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2024年5月11日发(作者:翟清心)

A Rock-Bending Receiver for 7 MHz

This simple receiver by Randy

Henderson, WI5W, originally published in

Aug 1995 QST,is a direct-conversion type

that converts RF directly to audio. Build-

ing a stable oscillator is often the most

challenging part of a simple receiver. This

one uses a tunable crystal-controlled os-

cillator that is both stable and easy to re-

produce. All of its parts are readily

available from multiple sources and the

fixed-value capacitors and resistors are

common components available from many

electronics parts suppliers.

THE CIRCUIT

This receiver works by mixing two

radio-frequency signals together. One of

them is the signal you want to hear, and the

other is generated by an oscillator circuit

(Q1 and associated components) in the

receiver. In Fig 14.61, mixer U1 puts out

sums and differences of these signals and

their harmonics. We don’t use the sum of

the original frequencies, which comes out

of the mixer in the vicinity of 14 MHz.

ing range with crystal pulling made rock

Instead, we use the frequency difference

bendingseem just as appropriate!

between the incoming signal and the

L2’s value determines the degree of

receiver’s oscillator—a signal in the

pulling available. Using FT-243-style

audio range if the incoming signal and os-

crystals and larger L2 values, the oscilla-

cillator frequencies are close enough to

tor reliably tunes from the frequency

each other. This signal is filtered in U2,

marked on the holder to about 50 kHz be-

and amplified in U2 and U3. An audio

low that point with larger L2 values. (In

transducer (a speaker or headphones) con-

the author’s receiver a 25-kHz tuning

verts U3’s electrical output to audio.

range was achieved.) The oscillator’s fre-

How the Rock Bender Bends

quency stability is very good.

Rocks

Inductor L2 and the crystal, Y1, have

more effect on the oscillator than any other

The oscillator is a tunable crystal oscil-

components. Breaking up L2 into two or

lator—a variable crystal oscillator, or

three series-connected components often

VXO. Moving the oscillation frequency of

works better than using one RF choke.

a crystal like this is often called pulling.

(The author used three molded RF chokes

Because crystals consist of precisely sized

in series—two 10-µH chokes and one

pieces of quartz, crystals have long been

2.7-µH unit.) Making L2’s value too large

calledrocksin ham slang—and receivers,

makes the oscillator stop.

transmitters and transceivers that can’t be

The author tested several crystals at Y1.

tuned around due to crystal frequency

Those in FT-243 and HC-6-style holders

control have been said to be rockbound.

seemed more than happy to react to adjust-

Widening this rockbound receiver’s tun-

ment of C7 (TUNING). Crystals in the

Receivers and Transmitters14.61

smaller HC-18 metal holders need more

inductance at L2 to obtain the same tuning

range. One tiny HC-45 unit from Interna-

tional Crystals needed 59 µH to eke out a

mere 15 kHz of tuning range.

Input Filter and Mixer

C1, L1, and C2 form the receiver’s in-

put filter. They act as a peaked low-pass

network to keep the mixer, U1, from re-

sponding to signals higher in frequency

than the 40-meter band. (This is a good

idea because it keeps us from hearing

video buzz from local television transmit-

ters, and signals that might mix with har-

monics of the receiver’s VXO.) U1, a

Mini-Circuits SBL-1, is a passive diode-

ring mixer. Diode-ring mixers usually per-

form better if the output is terminated

properly. R11 and C8 provide a resistive

termination at RF without disturbing

U2A’s gain or noise figure.

Audio Amplifier and Filter

U2A amplifies the audio signal from

U1. U2B serves as an active low-pass fil-

ter. The values of C12, C13 and C14 are

Fig 14.61—An SBL-1 mixer (U1, which contains two small RF transformers and a Schottky-diode quad), a TL072 dual op-amp

IC (U2) and an LM386 low-voltage audio power amplifier IC (U3) do much of the Rock-Bending Receiver’s magic. Q1, a

variable crystal oscillator (VXO), generates a low-power radio signal that shifts incoming signals down to the audio range for

amplification in U2 and U3. All of the circuit’s resistors are

1

/

4

-W, 5%-tolerance types; the circuit’s polarized capacitors are

16-V electrolytics, except C10, which can be rated as low as 10 V. The 0.1-

µ

F capacitors are monolithic or disc ceramics rated

at 16 V or higher.

C1, C2—Ceramic or mica, 10%

L1—4 turns of AWG #18 wire on

3

/

4

-inch

L3—1-mH RF choke. As a substitute,

tolerance.

PVC pipe form. Actual pipe OD is 0.85

wind 34 turns of #30 enameled wire

C4, C5, and C6—Polystyrene, dipped

inch. The coil’s length is about

around an FT-37-72 ferrite core.

silver mica, or C0G (formerly NP0)

0.65 inch; adjust turns spacing for

Q1—2N2222, PN2222 or similar small-

ceramic, 10% tolerance.

maximum signal strength. Tack the

signal, silicon NPN transistor.

C7—Dual-gang polyethylene-film

turns in place with cyanoacrylic

R10—5 or 10-k

audio-taper control

variable (266 pF per section) available

adhesive, coil dope or Duco cement.

(RadioShack No. 271-215 or 271-1721

as #24TR218 from Mouser Electronics

(As a substitute, wind 8 turns of #18

suitable).

(800-346-6873, 817-483-4422). Screws

wire around 75% of the circumference

U1—Mini-Circuits SBL-1 mixer.

for mounting C7 are Mouser

of a T-50-2 powdered-iron core. Once

Y1—7-MHz fundamental-mode quartz

#48SS003. A rubber equipment foot

you’ve soldered the coil in place and

crystal. Ocean State Electronics

serves as a knob. (Any variable

have the receiver working, expand

carries 7030, 7035, 7040, 7045, 7110

capacitor with a maximum

and compress the coil’s turns to peak

and 7125-kHz units.

capacitance of 350 to 600 pF can be

incoming signals, and then cement

PC boards for this project are available

substituted; the wider the capacitance

the winding in place.)

from FAR Circuits.

range, the better.)

L2—Approximately 22.7

µ

H; consists of

C12, C13, C14—10% tolerance. For SSB,

one or more encapsulated RF chokes

change C12, C13 and C14 to 0.001

µ

F.

in series (two 10-

µ

H chokes [Mouser

U2—TL072CN or TL082CN dual JFET op

#43HH105 suitable] and one 2.7-

µ

H

amp.

choke [Mouser #43HH276 suitable]

used by author). See text

14.62Chapter 14

2024年5月11日发(作者:翟清心)

A Rock-Bending Receiver for 7 MHz

This simple receiver by Randy

Henderson, WI5W, originally published in

Aug 1995 QST,is a direct-conversion type

that converts RF directly to audio. Build-

ing a stable oscillator is often the most

challenging part of a simple receiver. This

one uses a tunable crystal-controlled os-

cillator that is both stable and easy to re-

produce. All of its parts are readily

available from multiple sources and the

fixed-value capacitors and resistors are

common components available from many

electronics parts suppliers.

THE CIRCUIT

This receiver works by mixing two

radio-frequency signals together. One of

them is the signal you want to hear, and the

other is generated by an oscillator circuit

(Q1 and associated components) in the

receiver. In Fig 14.61, mixer U1 puts out

sums and differences of these signals and

their harmonics. We don’t use the sum of

the original frequencies, which comes out

of the mixer in the vicinity of 14 MHz.

ing range with crystal pulling made rock

Instead, we use the frequency difference

bendingseem just as appropriate!

between the incoming signal and the

L2’s value determines the degree of

receiver’s oscillator—a signal in the

pulling available. Using FT-243-style

audio range if the incoming signal and os-

crystals and larger L2 values, the oscilla-

cillator frequencies are close enough to

tor reliably tunes from the frequency

each other. This signal is filtered in U2,

marked on the holder to about 50 kHz be-

and amplified in U2 and U3. An audio

low that point with larger L2 values. (In

transducer (a speaker or headphones) con-

the author’s receiver a 25-kHz tuning

verts U3’s electrical output to audio.

range was achieved.) The oscillator’s fre-

How the Rock Bender Bends

quency stability is very good.

Rocks

Inductor L2 and the crystal, Y1, have

more effect on the oscillator than any other

The oscillator is a tunable crystal oscil-

components. Breaking up L2 into two or

lator—a variable crystal oscillator, or

three series-connected components often

VXO. Moving the oscillation frequency of

works better than using one RF choke.

a crystal like this is often called pulling.

(The author used three molded RF chokes

Because crystals consist of precisely sized

in series—two 10-µH chokes and one

pieces of quartz, crystals have long been

2.7-µH unit.) Making L2’s value too large

calledrocksin ham slang—and receivers,

makes the oscillator stop.

transmitters and transceivers that can’t be

The author tested several crystals at Y1.

tuned around due to crystal frequency

Those in FT-243 and HC-6-style holders

control have been said to be rockbound.

seemed more than happy to react to adjust-

Widening this rockbound receiver’s tun-

ment of C7 (TUNING). Crystals in the

Receivers and Transmitters14.61

smaller HC-18 metal holders need more

inductance at L2 to obtain the same tuning

range. One tiny HC-45 unit from Interna-

tional Crystals needed 59 µH to eke out a

mere 15 kHz of tuning range.

Input Filter and Mixer

C1, L1, and C2 form the receiver’s in-

put filter. They act as a peaked low-pass

network to keep the mixer, U1, from re-

sponding to signals higher in frequency

than the 40-meter band. (This is a good

idea because it keeps us from hearing

video buzz from local television transmit-

ters, and signals that might mix with har-

monics of the receiver’s VXO.) U1, a

Mini-Circuits SBL-1, is a passive diode-

ring mixer. Diode-ring mixers usually per-

form better if the output is terminated

properly. R11 and C8 provide a resistive

termination at RF without disturbing

U2A’s gain or noise figure.

Audio Amplifier and Filter

U2A amplifies the audio signal from

U1. U2B serves as an active low-pass fil-

ter. The values of C12, C13 and C14 are

Fig 14.61—An SBL-1 mixer (U1, which contains two small RF transformers and a Schottky-diode quad), a TL072 dual op-amp

IC (U2) and an LM386 low-voltage audio power amplifier IC (U3) do much of the Rock-Bending Receiver’s magic. Q1, a

variable crystal oscillator (VXO), generates a low-power radio signal that shifts incoming signals down to the audio range for

amplification in U2 and U3. All of the circuit’s resistors are

1

/

4

-W, 5%-tolerance types; the circuit’s polarized capacitors are

16-V electrolytics, except C10, which can be rated as low as 10 V. The 0.1-

µ

F capacitors are monolithic or disc ceramics rated

at 16 V or higher.

C1, C2—Ceramic or mica, 10%

L1—4 turns of AWG #18 wire on

3

/

4

-inch

L3—1-mH RF choke. As a substitute,

tolerance.

PVC pipe form. Actual pipe OD is 0.85

wind 34 turns of #30 enameled wire

C4, C5, and C6—Polystyrene, dipped

inch. The coil’s length is about

around an FT-37-72 ferrite core.

silver mica, or C0G (formerly NP0)

0.65 inch; adjust turns spacing for

Q1—2N2222, PN2222 or similar small-

ceramic, 10% tolerance.

maximum signal strength. Tack the

signal, silicon NPN transistor.

C7—Dual-gang polyethylene-film

turns in place with cyanoacrylic

R10—5 or 10-k

audio-taper control

variable (266 pF per section) available

adhesive, coil dope or Duco cement.

(RadioShack No. 271-215 or 271-1721

as #24TR218 from Mouser Electronics

(As a substitute, wind 8 turns of #18

suitable).

(800-346-6873, 817-483-4422). Screws

wire around 75% of the circumference

U1—Mini-Circuits SBL-1 mixer.

for mounting C7 are Mouser

of a T-50-2 powdered-iron core. Once

Y1—7-MHz fundamental-mode quartz

#48SS003. A rubber equipment foot

you’ve soldered the coil in place and

crystal. Ocean State Electronics

serves as a knob. (Any variable

have the receiver working, expand

carries 7030, 7035, 7040, 7045, 7110

capacitor with a maximum

and compress the coil’s turns to peak

and 7125-kHz units.

capacitance of 350 to 600 pF can be

incoming signals, and then cement

PC boards for this project are available

substituted; the wider the capacitance

the winding in place.)

from FAR Circuits.

range, the better.)

L2—Approximately 22.7

µ

H; consists of

C12, C13, C14—10% tolerance. For SSB,

one or more encapsulated RF chokes

change C12, C13 and C14 to 0.001

µ

F.

in series (two 10-

µ

H chokes [Mouser

U2—TL072CN or TL082CN dual JFET op

#43HH105 suitable] and one 2.7-

µ

H

amp.

choke [Mouser #43HH276 suitable]

used by author). See text

14.62Chapter 14

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