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An AM/FM/CW Sc
RF Signal Genera
This low-cost, easy-to-build and user-friendly RF signal generator
covers from 100kHz–50MHz and 70–120MHz, and is usable up to
150MHz. It generates CW (unmodulated), AM and FM signals suitable
for a wide range of tests. Its output level is adjustable anywhere
between -93dBm and +7dBm and it has an accurate frequency
display. It also includes a scanning function for filter alignment.
I
’ve always wanted a good AM/FM
HF/VHF signal generator. I have
tried to meet that need with a variety of designs over the years, some
analog, others using DDS chips.
More recently, I have tried low-cost
fractional-N oscillator chips, including the Si5351A. These were only suitable in specific circumstances, and did
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Silicon Chip
not make for a good general-purpose
test instrument.
Obviously, it’s possible to purchase
an RF signal generator, new or used,
but I couldn’t afford the price of a good
one. Cheap signal generators lack adequate performance and useful functions. Those with adequate performance are usually too expensive for
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most hobbyists or are unreliable and
difficult and/or expensive to maintain.
I have seen some designs published,
but these are typically simple analog
LC-based designs with coverage up to
around 150MHz, in a series of five or
six switch-selected bands.
Most lack accurate frequency readouts or adequate stability. Spurious
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canning HF/VHF
ator
Part 1
by Andrew Woodfield, ZL2PD
and harmonic outputs can also be a
problem.
(See the list of references at the end
of this article for three such designs
that I considered and rejected).
Table 1 (overleaf) shows what is
available at the moment. I rejected all
of these options for one reason or another – inadequate performance, lack
of features, high price or unreliability.
With few exceptions, the output levels of most of these generators are quite
limited. Those with a variable output
level typically use a simple potentiometer, with little regard to varying
output impedance or accuracy.
Output levels are also often too low
for use in many typical applications.
Modulation, where available, is often
limited. And, finally, some otherwise
useful digital-based designs are now
difficult or impossible to build due to
obsolete parts or unavailable software
or PCB layouts.
Basic analog and digital PLL-based
RF signal generators are available
between about $200 and $300. The
analog generators offer basic CW, AM
or FM modulation. Output level and
modulation depth on the low-cost
analog generators are typically controlled via internally mounted trimpots adjusted through small holes in
the panel.
The low-cost digital signal generators only offer FM and appear aimed
at the two-way radio industry.
These instruments are all perfectly
functional, but for hobbyists, these
features are too limited. To use them
effectively, you would also need extra
equipment such as a frequency counter, attenuators, amplifiers and a level
meter. It’s far easier to have these features built into the generator.
As Table 1 shows, moving up in
the market significantly increases the
price. Used equipment is available at
lower cost, but many otherwise excellent instruments have recognised
spare parts or reliability issues as the
equipment ages.
So I needed to come up with my own
design that would tick all the boxes,
and that is just what I have done. See
the table below which lists its features
and performance figures.
Features and specifications
Coverage
Tuning Steps
Accuracy & stability
Output level
Attenuation steps
Output socket
Spurious and harmonics
AM
FM
Scanning
Display
Power control
Controls
Power supply
Dimensions
Weight
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Specification
100kHz-50MHz, 70MHz-120MHz
10Hz to 1MHz in decade increments
Within 150Hz at 30MHz (typical), 0-40°C, 0-80% humidity
-93dBm to +7dBm (approximate)
0-80dB in 20dB steps (switched) + 0-20dB (variable)
SMA
Typically better than -30dBc
30% modulation <at> 1kHz
NB (12.5kHz spacing), 1.75kHz deviation <at> 1kHz (60%)
WB (25kHz spacing), 3kHz deviation <at> 1kHz (60%)
BC (12.5kHz spacing), 50kHz deviation <at> 1kHz (60%)
Programmable start and stop frequencies
10, 20, 50, 100, 200 or 500 steps/sweep
16x2 alphanumeric LCD
Soft on/off switch
Two knobs and eight switches
9-12VDC at 250mA
160 x 110 x 25mm (excluding knobs)
160 x 110 x 45mm (including knobs)
~250g
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Comments
Usable up to 150MHz
User-selected
Can be enhanced with software calibration
50termination
Within specified coverage frequency range
Suitable for standard broadcast FM receivers
1kHz resolution
Auto step size calculation
June 2019 27
Design approach
As shown in Fig.1, a modern signal
generator consists of five functional
blocks: the RF oscillator, the modulator, RF buffer amplifier, a variable
attenuator to control the output level, and some control electronics. The
logical implementation of the control
electronics is based on a microcontroller. The final block is the power supply, either battery-powered or mainspowered (or both).
The oscillator is a key element of
any signal generator. An analog-based
wide-range oscillator and modulator
involving sets of inductors and a tuning capacitor is impractical and cannot provide the desired functions and
performance required at a modest cost.
Table 1: I looked at a range of currently available commercial equipment, both
The cheapest digital options include
new and used. However, for anything that had better-than-mediocre performance,
that third column definitely caused me some heartache! I estimate the instrument the powerful Silicon Labs Si5351A
described here could be built for not much more than $75.00, plus case.
device or widely available direct digital synthesis (DDS) modules based
Design goals
Lower RF output levels are also use- on chips such as the Analog DevicThis design represents the outcome ful, eg, for receiver sensitivity tests. es AD985x (see our article on the
of an extended period of development The minimal useful level is mostly AD9850 in the September 2017 issue;
and testing over the last few years.
determined by the limitations of low- siliconchip.com.au/Article/10805).
This signal generator provides ba- cost shielding and simple hobbyist
Other digital options include PLL
sic CW (unmodulated) signals, plus construction methods used.
chips such as the Maxim MAX2870.
AM and FM modulation functions,
If an enclosure was carefully milled While it is possible to generate sineprimarily across the high frequency from a 25mm thick metal billet with waves from both the Si5351A and the
range from 100kHz to 30MHz, with shielding slots for flexible conduc- MAX2870, the additional circuitry
a continuously variable output level tive inserts, the lower limit could be required to obtain low harmonic consuitable for most requirements.
extended significantly, but relatively tent output signals coupled with the
This frequency range includes most few hobbyists could achieve this. So challenges of adding modulation make
common IFs (intermediate frequen- I’ve used simple shielding and a ba- them less attractive.
cies) such as 455kHz, 465kHz, 470kHz,
AD9850 DDS modules (as shown in
sic DIY folded aluminium sheet met10.7MHz and 21.4MHz.
al box. This is reflected in the modest the photos overleaf) are available from
Coverage extends to 50MHz, with lower output specification limit of
sources like ebay and AliExpress at
another range covering 70-120MHz. around -90dBm.
reasonable prices.
Coverage actually extends up to
The instrument’s display requireAchieving that performance, how150MHz with some limitations, to
ever, still requires moderately careful ments are modest, so I decided to use a
permit limited use in the popular 2m enclosure construction.
common 16x2 character alphanumeric
amateur radio band as well as parts
By using commonly available parts LCD. These are easy to read and drive
of the widely used international 138- and low-cost modules, I have been able from a micro.
174MHz land mobile band.
A rough outline of the design began
to keep the overall cost low. I estimate
Key design objectives included low the cost to build this signal generator to take shape and, adding up procescost, ease of obtaining parts and ease currently at around $75.
sor pins required, the very common
of construction.
Special parts such as chip-based attenuators, for example, were avoided
in favour of the low-cost combination
of slide switches and standard resistors.
The generator’s RF output is designed for applications requiring relatively high RF levels.
These include testing double-balanced diode mixers in high-performance receivers and for testing multi-stage passive filters, where stopband attenuation measurements reFig.1: the basic arrangement of a modulated signal generator with adjustable
quire relatively high signal generaoutput level. Our design follows this configuration.
tor outputs.
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Australia’s electronics magazine
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Fig.2: a typical
example of
how you can
apply amplitude
modulation to
the output of
an AD9850based signal
generator module
using discrete
components. In the
end it was decided
to abandon this
idea in favour
of a PWM-based
microcontroller
approach.
ATmega328P 8-bit microcontroller
appeared suitable. While an Arduino
was briefly considered, I would need to
use practically every pin on the device,
and I wanted to keep the instrument
compact, so I decided to use a standalone ATmega328 processor.
The RF buffer amplifier requires
only modest gain. It must handle the
somewhat unusual 200output impedance of the AD9850 module and
the following 50attenuator stages
and 50output. Another consideration is that the buffer should not be
overloaded by the sometimes high
output swing of the AD9850. Numerous designs published on the internet
suffer from this problem.
The buffer should also maintain its
gain across the design frequency range.
And the buffer should be able to work
into a reasonable range of loads and
survive typical bench treatment.
I’ve used MMIC amplifiers such as
the ERA-series devices from MiniCircuits to buffer AD9850, AD9851
and AD9854 DDS chips in the past.
These drive 50loads with good performance.
However, in testing this signal generator with a wide variety of filters,
amplifiers, receivers, transmitters and
other loads, several MMICs suffered
early deaths. These were probably due
to the very low impedances presented
by some of the test filters.
The search for a more suitable buffer
stage was ultimately concluded with
the inclusion of a traditional singlestage buffer amplifier using a robust
2N4427 VHF transistor. It is widely
available at low cost, as is its nearequivalent, the 2N3866. It proved more
than adequately robust over many
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months of use. The TO-39 case of the
transistor becomes warm during use,
but a heatsink is not required.
The design of the attenuator stage
also posed some challenges. Recently, PE4302 30dB step attenuator chips
have become popular. While only relatively new devices, these have recently
been listed by the manufacturer as obsolete. The replacement devices, while
having improved performance, also
come at a substantially increased price.
Relay-controlled fixed attenuators
can be used, but with an eye on cost
and simplicity, I decided to use inexpensive slide switches instead. Experience has shown these to perform adequately for this type of application.
However, these limit the attenuator
steps to specific attenuation values.
Ideally, the generator should have a
fully variable output level.
So I decided to build and test a Serebriakova attenuator as an alternative
to a more costly PIN diode-based design. This configuration is shown in
the lower right-hand corner of Fig.4,
the circuit diagram.
It’s a simple passive resistor net-
What is Frequency
Modulation (FM)?
With frequency modulation, the audible tone of (say) 1kHz results from the
carrier frequency of the signal generator
being instantaneously shifted (or “deviated”) from its nominal frequency in
proportion to the amplitude of the modulating tone.
As the amplitude of the tone increases,
at that 1kHz rate, the carrier frequency of
the generator proportionally increases.
Similarly, as the 1kHz tone’s amplitude
decreases, the carrier frequency is proportionally decreased. It is proportional
because the extent of the carrier frequency shift, or deviation, depends on the signal bandwidth required.
For broadcast radio FM, the peak deviation is ±75kHz. The resulting signal
fills the standard FM broadcast channel
bandwidth of 200kHz. Traditional VHF
FM two-way radio transceivers used for
amateur radio or commercial/government mobile radio use a much smaller
±5kHz deviation, and these signals occupy 25kHz channels.
More modern so-called “narrow-band”
amateur FM transceivers typically use
±2.5kHz deviation, and these use more
densely-packed channels spaced apart
by 12.5kHz.
work which acts as a variable attenuator, well suited for basic designs like
this. Apparently of Russian origin, the
attenuator network uses a 500linear
potentiometer to give a 20dB variable
attenuation range. It works well into
mid-VHF frequencies.
The input impedance is maintained reasonably close to the desired
50across the adjustment range of
the potentiometer, so the attenuation
is predictable. The output match to
50as the potentiometer is adjusted
Fig.3: the output of a DDS signal generator module contains the wanted
frequency plus a number of alias frequencies. These are normally filtered out
but it is possible to instead filter out the fundamental frequencies and keep one
of the higher alias frequencies to extend the signal generator’s range.
Australia’s electronics magazine
June 2019 29
This is the low-cost AD9850-based DDS signal generator used in this design.
Besides the chip it has a reference osciallator (the metal can at left) plus a
number of discrete components including a low-pass filter for the output.
is not perfect, but it’s an acceptable
compromise for this design.
Amplitude modulation with
the AD9850
A key objective of the signal generator was to deliver both amplitude
(AM) and frequency modulation (FM)
as well as providing an unmodulated
RF signal.
Amplitude modulation with the
AD9850 is well documented. Analog
Devices, the chip’s manufacturer, helpfully published an application note
(AN-423) which describes adding a
small signal NMOS FET and a few additional parts to do this. A quick test
confirmed that it works as described.
Most signal generators use a 1kHz
modulation tone, which can be produced in several ways. One approach
is to use the ATmega328 to generate
a 1kHz square wave using one of its
internal timers and then filter this to
give a 1kHz sinewave. But extensive
filtering is required to obtain a suitable tone. That involves quite a few
extra parts.
A second, similar approach is to
use the ATmega328’s counter/timer
in its pulse-width modulated (PWM)
mode. The resulting waveform is
closer to a sinewave but still requires
some filtering to remove the 31kHz
PWM frequency. Usefully, that filter
is far less complex given the much
higher clock frequency compared to
the 1kHz tone.
A third option is to build a discrete
1kHz sinewave oscillator and just use
the ATmega328 to turn it on and off as
required. At first glance, the discrete
oscillator approach is attractively simple and uses relatively few components, so I tested this out, using the
circuit shown in Fig.2.
It works quite well. The 3.3nF capacitor value can be adjusted to give
the required modulation level at the
AD9850’s RF output. This works by
replacing the fixed resistor (“RSET”)
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Silicon Chip
on pin 12 of the AD9850, typically
3.9k, with the variable resistance of
Q2’s channel. This resistance sets the
AD9850 digital-to-analog converter
(DAC) current and, subsequently, the
AD9850 RF output level.
By varying the gate voltage of the
2N7000 at 1kHz using the voltage from
the collector of audio oscillator Q1,
the AD9850 RF output is amplitude
modulated.
However, this analog tone is not
precisely 1kHz. Its frequency is determined by the passive components
around Q1. To give a more accurate
(and potentially adjustable) modulation frequency, the PWM-based approach was used in the final circuit.
See the section of Fig.4 labelled “OUTPUT LEVEL CONTROL”.
Pin 11 (output PD5) of IC1 produces
the 1kHz sinewave as a 31kHz PWM
square wave, or potentially at other
frequencies by changing the software.
This is filtered and used to control a
current sink made using standard NPN
transistors. An extra 100nF bypass capacitor was added to pin 12 to the final PCB to address AD9850 module
stability.
The 31kHz pulse width modulated
1kHz signal is produced by the ATmega328 from its 8MHz internal RC
oscillator. The variable DC voltage of
0-5V arriving on the base of Q1 is converted to a variable collector current
in Q1 of 0-700µA, the maximum current value being set by its 1kemitter
resistor. This figure was selected to exceed the 625µA maximum current sink
range required by the AD9850.
This approach is not perfect. Using
the RSET pin and the standard unbalanced RF output from the AD9850
module, the typical approach used in
these low-cost modules, the output
modulation produced is asymmetric.
In practice, however, this does not
matter terribly.
This simple circuit delivers cleansounding amplitude modulation with
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the AD9850 and uses fewer components than the other options. It also
allows other modulation tones to be
added in future if required. Finally,
this approach also adds another important feature – reasonably accurate
linear control of the AD9850 RF output level.
Note though that this approach requires the removal of that 3.9kresistor
from the module as supplied, and the
addition of a wire to control pin 12
from Q1 to one of its pads. This change
will be described in more detail later.
Frequency modulation (FM)
Again, there are several options to
produce FM with the AD9850. One approach would be to externally modulate the AD9850’s separate 125MHz
reference crystal oscillator. Frequency
and phase modulation could be both
implemented this way. Unfortunately,
the 125MHz reference oscillator in the
low-cost modules is inside a sealed
metal can.
There is no external voltage tuning input which might otherwise be
pressed into use to produce FM. It’s
possible to replace the reference oscillator module with a discrete oscillator
to allow for external modulation, but
that takes some effort.
It is also possible to use the AD9850internal phase modulation register but
resolution is too limited (4 bits).
Another Analog Devices application
note (AN-543) suggests a solution. It
describes a powerful Analog Devices
DSP chip which samples incoming stereo audio at 48ksamples/sec and then
sends a stream of 40-bit frequency-setting words serially at very high speed
to the AD9850.
Each of these 40-bit words programs
the AD9850 to a new instantaneous
frequency, which is necessary to emulate a stereo FM signal (including the
19kHz and 38kHz pilot tones).
With some care and a few lines of
assembly code for speed where necessary, the ATmega328 can modulate
the AD9850’s output frequency in this
manner. Sadly, the resulting modulation sounds pretty average. The problem is the time required by the ATmega328 to send the serial string of
40 bits to the AD9850 each time its
frequency has to be updated for frequency modulation via the typical
3-wire interface.
The poor result is not surprising.
With the conventional serial load
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method and our 8MHz, 8-bit chip, it
is (just!) possible to load four modulation samples per 1kHz cycle into the
AD9850. A four-point sinewave is actually a triangle wave, which is full
of harmonics!
Closer study showed that there is
another way to communicate with
the AD9850 chip. Almost every
AD9850/51 based design uses the
three-wire serial bus to send 40-bit
control words to the AD9850 each time
the frequency needs to be updated.
However, the AD9850 can also be
controlled using a parallel interface.
This requires sending five 8-bit words
in quick succession to the chip, along
with some control signals via two or
three additional pins. The only published example I could find is based
on a PIC processor.
There is a considerable advantage
in this method. Rather than taking
about 250µs for the ATmega328 to load
each 40-bit word serially, the parallel
approach can reduce this to as little
as 2.5µs.
With the parallel loading method, it
is possible to send 20 samples per 1kHz
cycle without any trouble at all, even
with the (relatively) slow 8MHz clock
in the ATmega328. This is much closer
to a proper sinewave. The difference is
clearly audible in an FM receiver. The
parallel method gives a demodulated
signal that sounds very clear and clean,
just like a sinewave should.
So for FM, the 20-point sampled
waveform is created by calculating
the required AD9850 output frequency
every 50µs and sending that data over
the fast parallel interface.
The FM deviation is controlled by
changing the magnitude of the frequency changes which occur 20,000
times per second (20 points x 1kHz).
Selecting narrow band FM (the LCD
shows “FM-NB”) on this generator for
12.5kHz spacing FM two-way radios
produces ±1.5kHz FM; selecting wideband FM, for older 25kHz channel
spaced two-way radios, gives ±3kHz
FM (“FM-WB”), while selecting broadcast FM produces ±50kHz FM signals
(“FM-BC”).
Frequency scanning
A further feature of this signal generator was added for testing and aligning filters. For example, while designing this Signal Generator, I was also
building a 9-band HF transceiver. Its
receiver front end features nine sets of
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coupled tuned circuits, each requiring
careful alignment, with three or four
adjustments per set.
In the scanning mode, the generator
briefly produces a signal on a series
of discrete frequency steps across a
defined range. For the transceiver example, the signal generator could be
programmed to produce signals across
each of the nine bands used for the
bandpass filters being tested.
By monitoring the amplitude of the
resulting output from each filter on an
oscilloscope, it is possible to quickly
align each filter while seeing the impact of every change. This forms, in effect, a ‘poor man’s spectrum analyser’.
This saves considerable time and effort over manual alignment methods.
The start and stop frequencies can
be set anywhere across the range of
the signal generator. Since filters are
generally fairly broad, a 1kHz step size
for setting the start and stop frequency
is acceptable.
I decided to add a SCAN pushbutton to the design, to enable this mode.
As I had run out of pins on the ATmega328, I used two diodes (D1 & D2) so
that pressing this button is effectively
equivalent to pressing the two existing
buttons (MODE and STEP) simultaneously. The micro can detect this as a
press of the SCAN button – see Fig.4.
Expanded frequency coverage
Typical AD9850 modules are fitted
with a 125MHz reference oscillator.
DDS oscillators deliver clean sine outputs up to about 30% of the reference
frequency; in this case, say 40MHz. Increasing but acceptable levels of aliasing products are present in the output
spectrum up to 45% of the reference
frequency, say 50MHz.
Beyond this, as the output frequency
approaches the Fourier limit of about
60MHz, spurious products render the
output unusable.
The cheap modules are usually supplied with an onboard elliptical lowpass filter with a cutoff frequency of
70MHz to maximise the output frequency range. In fact, these modules
have three outputs. The first is the filtered output as described. It appears on
my module on the pin labelled “SINB”.
An adjacent pin, “SINA”, might appear to be similar. However, this signal
comes directly from the AD9850 DAC.
It is a 180° phase-shifted (inverted) version of the signal at SINB but without
any additional low-pass filtering.
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The third available output comes
from an internal comparator in the
AD9850. It produces a square wave
version of the output. This is output
level dependent, the duty cycle being
set by adjusting a miniature trimpot on
the module. If it is adjusted for a good
50% duty cycle output at a lower frequency setting, it tends to be less accurate at higher frequencies.
There is little difficulty in obtaining reasonably clean filtered signal
generator outputs up to 50MHz from
the filtered (SINB) pin. Some testing
showed that output was acceptable
down to 100kHz. That’s useful for covering receiver intermediate frequencies (IF) and IF filters between 455kHz
and 470kHz, for example.
Looking more closely at the module,
the second SINA output looked potentially useful too. Because this output
is not filtered, the full set of DDS alias
frequencies are available here.
In one example, illustrated in Fig.3,
the “wanted” output (labelled Fout) is
at 30MHz. As the user increases this
frequency, tuning towards 35MHz for
example, this output frequency increases, shown by the blue arrow.
At the same time, the AD9850 (like
June 2019 31
Fig.4: along with the 16x2 LCD module, the ATmega328P microcontroller (IC1) drives the AD9850 signal generator
module using an 8-bit parallel bus plus three control lines. This allows it to modulate the output frequency at 20kHz
which results in clean 1kHz frequency modulation. Amplitude modulation is applied using PWM from pin 11 of
IC1, which is filtered and then controls a current sink comprising transistors Q1 and Q2. The resulting current flow
controls the signal generator output level. The output signal is buffered by transistor Q3 and then passes four switched
20dB attenuators and then a 0-20dB variable attenuator (VR2) which gives a 100dB overall output range. Q4 and Q5
form a “soft power” switch for the circuit, which is controlled by pushbutton switch S3.
all DDS chips) also produces “alias”
frequencies. These are shown in orange. The nearest is at 95MHz, ie, the
clock frequency of the DDS (125MHz)
minus 30MHz. It decreases in frequency as the user tunes from 30 to 35MHz,
ending up at 90MHz (ie, 125-35MHz).
There are many other alias frequencies which are produced simultaneously, the next nearest being
at 155MHz (the clock frequency of
125MHz plus 30MHz), with others at
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220MHz, 280MHz and so on, theoretically continuing forever. The direction
these alias outputs tune can be seen by
the direction of the arrows, some rising while others reduce in frequency
as the primary frequency is increased.
The amplitude of all of these signals
follows a strict mathematical relationship, called the “sine x upon x” curve.
That’s shown in green on the figure.
There’s about a 10dB level difference
between the 30MHz output and the
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95MHz alias signal, for example.
That’s the reason for the substantial
onboard filter on the AD9850 module.
It’s a low-pass filter designed to cut
off at 70MHz, so the majority of these
aliased products do not appear at the
SINB output. However, since there is
no similar low pass filter on the SINA
output, these alias signals are all usefully present, in full, at this pin.
As the user continues to tune the
AD9850’s output upwards in frequensiliconchip.com.au
cy, the ‘wanted’ and first ‘alias’ output
ultimately coincide and pass each other at Fout=62.5MHz.
A few tests using this SINA pin
suggested that the usually unwanted
alias frequencies above 65MHz could
be obtained from the module using an
external high-pass filter (HPF). That
would allow the signal generator to
provide useful outputs from, say,
about 70MHz up to about 120MHz.
With additional filtering, still higher
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aliasing products could be filtered out
and amplified.
This permits the generator to produce signals across the 2m amateur
band or across part of the 138-174MHz
land mobile bands. As it turns out, useful outputs across these bands could be
obtained just from using a single HPF,
and the maximum tuning frequency
for the signal generator was therefore
set at 150MHz. Those wanting other
bands or fewer aliasing outputs can
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modify the HPF to suit individual requirements.
Detailed circuit description
The final circuit arrangement is
shown in Fig.4.
While it may appear complex at first
glance, this design uses remarkably few
components given the range of modulation modes and coverage it provides.
Some of the complexity is hidden in
the software for IC1.
June 2019 33
NAVIGATING THE MENUS
Starting frequency and mode
Press “MODE” to select next mode (AM)
Next press selects narrowband FM
Twice more selects broadband FM
(wideband FM not shown)
Once more selects SCAN mode
MODE button
Pressing SCAN selects ‘start’ frequency
(Adjust with “tune/step”)
Pressing SCAN again selects End;
then Steps
To enable the frequency modulation
described above, the AD9850’s 8-bit
data port (pins D0-D7) is connected
to micro IC1’s PORTB digital outputs
(PB0-PB7). The three 10kseries resistors have been added so that IC1 can
be reprogrammed in-circuit (via ICSP
header CON3) while IC1 is still connected to MOD1.
MOD1 is also connected to 5V power (VCC) and GND, plus the slave select (SS) and reset (RST) pins, which
go to digital I/Os PC4 and PD4 on IC1
respectively.
Its two output signals are fed to the
HPF and switch S4, while the square
wave output goes to CON4, although
the signal which appears there is of
limited use, as its duty cycle varies
with frequency.
With switch S4 in the position
shown, the lower frequency (100kHz50MHz) signals pass through S4a, the
100nF coupling capacitor and S4b directly on to the buffer amplifier (the
base of transistor Q3).
For higher frequency signals, S4
is moved to the alternative position
where the buffer amplifier is fed from
the output of the HPF, which receives
its input from the unfiltered DDS output pin.
The HPF is a standard seven-pole
Chebyshev filter. Elliptical filters provide a faster pass-to-stop band cut-off,
but the resulting spurious and harmonic rejection is less effective compared
with the Chebyshev type.
The filter was optimised to suit
standard leaded components and
home-made inductors.
For best performance, the coupling
between the coils must be minimised.
The PCB layout provides for small tin
plate shields to be fitted between filter
stages, a simple and effective solution.
The alternative HPF shown could
potentially shift the 70-150MHz upper
output range to 125-187.5MHz with
appropriate software changes.
RF buffer amplifier
Pressing SCAN again starts Scanning
SCAN button
MODE button
34
34 S
Silicon Chip
As noted earlier, the buffer amplifier is a robust discrete design, based
on NPN transistor Q3. This is a wellknown single transistor broadband arrangement providing about 15dB gain
along with good dynamic range. Gain
is necessary to provide the required
maximum output level for the signal generator and to compensate for
the insertion loss of the Serebriakova
attenuator.
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Alternative discrete buffers seen in
other AD9850/51 based designs lack
sufficient gain across the output range
and/or frequently overload with the
typically higher module output levels
present below 10MHz.
By contrast, this buffer amplifier’s
gain is relatively flat and only reduces
above 50MHz. This is acceptable given
the application and circuit simplicity.
If you find the 2N4427 transistor
difficult to source, you may be able to
find a 2N3866 instead, although the
gain may reduce by several decibels.
The output of the amplifier is taken
from the centre tap of autotransformer
T1 and coupled to the output attenuator by a 100nF capacitor.
The attenuator consists of four identical 0/20dB switched attenuators, followed by the aforementioned 0-20dB
Serebriakova attenuator, giving an
overall range of 0-100dB. This allows
you to adjust the output from about
-93dBm to +7dBm.
As mentioned earlier, this range is
limited by shielding effectiveness and
RF signal leakage across the attenuator sections.
Better shielding between sections
is likely to allow another 20dB fixed
attenuator to be added, significantly
improving its utility for small signal
work. Further improvements would
likely require considerable additional
design efforts around the power supply and control sections.
User interface
IC1 updates the 16x2 LCD using a
typical 4-bit interface. The lower four
bits of PORTC on IC1 (pins 23-26) drive
the four upper LCD data pins, while
pins 12 and 13 (digital outputs PD6
& PD7) drive the RS and EN control
lines of the LCD.
The backlight brightness is fixed using a 1kresistor, with the backlight
powered whenever the device is on,
and trimpot VR1 provides contrast
adjustment.
The Grey code pulses from the rotary encoder are sensed using IC1’s
PD2 and PD3 digital inputs (pins 4
& 5), while presses of the encoder’s
integral pushbutton and the SCAN
and MODE pushbuttons (S1 & S2) are
sensed using digital inputs PD0 and
PD1 (pins 2 and 3).
These have internal pull-ups enabled so that they are held high when
no buttons are being pressed.
As mentioned earlier, diodes D1 and
siliconchip.com.au
To whet you
appetites for part
2, the construction
details (scheduled
for our July
issue) here is the
author’s completed
prototype PCB. As
you can see, despite
its complexity and
performance, there
really isn’t all that
much to building it!
D2 have been added to allow presses
of three buttons to be sensed using the
two available pins.
Jumper JP1 and ICSP header CON3
have been provided to allow IC1 to be
re-programmed in situ. Removing JP1
prevents the programmer from trying
to power the RF circuitry. CON3 has
the standard Atmel 6-pin programmer pinout.
Power switching
The external power supply, nominally 12V DC, directly powers the
output buffer. The buffer can operate
down to 9V although harmonic distortion at full output increases by about
6dB at 9V compared to 12V.
The 12V supply is also regulated
down to 5V by REG1 for the AD9850
module and the ATmega328 processor. Since the AD9850 module is current-hungry, REG1 requires a heatsink.
Dissipation losses would be reduced
by using a switchmode regulator but
this can introduce switching noise inside the signal generator, and could
potentially modulate the output buffer
output signal.
As it turns out, the metal signal generator case forms an effective heatsink
for REG1, and this avoids the need for
additional hardware.
The signal generator will continue
to operate with a supply voltage down
to 6V; however, its performance degrades significantly below 9V. By 6V,
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the maximum output falls by 10dB
and harmonics are only suppressed
by 10dB due to the reduced dynamic
range in the buffer stage.
So, operation at 6V is possible but
not recommended.
A ‘soft switch’ circuit has been added to allow the use of a momentary
pushbutton (S3) as a power switch.
The circuitry to provide this function is shown at the upper right of
Fig.4. It was initially described by Zetex in their February 1996 Design Note
27, for use as a relay driver.
However, several problems were encountered with that design, including
References
1. Gary McClellan, Programma-II synthesised signal generator, RadioElectronics magazine, Aug & Sept
1981 (300kHz to 30MHz CW/AM signal generator, 10kHz tuning steps, 10300mV output)
2. G. Baars, PE1GIC, DDS RF Signal
Generator, Elektor, October 2003
(50Hz to 70MHz, CW/AM/FM, 1Hz to
1MHz tuning steps, 0 to -127dBm out)
3. Ian Pogson, Solid state modulated RF
test oscillator, Electronics Australia,
May 1979 (455kHz to 30MHz in four
ranges, approximately 100mV output)
4. http://lea.hamradio.si/~s53mv/dds/
theory.html
5. www.picmicrolab.com/ad9850pic16f-interface-parallel-data-load/
Australia’s electronics magazine
some curious component choices and
overheating. A minor redesign and the
use of a higher-gain switching transistor solved them all.
When the supply is initially connected, the voltage appears on the
emitter of Q4 and the 1µF capacitor
charges via the three series resistors
(2.7k, 1k and 270k). However,
Q4 cannot turn on until momentary
switch S3 is pressed and no current
is drawn from the supply.
When S3 is pressed, current is supplied to the base of Q5, which switches
it on, and it in turn sinks current from
the base of PNP transistor Q4, switching it on also and bringing up its collector voltage.
Current can then flow from Q4’s
collector to Q5’s base via the two 1k
series resistors, so Q5 remains on and
so does Q4.
However, the 1µF capacitor discharges because Q5’s collector is
now being pulled low, to 0V. So if S3
is pressed again, Q5’s base goes low,
switching it off, and in turn switching
off Q4, so the circuit is back in the initial off-state.
Part Two, next month
Next month’s article will have the
parts list, details of PCB assembly,
case construction, programming IC1
and how to use the RF Signal Generator. We’ll also have performance data,
SC
including spectrum plots.
June 2019 35
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