Circuit A shows a 27MHz transmitter circuit without a crystal. The main reason for a crystal is to comply with the strict transmitting laws in most countries. A fairly narrow band has been allowed at 27MHz and to keep within this area, a crystal has been used. Since a crystal is not an expensive component when bought in the millions, manufacturers have included them in their circuits to get instant approval.
However the important reason for using a crystal is to get reliable operation.
When a circuit does not have a crystal, the oscillator is said to be “voltage dependent” or “voltage controlled” and when the supply voltage drops, the frequency changes.
If the frequency drifts too much, the receiver will not pick up the signal.
For this reason, a simple circuit as shown in circuit A is not recommended. We have only included it as a concept to show how the 27MHz frequency is generated.
The two transistors are doing two things at the same time. The second transistor is a self-contained oscillator and it gets its feedback (to oscillate at 27MHz) from the transformer. The main coil is the 8t section and the feedback to the base is 4 turns.
The first transistor is also connected to the second transistor and the two form a low-frequency oscillator in which the first transistor forms the timing for the oscillator and the second transistor provides positive feedback.
The first transistor turns on via the 1M and the transistor sees this as pulling the base “down.” The collector of Q1 pulls the base of Q2 “up” and Q2 turns ON. This causes current to flow in the 100R and the voltage on the right side of the 6n8 falls. The capacitor tries to make the left side fall too and turn on the first transistor even more. This happens until Q1 cannot turn on any more and the 6n8 charges a little more. This turns off Q! a small amount and the to transistor begin to turn off.
The frequency of the tone is determined by the value of the 6n8. All the time that this is happening, Q2 is oscillating at 27MHz and it is just being “DC shifted” up and down.
The tone consists of short spikes, unlike the tone produced by Circuit B, which has an almost even mark-space ratio.
The second circuit comes from a GS Remote Control Car. It does not have the 2k2 current-limiting resistor and you can experiment to see which circuit consumes the least current and has the best range.
See [GS Remote Control Car Receiver Circuit](#GS REMOTE CONTROL RECEIVER) below.
A 27MHz transmitter
(receiver for this circuit [HERE](GS REMOTE CONTROL RECEIVER))
Circuit A - Birds Nest
Circuit A was quickly constructed on a piece of copper board to act as an earth plane and to make sure it worked and to see if any improvements could be made. If a circuit works well in an open format such as this, you can be sure it will work better when constructed on a printed circuit board where the circuit is much “tighter” and the impedances are lower. The layout above is called a “Birds Nest” and allows rapid modifications to be made and you can touch the parts to see if your hand capacitance changes the frequency or stops the circuit working.
Circuit B also produces a tone. But this time two transistors are used in a multivibrator arrangement, in which one of the transistors is used to turn the third transistor on and off.
Circuit A is a very efficient and clever circuit and requires less components. That’s why you must study all types of circuits before producing your own design as simplicity is the secret to success.
The tone is used by a receiver to determine the signal is coming from the chosen transmitter. The receiver can have a detector stage to detect the exact frequency or the tone can be used to change the state of a stage. This is called integration, where the energy from the pulses from the tone are added together to charge or discharge a capacitor.
Circuit B comes from a Russian design, and it uses Philips transistors!
We tested the output with our Field Strength Meter MkII and found it had a good output. Details of Field Strength Meter MkII are discussed below.
But the circuit has some poor features. The poorest feature is the printed-circuit coil. This type of coil has the lowest value of “Q.” “Q” is the name for the “Quality factor” for a coil and it effectively determines how much amplitude you will get. Quite often the output of a coil will be higher than the voltage being supplied to it and this gives the value of “Q.”
The other poor design is turning the emitter of the third transistor on and off. A better solution is to drive the base as has been done in Circuit A. This allows full voltage to be applied to the stage.
Here is the circuit:
The topside of circuit B
The underside of circuit B
Circuit B consists of two blocks. Block 1 is a multivibrator and this has an equal mark/space ratio to turn the RF stage on and off.
We have covered the operation of a multivibrator in the electronics course on Talking Electronics website, in the subscription section.
The only thing you have to know for this circuit is the fact that the middle transistor turns on for 50% of the time and the voltage between the collector and emitter drops to less than 0.3v This voltage is too low for the third transistor to operate and thus the RF stage is turned off.
The second building block is the RF oscillator.
The actual operation of the stage is very complex and beyond the scope of this discussion. However some of the points are as follows:
The feedback to keep the stage operating is provided by the 27p capacitor.
The frequency-producing items are the coil (made up of the full 7 turns) and the 47p air trimmer. These two items are called a parallel tuned circuit. They are also called a TANK CIRCUIT as they store energy just like a TANK of water and pass it to the antenna.
The base is kept rigid by both of the 4n7’s. In other words, the base does not move.
The stage is turned on by the 22k and 15k voltage dividers. A voltage of 5v is produced at the join of these two components. The voltage on the emitter will be 0.6v lower.
This will cause current to flow in the 220R and also in the 3t winding. These turns will produce magnetic flux that will cut the other 4 turns and produce a voltage in them. This energy will pass to the antenna and some of it will charge the 47p and in doing so the voltage on the collector will reduce. This voltage will be passed to the emitter via the 27p and this will turn the transistor on more. This will continue until the coil cannot produce any more voltage and the transistor will begin to turn off. The collapsing magnetic flux in the 3 turns will cut the 4 turns and produce a voltage in the opposite directions and the other half of the cycle will be produced.
The frequency of the circuit is adjusted by the 47p air trimmer.
The following receiver matches up with Circuit B above.
27MHz Receiver
The circuit consists of a number of building blocks and these can be identified when a capacitor separates one stage from another.
The first stage is actually a 27MHz oscillator with a very small output due to the 4k7 resistor connecting the stage to the positive rail. This allows very little current to enter the stage and the transistor operates on a very “delicate basis.”
When a circuit is oscillating and delivering a signal to the air surrounding the antenna, any other signal entering the same surroundings will cause an interference with the generated signal and the circuit will find it more-difficult to deliver a signal, especially when the signal has the same frequency. This will cause the voltage on the collector of the transistor to alter and produce a signal that can be passed to further stages of amplification.
The 5v1 zener is designed to keep the voltage on the first stage constant as the transistor is oscillating and is a voltage-controlled oscillator.
All the components in the first stage are designed to make it very sensitive to detecting a signal.
Normally, all the surrounding signals upset the clean sine-wave produced by the stage and the result is a lot of “noise” or “hash” or “background noise” at the “pick-off” point.
If the 27MHz signal produced by a transmitter contains a tone, this tone will appear at the “pick-off” point along with the hash.
The frequency of the hash is fairly high and on the second stage there are three components to remove it.
The first is the 1k5 resistor. This, in combination with the 47n, has a slight effect.
Next, the 15n between base and ground will remove high frequencies. And finally the 2n2 will send any amplified signal back to the base for cancellation. This capacitor has a greater effect on canceling high frequencies.
The third and fourth stages also remove some of the high frequency component of the signal and the result is a clean signal with only the tone appearing on the base of the fourth transistor.
This signal has a large amplitude and will turn the transistor on fully.
The transistor normally sits with the collector very close to rail voltage due to the low value of collector resistor and this means transistor Q5 is not turned on.
The 47u gets charged via the 1k5 resistor and the relay is not energised.
When the fourth transistor sees a tone, it turns on at the frequency of the tone and this puts pulses of short-circuit across the 47u and it rapidly discharges.
As it discharges, the voltage on the collector drops and this turns ON Q5 to operate the relay.
When the tone stops, the 47u rapidly charges via the 1k5 and the relay switches off.
The photo below shows a switch added to the PC board and a LED connected to the output of the relay to test the receiver.
The pot in the centre of the board adjusts the sensitivity of the receiver.
Receiver for transmitter in Circuit B
The relay can be latched ON via the following circuit but it cannot be turned on remotely. The power has to be disconnected to release the relay. This is only suitable for a “one-shot” operation where a device has to be turned on only once.
Relay turns ON and stays ON (Latching Circuit)
If a long tone is required to turn on the relay (to prevent false triggering), the following circuit can be used. The 100u electrolytic takes about 2 seconds to discharge via the 10k resistor, as the 4k7 adds to the time-delay, since it is providing charging-current that the transistor has to overcome.
2-second tone to turn relay ON
The following circuit allows a single channel transmitter/receiver to turn an appliance on and off by sending a short pulse to turn a circuit on and a long pulse to turn a circuit off.
This is handy when you cannot see the result of your operation. A simple toggle operation is not suitable as you do not know the state of the output at the start of the operation.
By sending a long pulse, you definitely know the output will be OFF and you can then control the output remotely.
A short pulse is less than 0.25 sec and a long pulse can be any length longer than 1 second.
These times can be adjusted by changing the value of the components.
When a short tone is received, the lower 47u discharges and pulls the base of the BD136 towards the 0v rail and turns the transistor ON. This activates the relay and the contacts take the 4k7 to the 0v rail to keep the transistor ON.
During this time the top 47u charges via the 100k but not enough voltage appears across it to turn on the BC557 transistor.
If the tone appears for a long period of time, the top 47u charges and turns on the BC557 and the voltage between the emitter/collector terminals is less than 0.3v. This voltage is too low for the BD136 to remain on and it turns off.
When the tone is turned off, the BC557 remains on for 1 second and then turns off.
The circuit is then ready to be activated again.
Short tone = ON Long tone = OFF
The circuit above can be added to many different receiver circuits, thus using only one output to provide an on/off function.
This circuit is the receiver for GS Remove Control transmitter shown in [Circuit “A”](#CIRCUIT A) above.
The purpose of presenting a number of circuits is to show the basics of how this type of circuit works.
The secret behind a receiving circuit is to create a “front-end” that is actually oscillating at the frequency to be detected and it transmits a very weak signal out the antenna. When a signal of the same frequency is detected by the front-end it takes more current and less current according to the tone being carried by the 27MHz signal (as the tone is actually increasing and decreasing the strength of the signal). This amplitude appears on the output of the “front-end” and is picked off via the 39n capacitor. It is then amplified by two stages. The 10n on the collector of the second transistor is designed to remove the “hash” or background noise. This signal then turned into a DC voltage by charging a 1u electrolytic and the negative portions of the signal are removed by the diode. When no signal is detected, the transistor is not turned on and the motor operated in the forward direction. A signal turns on the transistor and the other two transistors in the half-bridge are turned ON to reverse the motor.
(transmitter for this circuit [HERE](#CIRCUIT A))
The next circuit is a 2 channel transmitter.
This circuit does not use a crystal but has a clever feature of using the two push buttons to turn the circuit on when it is required to transmit.
Click HERE for RX-3 IC datasheet .pdf
We have already discussed the operation of a circuit such as this, with a multivibrator and RF oscillator. The only new feature is the arrangement for producing two different tones.
The receiver requires a 1kHz and 250Hz tone for the forward and reverse outputs. The frequency of the multivibrator is determined by the value of resistance on the base of each transistor. The multivibrator is driven directly from the supply with the forward button and via a 150k for the reverse frequency.
2 Channel Transmitter PC board
Circuit for the RX-3 IC
The circuit for the receiver has not been taken off the printed circuit board, however a general circuit is provided in the datasheet for the IC and this has been reproduced above.
Both output of the chip cannot be HIGH at the same time as this will destroy the transistors in the “H-bridge.”
For the forward direction, the forward output is HIGH and this turns on Q9, Q11 and Q13.
For the reverse direction, the backward output is HIGH and this turns on Q8, Q10 and Q12.
This toy remote control car cost less than $8.00, but a defect in the design was noted.
The motor would reverse approx every 2 minutes for a short period of time, even though no transmitter button was pressed and the motor would operate in bursts when the car was distant from the transmitter. The interference was not from any electronic device in the home as the receiver was taken to an open space and it still faulted. The first transistor was removed and the fault did not occur. This means the RF transistor is generating a fault that is detected by the chip to turn on an output.
This could be due to the chip detecting a frequency of 1kHz or 250Hz to turn on an output. Random noise could be in this range and that’s why the RX-3 receiver chip is unreliable.
Maybe that’s why the car was $8.00!
Another point of comparison: the RX-3 receiver circuit consumed 4.4mA at 4.5v, while the RX-2B receiver consumed 0.7mA at 3v.
This circuit uses the TX-2B RX-2B chipset discussed on the previous page. The chip has 5 channels and the circuit uses 4.
Click HERE for TX-2B RX-2B chipset datasheet .pdf
4-Channel Transmitter PC Board
TX-2B circuit on datasheet
The receiver using the RX-2 chip:
4-Channel Receiver PC Board
RX-2B circuit on datasheet
There are five pieces of test equipment you can buy or build to test the output of a transmitter.
When working with a transmitter, the first thing you will want to do is determine if the transmitter is producing RF.
Talking Electronics has three kits for this.
LED Power Meter connected to a mini multimeter
The multimeter in the photo has a sensitivity of 2,000 ohms per volt.
This means the resistance inside the meter is 20,000 ohms when the pointer is on the 10v scale.
This type of meter is called a low sensitivity instrument and is ideal for the job we are doing.
If a high impedance instrument is used, it can pick up stray RF and produce a false reading.
A high impedance instrument can be 20,000 ohm per volt, 50,000 ohms per volt or 100,000 ohms per volt (commonly called a FET meter.)
Digital multimeters can have higher input impedances.
FIELD STRENGTH METER MkII Modification
FIELD STRENGTH METER MIII
Field Strength Meter MIII Circuit
The 100p and 18 turn coil form a tuned circuit that oscillates at a particular frequency. The frequency at which the components oscillate is changed slightly by the 47p air trimmer. The signal then passes into a 2-diode rectifier with one diode passing the voltage to the meter and the other diode discharging the 47p on the negative half of the waveform. The 100n across the meter stores and smoothes the voltage for the 1mA (Full Scale Deflection) movement.
This circuit shows the amazing ability for two passive components to “amplify.” The 100p and 18 turn coil form a TUNED CIRCUIT and when the incoming frequency is exactly the frequency at which these two components oscillate, the output rises considerably.
If you have transmitter, you can set up the circuit to detect an exact frequency by winding the 10cm tinned copper wire antenna around the antenna of the transmitter. Each centimetre gives about 2p of capacitance and this is sufficient to connect the two together “RF wise.”
The circuit requires 18 turns but if you add one turn, you can stretch the coil to get the circuit to peak then remove it later.
Finding the resonant frequency of the coil and capacitor is a very difficult thing to do as the peak comes and goes in less than 1/10mm of stretching the coil.
In addition, you cannot touch the coil or be anywhere near the circuit when making the adjustments as you body completely “soaks away” the energy.
You have to use a plastic knitting needle and move the end turn very slowly while watching the meter.
You will see it move from zero to more than half way as the adjustment is made.
You now have a piece of test equipment that will indicate when a transmitter is operating at an exact frequency.
If you want to know if the transmitter is producing RF, you will need Field Strength Meter MkI as it purely detects RF.
Talking electronics has designed a PC board with Field Strength Meter circuit to detect 27MHz. Most of these transmitters are very low power and getting a reading on a meter (actually called a “movement”) is very difficult.
To help get a reading we have added a transistor amplifier.
The result is: 27MHz FSM
Click HERE to go to the project.
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