One Transistor Amplified Microphone

Two Transistor Amplified Microphone plus voice filtering

Super Cheetah "Soft Mute" conversion

2SA1012 to P-Channel MOSFET conversion for Uniden radios for improved ruggedness

Improved AM modulator for Uniden CB radios

Simplified PTT switching for modern CB radios


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One Transistor Amplified Microphone v1.0 © Daz 2010

aka "Power Mike" circuit
 

Capacitors
C1    47 uF 16V Electro
C2    47 uF 16V Electro
C3    2n2 Ceramic
C4    47 nF Polyester
C5    2n2 Ceramic
C6    2n2 Ceramic
C7    100n Polyester

Resistors - all ¼ or ½ watt metal film
R1    100 ohm
R2    100 ohm
R3    10k
R4    470k
R5    1k

Semiconductors
Q1    BC549C

Misc.
SW    Ganged with PTT switch, on during Tx
Electret    2-wire electret microphone insert
 

Circuit operation


Q1 is used as a typical common-emitter small signal amplifier. Bias is applied via R4 to keep the transistor biased near the midpoint. R5 is the output collector load. R1 & C1 filter the supply voltage to reduce turn-on clicks, C2 decouples the supply voltage to the electret mike to prevent feedback via the supply rail. A BC549C transistor is recommended for low noise, and high gain. Gain depends on the individual transistor characteristics, and can be from 15 to 25 dB.  Current consumption is around 5 mA.

C3, C5 and C6 decouple the input and output from nearby RF. This prevents RF feedback from occurring. C3 needs to be placed directly at the rear of the microphone element. Connect the mike element using shielded cable to prevent hum pickup.

The coupling capacitors C4 and C7 have values chosen to reduce low frequency content in the audio below 300 Hz. The values can be changed if required, and aren't critical.

There is no level control in this circuit. Use the transceiver mike gain control instead, or add a 10k pot at the output terminals, wired as a voltage divider (normal volume control).


Two Transistor Amplified Microphone v1.3 with voice filtering © Daz 2010


Capacitors
C1    47 uF 16V Electro
C2    47 uF 16V Electro
C3    2n2 Ceramic
C4    100n Polyester
C5    2n2 Ceramic
C6    120n Polyester
C7    10n Polyester
C8    82n Polyester
C9    47n Polyester
C10  100n Polyester
C11  47n Polyester
C12  2n2 Ceramic
C13  1uF 16V Electro

Resistors - all ¼ or ½ watt metal film
R1    100 ohm
R2    100 ohm
R3    10k
R4    470k
R5    1k
R6    20k
R7    20k
R8    10k
R9    1k

L1    47 mH choke inductor

Semiconductors
Q1    BC549C
Q1    BC549

Misc.
SW    Ganged with PTT switch, on during Tx
Electret    2-wire electret microphone insert
 

Circuit operation


Q1 is used as a typical common-emitter small signal amplifier. Bias is applied via R4 to keep the transistor biased near the midpoint. R5 is the output collector load. R1 & C1 filter the supply voltage to reduce turn-on clicks, C2 decouples the supply voltage to the electret mike to prevent feedback via the supply rail. A BC549C transistor is recommended for low noise, and high gain. Gain depends on the individual transistor characteristics, and can be from 15 to 25 dB. Current consumption is around 9 ma.

C3, C5 and C6 decouple the input and output from nearby RF. This prevents RF feedback from occurring. C3 needs to be placed directly at the rear of the microphone element. Connect the mike element using shielded cable to prevent hum pickup.

The input coupling capacitor C4 reduces low frequency content in the audio below 300 Hz.

There is no level control in this circuit. Use the transceiver mike gain control instead, or add a 10k pot at the output terminals, wired as a voltage divider (normal volume control).

The output filter consists of two stages, a lowpass and a bass notch filter.

Lowpass:
The lowpass filter serves two purposes: It boosts the high frequency content by more than 3 dB, and it sharply cuts frequencies over 3 kHz, which can cause adjacent channel splatter on AM. It is implemented as a type of elliptic filter, which consists of a lowpass filter with a notch added for a sharper cutoff.

Bass notch filter:
The bass notch filter sharply reduces power-hungry low frequency energy around 100 to 200 Hz, without being overly complex.

* revised 20/10/2010 - Buffer amplifier added to output to make unit insensitive to transceiver input impedance

Frequency response plot:


"Soft squelch" conversion for Uniden board CB radios © Daz 2010

This mod works on radios such as: Hatadi Super Cheetah, Stalker 9, Realistic TRC-451, DSE Hornet 2, Galaxy Pluto, RCI 2950 DX... etc.

For reference: IC1 = NJM2902N = LM324 quad OpAmp equivalent

Part numbering is from Pearce Simpson Super Cheetah schematic
Verify that this matches your radio first!

Procedure:
Remove R232 (4M7 squelch hysteresis)
Add 100k resistor from pin 8 to pin 9 on IC1 (linearization)
Add 100n monolithic capacitor from pin 8 to pin 9 on IC1 (smoothing)
Replace C28 22uF with 100n monolithic (faster smoothing)
Replace R40 3k3 with 100k (linearization)
Short out R314 (wire ccw end of squelch control directly to GND) (squelch control range fix)
Add 47k from pin 9 on IC1 to pin 7 on IC1 (direct feed from AGC amp)

Optional: (improved muting response)
Replace TR11 with a VN10KM MOSFET (better linearity) - form leads to fit: D=C G=B S=E
Replace R40 3k3 with 470k (better smoothing)
This makes the muting audio level control more linear.

All resistors Carbon or Metal Film 0.25 or 0.5 watt miniature

This conversion makes the Squelch control into a linear acting mute. Signals are unmuted proportionally to their strength, with no delays. This allows weak signals to still be heard at low volume, and can effectively suppress noise in between words on SSB.
 

 Example Recording (mp3)
 


2SA1012 to IRF4905 MOSFET replacement for Uniden radios for improved ruggedness - added 19/02/2012

Because power MOSFETs are readily and cheaply available, they are widely used as replacements for RF final and driver stages. They can also be used to replace the common PNP modulation transistors with some minor changes, although the distortion levels may be slightly higher. This circuit and variations of it are still being evaluated by the author.

This modification does not increase power, it only makes the modulator stage more rugged, and able to handle higher current demands!
If your radio is working well already, there is nothing to gain from this mod.
If you have had repeated 2SA1012 failures, or are having trouble finding a genuine 2SA1012, this mod is for you!

Disconnect the power to the radio first, as the modulator stage is permanently connected to the 13.8V line!
Remove 2SA1012 bipolar transistor - keep all mounting hardware
Replace 2SA1012 with an IRF4905* or IRF9540 P-channel MOSFET - Carefully clean off mica washer and heatsink surface, then apply new thermal paste and mount MOSFET normally & solder in
Remove TR43 (2SB525) - it is not required
Move R213 (10k) to connect from MOSFET gate to MOSFET source terminals
Add a wire link from MOSFET gate to TR42 (2SC945) collector
Replace R215 (150 ohms 1/2W) with a wire link (ie: short it out)
Add a 220 ohm 1/4W resistor from TR42 emitter to GND
Power up, and using a 50 ohm dummy load, readjust AM POWER for 4 watts average carrier power on AM transmit when unmodulated.
Using a 1kHz sinewave tone, test that AM modulation reaches close to 100% with no major distortion. (use a CRO, or check that no adjacent channel splatter is present)
At 4W average AM carrier power, 100% modulation should be hitting around 16W PEP (typically higher)
Test that close to 13.8V is present on the MOSFET drain terminal in SSB transmit mode

2SA1012 ratings: 5A, 25W, <0.4V Vsat
IRF9540 ratings: 23A, 130W, on resistance = 0.117 ohms
IRF4905 ratings: 74A, 200W, on resistance = 0.02 ohms *preferred choice

Therefore, a P-Channel power MOSFET should be much more rugged than the 2SA1012, and drop minimal voltage in SSB mode.

Part numbering from Super Cheetah schematic:

TR42 amplifies the audio from the microphone amplifier stages, and drives darlington pair TR43 and TR544. Since both the TR42 and TR43/TR544 stages are common emitter, the signal is amplified and inverted twice. Some negative feedback is applied via R212 back to TR42's emitter. This helps reduce distortion and stabilize the DC operating point (AM carrier power).

C183 is originally a 10V rated part, but is subject to over 12V in SSB mode. It should be replaced with a 16V 100uF electro.

A PNP power transistor is used for TR544 to pass the heavy current to the final and driver stages with minimal voltage drop. Low voltage drop is important for maximum peak power capability. This is the reason behind using the 2SA1012, with it's very low Vsat voltage of <0.4V.
 
 

Modified circuit:
This mod was first tested with an IRF9540. but an IRF4905 works better due to lower on-resistance

The modified circuit has TR43 removed, and the TR42 collector connected directly to the MOSFET gate.

R215 is replaced with a short, because MOSFETs are voltage controlled, not current controlled. This means in SSB mode TR45 can switch the MOSFET gate to ground, placing almost the full 13.8V across the MOSFET gate/source junction. This is more than enough to turn TR544 fully on for lowest on resistance, thus allowing the RF final and driver stages to get as close as possible to the full 13.8 volt supply.

Rnew is required to pull TR42's emitter closer to ground so the MOSFET can get sufficient gate drive to turn fully on during positive AM modulation peaks. Unfortunately, this makes the DC operating point of the circuit less stable, and the AM power adjustment more critical.

The distortion performance of this circuit may be inferior to the original configuration for two reasons:

More testing has now been done, and an improved version of this circuit is shown below.


Improved modulator for Uniden CB radios


 

How it works:

The 741 output is coupled to the MOSFET gate via a 180 ohm current limiting resistor (not critical - any value from 100 ohms to 470 ohms should be OK). This stops TR45 directly shorting the OpAmp output in SSB mode.

The P-channel MOSFET functions as a common source inverting amplifier, so the negative feedback goes via a 100k resistor to the non-inverting OpAmp terminal. The 3k3 resistor scales the negative feedback to set the gain. The negative feedback helps linearize the MOSFET for low distortion. The 1uF capacitor degenerates the total gain at DC to produce a stable operating point (carrier power). Because there is no feedback resistor from the OpAmp inverting terminal to the output terminal, the entire OpAmp open loop gain is available at DC to correct for the MOSFET linearity and temperature drift characteristics.

The 100n ceramic capacitor decouples the supply rail at high frequencies to assist stability. The 680p capacitor produces a dominant pole to help stabilize the negative feedback by reducing the gain at frequencies where the system would otherwise be unstable due to phase shifts caused by MOSFET gate capacitance.


Simplified PTT switching for modern CB radios

Since modern CB radios use DC switching for the Rx line, it is easy to use a MOSFET inverter to derive this from the PTT line. This then allows simple SPST switches to do the PTT switching, and any number of them can be connected in parallel.


 

How it works:

The PTT line is normally HIGH at a voltage of about 8 volts. This turns on MOSFET Q1, grounding the Rx line to enable receive. When the PTT line is grounded the transceiver switches to transmit mode, and MOSFET Q1 turns off. Zener diode D1 (18V 400mW) protects the MOSFET gate from damage due to ESD. C1 and C2 (10nF ceramic) keep RF out of the MOSFET.
 



Still to come:

MOSFET final and driver conversions done properly
IRF540 - Applying correct bias and thermal bias compensation, tuning
 

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