique #3

The RF output transistor is an FET (often an IRF510 or similar). The FET's source is grounded. The FET's drain is connected to a transformer, which has the modulation (audio) amp on one side and the RF output taken from the other side.

Simple Modulators for Solid-State Transmitters - technique #4

This is the system used in Charles Wenzel's circuit. This design has had many re-incarnations, for example in a proposed 13.5 MHz transmitter circuit. The Wenzel modulator is capable of high quality modulation at levels approaching 100%. For 100 milliwatt transmitters, suitable transistors are 2N4401 or 2N5551.

Finals

The Final (aka Power Amp, Output Amp) is the final stage of a tansmitter. This stage generally has some gain (voltage and current). Shown here are some partial schematics of finals taken from a wide variety of sources. Unless otherwise noted the input is on the left side, output on the right.

This circuit will output 1.2 watts with a 13.8 volt power supply. Value of RFC not critical, but must be able to handle some current, try 15 turns of wire on a toroid core.


This circuit will output 4 to 5 watts with an adequate power supply. The design shown is optimized for 7 MHz; the transformers may need a bit of modification to optimize for other bands. Heat-sinks hould be provided for the transistors.

Low-pass filters
Transmit RangeC1C2L1
1500-2000 kHz1800 pF1800 pF30 turns, #26 wire on T-50-2 toroid
3500-4500 kHz 680 pF680 pF21 turns, #22 wire on T-50-2 toroid
5500-7300 kHz470 pF470 pF14 turns, #22 wire on T-50-2 toroid
5500-7300 kHz820 pF820 pF2.2 µH

A low-pass filter attentuates the energy above a specified cut-off frequency. These filters are used to reduce the intensity of harmonics so that they don't interefere with other signals. Most of this filters on this page were designed for various ham radio gear operating in the bands from 1.8 to 14 MHz.

Unless otherwise noted these filters have 50 or 52 ohms input and output impedance. Capacitances are expressed in picofarads, inductances in microhenries. Most authors recommend using silver-mica capacitors.


approx.
cutoff freq.
C1C2C3L1, L2
1200 kHz.0039 µF.0056 µF.0039 µF6.8 µH
1800 kHz0033 µF.0043 µF.0033 µF5.6 µH
2000 kHz1592 pF3184 pF1592 pF3.98 µH
7300 kHz470 pF1000 pF470 pF42 turns,
#26 wire
on T-50-2

Cutoff
Frequency
30 dB
Attenuation
Point
C1,/C4 C2,/C3 L1,/L3 L2
2.16 MHz4.0 MHz820 pF2200 pF4.44 µH5.61 µH
4.12 MHz7.3 MHz470 pF1200 pF2.43 µH3.0 µH
7.36 MHz12.9 MHz270 pF680 pF1.38 µH1.70 µH
10.37 MHz15.8 MHz270 pF560 pF1.09 µH1.26 µH