All posts by Martin Blustine

I studied physics and went on to work in infrared optics, millimeter wave and microwave engineering until retirement. My interests lie in teaching, music, radio astronomy, infrared systems and microwave and antenna engineering. I enjoy writing technical papers about ham radio topics. When I am not operating CW, I enjoy homebrewing ham gear and restoring vintage HP and Agilent test and measurement equipment.

Spectral Purity of a QRP Transmitter Driver Amplifier

Introduction

Some months ago, we reported on a commercially available, off-the-shelf 3W MMIC amplifier [1] to be used as part of a transmitter driver with receive bypass [2]. It was our intent to use as many COTS components as possible to simplify and shorten the construction timeline for a 10-band QRP SSB transceiver. An inexpensive amplifier that is widely available through AliExpress [3] is advertised to work from 2 to 700 MHz, which is more than adequate for our requirements (Figure 1. The gain of this amplifier was 45 dB.

Figure 1. Wideband 3W Shortwave Amplifier. This wideband shortwave amplifier is advertised as being capable of 3W output power. Our plan is to drive it to 1W so that our 10 dB gain power amplifier can be driven to 10W. The 3W MMIC amplifier works from 2 to 700 MHz, which is more than adequate for high-frequency use. The measured gain of the amplifier is 45 dB. Power dissipation is greatly improved by the application of diamond heatsink compound between the circuit board and the heatsink. The amplifier is operated at +9 VDC to reduce its thermal dissipation. Please click on the Figure to open it in a new window.

Since our last report, some changes have been made to the original circuit to reduce its gain, increase its stability, improve its spectral purity, and enhance its receive isolation. The 3W MMIC amplifier is of single-ended construction. Consequently, there is no cancellation of even (or odd) harmonics of the signal being amplified, and it turns out that when operated at +9 VDC, or even +13.8 VDC, the MMIC amplifier is quite nonlinear.

This article discusses all of the circuit improvements. In particular, the spectral purity of the transmitter driver amplifier is demonstrated. Use of the single-ended amplifier requires the addition of another low-pass filter bank [4] between the driver amplifier circuit and the transmitter, in addition to the one that is provided at the transmitter output.

Low Pass Filter Bank

Thanks to Hans Summers, G0UPL, at QRP Labs [5] for providing bare boards so that my original filter bank, consisting of 10 low-pass filters, Figure 2, that employed the Ed Wetherhold (SK), W3NQN, design [6] could be built and tested.

As we will soon demonstrate, an additional low-pass filter bank results in greatly improved spectral purity. Since an additional low-pass filter bank had not yet been built, we have employed the transmitter low-pass filter bank, as required, for measurements in this paper.

Figure 2. Ten-Band Low Pass Filter Bank on Its Interconnect Backplane. The 40m low-pass filter that was used to process the 7.1 MHz signal is located four filters from the left. All of the filters employ the Ed Wetherhold (SK), W3NQN, design. The bare boards for these filters were obtained from Hans Summers, G0UPL, at QRP Labs. Readily available Arduino relay boards were used throughout. Since these are power relays, the relay contacts are DC-wetted through bias-T’s, not shown, to reduce the contact resistance. The QRP Labs filters employ a single DPDT relay per filter band, whereas my filters employ two separate SPDT relays per band. Please click on the Figure to open it in a new window.

Revised Transmitter Driver With Receive Bypass Schematic
A revised schematic diagram is shown in Figure 3. Changes to the original design [7] include the removal of relay optical isolation for push-to-talk with the deletion of its attendant FET driver, and the addition of relay grounding for the receive bypass path during transmit. An additional relay pair was added to perform the grounding function. A 3 dB attenuator was added to the driver amplifier input to improve the amplifier stability and to reduce its gain. A photo of the completed design with the 3 dB coaxial attenuator installed is shown in Figure 4. If there is sufficient isolation, the 3 dB attenuator will be added to the back of the circuit card. The revised design uses a separate power management circuit board to supply +13.8 VDC to the +9 VDC onboard voltage regulator during transmit. This greatly simplifies the circuit board.

Figure 3. Revised Driver Schematic Diagram. The schematic has been simplified when compared to the previous iteration. The logic input has been removed so that the module may be keyed by the power management module during transmit. The receive bypass path is grounded at both ends during transmit. Power is supplied to the driver amplifier by an LM317 adjustable voltage regulator that receives power from the power management module during transmit. Please click on the Figure to open it in a new window.

Figure 4. The Completed Driver Amplifier Board As Revised. The black driver amplifier heatsink is visible. The lower relay pair provides the transmit/receive function. The upper relay pair grounds each end of the semi-rigid coax receive path during transmit. The LM317 adjustable regulator regulates +13.8 VDC from the power management module down to +9 VDC for use by the driver amplifier. This reduces the amplifier power dissipation. Please click on the Figure to open it in a new window.

The measured spectrum of the amplified 7.1 MHz signal without low-pass filtering is shown in Figure 5. The amplifier has been driven to 1W. Since the amplifier is single-ended, the even harmonics have not been suppressed, and the 2nd harmonic is barely 10 dB below the carrier. It is evident that this MMIC amplifier is nonlinear.

Figure 5. Spectral Purity of a 7.1 MHz Signal Prior to Low Pass Filtering. Even and odd harmonics are visible because the driver is single-ended, not push-pull. A push-pull amplifier would provide some attenuation of the even harmonics but not the odd harmonics. The spectrum analyzer display shows the 7.1 MHz carrier at 0 dBm. Since the spectrum analyzer input is padded by 30 dB, 0 dBm corresponds to 1W. The second harmonic is barely -10 dBc for this drive level. Please click on the Figure to open it in a new window.

The measured spectrum of the amplified 7.1 MHz signal with low-pass filtering is shown in Figure 6. The amplifier drive level was left unchanged from the previous measurement. With the low-pass filter applied to the signal, both the even and odd harmonics have been suppressed by nearly 60 dB.

Figure 6. Spectral Purity of a 7.1 MHz Signal After Low Pass Filtering. The even and odd harmonic content of the 7.1 MHz signal has been suppressed by nearly 60 dB. The implication is that the W3NQN 40m low-pass filter is doing a great job of attenuating the 2nd harmonic and higher-order products. About 1 dB of signal attenuation is observed after passing it through the low-pass filter, as one might expect. As in the previous figure, 0 dBm corresponds to 1W due to the presence of a 30 dB pad at the spectrum analyzer input. Please click on the Figure to open it in a new window.

Summary

We have described revisions to the original circuit design that result in a much simpler driver amplifier that retains a receive bypass function. The revised circuit is keyed from the power management module on transmit so that it does not have to be keyed directly from push-to-talk.

The spectral purity of the amplified signal before and after low-pass filtering has been demonstrated. Higher order harmonics are attenuated by nearly 60 dB by Ed Wetherhold, W3NQN, low-pass filters.

The low-pass filter bank that was used for spectral evaluation is at the transmitter output. Consequently, another low-pass filter kit has been ordered from QRP Labs that will cover 5 of the 10 bands. Another kit will be ordered at a later date to cover the remaining 5 bands. Since these low-pass filters come without an integral transistor interface for microprocessor I/O, one will have to be built.

A short YouTube video [8] of a test may be viewed at https://youtu.be/nTQk9CR1W9w

References

[1] 2 MHz-700 MHZ 3W HF VHF UHF FM Transmitter RF Power Amplifier For Radio https://www.aliexpress.us/item/3256807249993037.html?spm=a2g0o.order_list.order_list_main.25.1adb1802la12vX&gatewayAdapt=glo2usa

[2] Blustine, Martin, RF Driver Amplifier With Receive Bypass, N1FD, Nov. 1, 2025. https://www.n1fd.org/2025/11/01/rf-driver-amplifier/

[3] AliExpress, op. cit.

[4] QRP Labs, Ultimate Relay-Switched LPF Kit, https://qrp-labs.com/ultimatelpf.html

[5] QRP Labs, Low Pass Filter Kit, https://qrp-labs.com/lpfkit.html

[6] Wetherhold, Ed, W3NQN, Second-Harmonic Optimized Low-Pass Filters, QST, Feb. 1999, pp. 44 – 46.

https://www.arrl.org/files/file/Technology/tis/info/pdf/9902044.pdf

[7] Blustine, Martin, op. cit.

[8] YouTube Test Video, https://youtu.be/nTQk9CR1W9w

Disclaimers

This circuit design is provided for informational and educational purposes only and is supplied “as is” and without warranties of any kind, express, implied, or statutory. No representations or warranties are made regarding the accuracy, adequacy, completeness, legality, reliability, or usefulness of this information, either in isolation or in the aggregate. This circuit design may contain links to or information based on external sources or third-party content. Endorsement and responsibility for the accuracy or reliability of such third-party information or for the content of any linked websites are not taken.

RF Driver Amplifier Circuit With Receive Bypass

This article discusses how a 3W commercial off-the-shelf (COTS) amplifier [1] may be used to drive a COTS 30W power amplifier [2] for use in a QRP transceiver transmitter. When homebrewing, it can be challenging to determine when to design and build something from scratch or when to assemble it from COTS parts. Several low-power amplifiers were considered for use as driver amplifiers, and the one selected is capable of a 1W (+30 dBm) output with only 0.032 mW (-15 dBm) input, resulting in a 45 dB gain at 10.12 MHz. This amplifier works over the entire HF spectrum. The 30W power amplifier was advertised for use as a linear amplifier that follows a low-power transceiver. It is provided with a receive bypass relay circuit so that the received signal will pass through the linear amplifier unimpeded. The 3W amplifier, however, does not have a receive bypass circuit. To use it in this application, a receive bypass path must be provided. That is the subject of this article.

Component Parts

The 3W amplifier selected for this application is shown in Figure 1. It consists of two Monolithic Microwave Integrated Circuits (MMICs) cascaded to produce the specified gain and power output. It was acquired from a seller on AliExpress [3] for less than $15. Upon arrival, the circuit board was removed from its heat sink. That is when it was discovered that no thermally conductive paste of any kind was applied to the interface. The ground tabs on the MMIC amplifiers were designed to dissipate heat. However, the only conduction path is through the via holes in the circuit board in proximity to the ground tabs. This is an ineffective conduction path to the ground plane on the rear side of the circuit board.

RF Driver Amplifier

Figure 1. A Commercial-Off-the-Shelf MMIC Driver Amplifier. This is a commercially available MMIC amplifier with an advertised output power of 3W. When operated with 12 to 15 VDC, the amplifier overheats. There was better luck once a layer of diamond thermal compound had been spread between the circuit board and the heatsink. Once reassembled onto its heat sink, the amplifier ran lukewarm at an operating voltage of +9 VDC with a power output of 1W (+30 dBm) when driven with 0.032 mW (-15 dBm). If the photo is studied closely, the grey thermal compound may be seen finding its way to the top of the PCB through the PCB via holes. Please click on the image to open in a new screen.

Once diamond thermal compound {4] had been applied to the back of the circuit board, the thermal paste began to fill the via holes thereby increasing the area of the conduction paths to the rear ground plane and to the heat sink beneath.

Next, operation was attempted at +13.8 VDC. While not hot enough to boil water, the heatsink became uncomfortably warm with the module dissipating more than 6W. Clearly, something didn’t seem quite right. These modules were specified for operation between +12 VDC and +15 VDC for the stated output power. The reliability of operation at this temperature was questionable.

If the heat sink area and volume is not increased, the simplest remedy is to reduce the operating voltage. Operation at +9 VDC was investigated with very good results. The RF power output of the module at 10.12 MHz is shown in Figure 2. The modulation sidebands are due to the bench switching power supply used. An output power of 1W (+30.11 dBm) was achieved for  0.032 mW (-15 dBm) input power, and the power dissipation dropped to 3W. One watt is more than enough power to drive the power amplifier to 10W (+40 dBm). When cooled by the fan in the transmitter, the MMIC driver amplifier will operate reliably.

Figure 2A

Figure 2B

Figure 2. Output Power of the 3W MMIC Driver Amplifier. At A, the spectrum analyzer photo is of the amplifier output power at 10.12 MHz. The modulation sidebands that originate with the switching power supply are visible. An output power of +0.11 dBm is observed. At B, since a 30 dB attenuator protects the spectrum analyzer input, the actual power achieved is 1W (+30.11 dBm) for -15 dBm input power. The gain at +9 VDC operating voltage is 45 dB. This is 10 dB higher than the specified gain, at least at 10.12 MHz. Please click on each image to open in new screens.

The 2-channel relay selected for this application is shown in Figure 3. These are commonly referred to as Arduino relays. Typically, they are operated from the TTL outputs of an Arduino after inversion. The relays may be operated with positive logic or negative logic by moving a small jumper. The relay inputs are optically isolated which greatly simplifies their use.

Figure 3. A 2-Channel Arduino Relay. These relays are optically coupled and can be controlled with positive and negative logic by moving the tan jumper that is visible in the photo. This module consists of two discrete, individually controllable single pole double throw (SPDT) relays. Please click on the image to open in a new screen.

Voltage regulation is provided by the LM317 adjustable voltage regulator [5]. The ripple output of the device is not of concern because it is being operated from a bench power supply. The voltage adjustment potentiometer has been bypassed; nonetheless, since the ripple voltage tends to increase with increasing adjust resistance.

A 2N7000 MOSFET is selectable at the logic input to the relay pair. If selected, it serves two purposes; a high impedance logic input for CMOS as well as a method for logic signal inversion, if desired, at the relay input.

Circuit Design

The circuit was designed on EasyEDA [6], a free, easy-to-use online design software package. As is usually the case, the Gerber files were transmitted to JLCPCB [7], a printed circuit fabrication house in Hong Kong. Turnaround time is typically 5 to 10 days depending upon the complexity of the circuit.

The circuit schematic diagram is shown in Figure 4. All of the key components of the previous section are shown on the schematic. Note that the receive path is through the normally closed contacts of the relays. Thus, no relay coil current is required during receive.

RF Driver Amplifier

Figure 4. Driver Amplifier Receive Bypass Schematic Diagram. The module has been designed around readily available COTS component parts. All parts are of the through-hole variety since there is little area to be gained through the use of SMT because the amplifier and relay are so large. Please click on the image to open in a new screen.

The jumpers for logic high input and logic low input operation are shown next to J1 and J3. Some of the connections to the relay are made with pin headers and Dupont ribbon wires. Power connections to the driver amplifier are made by connecting wires to screw terminal, J8.

Through-hole components are used in construction. Surface mount (SMT) parts would not reduce the area of the circuit board by much because the 2-channel relay board and 3W driver amplifier are relatively large, and the driver amplifier connects to the circuit board with right angle SMA adapters.

Two SMA connectors provide circuit I/O.  SMA connecter, RF4, provides the interface to the transceiver bandpass filters while SMA connector, RF1, provides the interface to the power amp.

The relay coil is operated with supply +13.8 VDC while the driver amplifier is operated with regulated +9 VDC.

The circuit board layout is shown in Figure 5. Places for the 2-channel relay with mounting holes and the driver amplifier with mounting holes are provided. The driver amplifier will be connected to the PCB with right angle SMA-male to SMA-male adapters.

Figure 5. Driver Amplifier Receive Bypass Circuit Board Layout. This is the silkscreen view of the assembly. The dimensions of the board are visible in the photo. Please click on the image to open in a new screen.

A 3-D rendering of the design is provided in Figure 6. Please note that some of the components are missing because 3-D models were not provided for the entire online library.

Figure 6. A 3-D Rendering of the Driver Amplifier Receive Bypass Circuit Board Layout. This 3-D virtual reality image was generated by EasyEDA. Some of the components are missing because 3-D images of the parts were not found in the library. Please click on the image to open in a new screen.

Conclusions

A design has been described that may be useful in conjunction with just about any RF amplifier for use in ham radio transceivers. The amplifier receiver bypass described in this paper will permit bi-directional operation as is required in one direction on transmit and the opposite direction on receive.

References

[1] https://www.aliexpress.us/w/wholesale-3W-shortwave-amplifier.html?g=y&SearchText=3W+shortwave+amplifier&sortType=price_asc

[2] https://www.aliexpress.us/w/wholesale-30W-shortwave-amplifier.html?spm=a2g0o.productlist.search.0

[3] 3W shortwave amplifier. Op. cit.

[4] https://www.amazon.com/JunPus-JP-DX2-Diamond-Thermal-Grease/dp/B0D7ZB43CF/ref=sr_1_1?crid=2Y1JXHD9J9MJZ&dib=eyJ2IjoiMSJ9.4cYW0erokqTHc7fpr9sWpA.vo3kXvGYCUoitzHMexiezvzYV0lb71EJvz3U3OOC614&dib_tag=se&keywords=JP-DX2-JunPus&qid=1761789390&sprefix=jp-dx2-junpus+%2Caps%2C85&sr=8-1

[5] https://www.ti.com/lit/ds/symlink/lm317.pdf

[6] https://easyeda.com/

[7] https://jlcpcb.com/

Disclaimers

This circuit design is provided for informational and educational purposes only and is supplied “as is” and without warranties of any kind, express, implied, or statutory. No representations or warranties are made regarding the accuracy, adequacy, completeness, legality, reliability, or usefulness of this information, either in isolation or in the aggregate. This circuit design may contain links to or information based on external sources or third-party content. Endorsement and responsibility for the accuracy or reliability of such third-party information or for the content of any linked websites are not taken.

Some Fun with Boolean Algebra

Introduction

This article will demonstrate how a simple logic problem may be solved using Boolean algebra.

Background

In the late 1950’s through the early 1970’s something called “New Math” [1] was introduced into grade school curricula under an initiative from the National Science Foundation (NSF). However, New Math was a misnomer, and nothing could be further from the truth. The math wasn’t new at all. It was just that an NSF committee had decided to introduce the elements of something called symbolic logic to school children. The elements of symbolic logic had been taught in college-level mathematics and philosophy courses for at least 175 years! Some of us even used a text, Symbolic Logic [2], written by the student of Bertrand Russell [3], Irving Copi [4].

During the cold war, it was thought that an introduction to the idea of logical reasoning would be more beneficial to young students than rote learning [5].  It was perceived that the United States had fallen horribly behind the Soviets in the areas of science and mathematics [6]. While that may have been the case, it turned out that in attempting to teach these more advanced concepts to the young, it may have set a backward trajectory for math and science education for many years to come.

Sensing that something was missing from my school curricula in 1963; I audited a summer school algebra course being taught in the neighboring town. It featured New Math. Having been schooled in Old Math; I soon understood of how little use New Math would be, i.e., until I began to play with logic circuits. The next time I saw the material was when I took a course in digital logic about 12 years later.

As I think back, maybe the time spent teaching New Math would have been better spent teaching a few skills in critical thinking?  By the 1970’s New Math had been, ironically, supplanted by Old Math, and textbooks that illustrated Venn diagrams on the covers had largely vanished.

As the late Tom Lehrer [7] of MIT (and later of UC Santa Cruz) sardonically reflected in his song lyrics:

New math, new-hoo-hoo math,
It won’t do you a bit of good to review math!
It’s so simple, so very simple,
That only a child can do it!

Enter George Boole

George Boole was a self-taught philosopher, mathematician and logician who served as the first professor of mathematics at Queens College, Cork, Ireland, in 1849 [8].

If you suffered through a course in symbolic logic, Boolean Algebra would have been one of the topics along the way.

Boolean logic symbols, and logic symbols in general, differ somewhat from those of grade school mathematics. For example, the plus symbol (+) stands for the logical symbol “OR”. We won’t have to introduce the added complexity of the OR symbol in this paper but it is really not hard to use. The dot symbol ( · ) that normally stands for multiplication stands for “AND”. This symbol along with something called an inverter will be used to solve the logic problem described in this paper. An inverter has the property that whatever is present at the input appears inverted at the output.

The Logic AND Gate

The logic AND gate is represented by the symbol shown in Figure 1. An accompanying  truth table for the AND gate is also shown. What is important to remember about AND gates is that if any statement is false, the whole statement is false. This may be inferred from the truth table. The cases shown are,

1.      A is true and B is false; the ANDing of the two, X, is false,

2.      A is false and B is true; the ANDing of the two, X, is false,

3.      A is false and B is false; the ANDing of the two, X, is false, and

4.      A is true and B is true; the ANDing of the two, X, is true.

Figure 1. The Logical AND Gate. If either of the inputs, A or B, is false, the output, X, is false. Please click on the figure to open it in a new window.

The Logic Problem to Be Solved

A QRP radio is under construction and Rick, N3FJZ, is the author of the software that operates many features of the radio and the display.  Rick maintains a website [9] as well as a YouTube channel [10]. Both sites are dedicated to homebrewing.

Since the software was intended for SSB operation, not CW, there is a logic state that is disallowed whenever band privilege restrictions are not entered as part of initial software setup. CW operation was never intended to be part of software setup [11].

There are two distinct modes of operation: general coverage receive and ham band transceive. If the receive frequency is set to anything other than a ham band, a general coverage command is asserted by the software. This command will switch out the low-pass filters, the power amplifier, and the band-pass filters. In their place, the command injects a bypass path around them. It is when the radio is in this state that Push-to-Talk (PTT) may be asserted, and the power amplifier will be biased. This should be disallowed.

A Possible Hardware Solution

Instead of modifying the code, a simple hardware modification is possible that will lock out the disallowed transmit state for the radio in general coverage mode.

It is known that a filter bypass flag appears on one of the Arduino microcontroller pins when the radio is tuned to anything other than one of the ham bands.

It is also known that a PTT flag appears on one of the Arduino microcontroller pins when the microphone PTT button is pressed or the PTT button on the control panel is pressed.

If we could use the filter bypass flag to inhibit transmit PTT whenever the radio is tuned to general coverage, the problem would be solved.

Figure 2 shows a truth table for the hardware solution for the problem as it is understood.

Figure 2. A Truth Table That Shows the Hardware Solution for the Problem as It Is Understood. All possible states of the PTT switch are shown in column A. All possible states of the Filter Bypass General Coverage command are shown in column B. Only one output state of X should be permitted. That is the one for which PTT is asserted and the radio is tuned within a ham band, either a SSB segment or a CW segment. All other cases shown in the truth table should be inhibited. Please click on the figure to open it in a new window.

The truth table in Figure 2 may be reduced to a single logical equation since we are only interested in the case for which X = 1. (any letter with a bar above it is the inverse of logical one, or zero). Thus,

This is read as A and B-bar equals X. The logic symbol that represents this is shown in Figure 3. Here we have drawn the symbol of a logical inverter to invert the symbol, B, to make it B-bar.

Figure 3. Simple Logic Circuit That Will Solve the Problem. For the single case of interest, A enters one of the AND gate inputs directly while B is inverted by an inverter gate so that it becomes one, or true, at the other AND gate input. We are not finished with the circuit because it would involve the purchase of two types of gates, and that seems wasteful because an inverter gate and an AND gate would be required. Please click on the figure to open it in a new window.

Let’s see if this circuit can be implemented with NAND gates. A NAND gate may be thought of as an AND gate whose output has been inverted. Thus, we can implement Figure 3 with NAND gates as shown in Figure 4. An inverter gate may be created by tying the two inputs of a NAND gate together. As an exercise, try applying all of the A and B inputs in the truth table of Figure 2 to Figure 4 to be convinced that this logic diagram will work. One way of looking at it is to observe that we have a NAND gate that has been inverted. That produces an AND gate. Thus, Figures 3 and 4 are equivalent.

Figure 4. The Logic Diagram Of Figure 3 Implemented With NAND Gates Only. This may be implemented with a single 14-pin dual inline package (DIP) or surface mount package (SMP). The gates come four gates to a package so the extra gate may be used for an extra output or it may be tied high, if unused, to prevent it from toggling. The CD4011 would be ideal for this project because of its wide supply voltage range. Please click on the figure to open it in a new window.

Printed Circuit Board Layout

A printed circuit board layout was completed for a single CD4011 Quad NAND gate on the free, easy-to-use EasyEDA online graphics package [12]. The board is being fabricated by JLCPCB [13] for rapid turnaround.  The schematic diagram is shown in Figure 5. A 3-D rendering is shown in Figure 6. The total board area is approximate 1 square inch, and it will fit nicely onto the corner of the front panel PCB as a mezzanine board. There, it will connect directly to the Arduino MEGA 2560 to perform the lockout function.

Figure 5. Transmit Lockout PCB. The schematic was completed on the easy-to-use EasyEDA online graphics package, as was the Gerber file for PCB fabrication. Please click on the figure to open it in a new window.

.

Figure 6. The CD4011 Quad NAND Gate 3-D PCB Layout. A single CD4011 Quad NAND gate is all that is necessary to implement the transmit lockout during general coverage mode. The screw terminal strips do not appear in the virtual rendering because they were unavailable in the library. Please click on the figure to open it in a new window.

References

[1] New Math, https://en.wikipedia.org/wiki/New_Math

[2] Russell, Bertrand, https://en.wikipedia.org/wiki/Bertrand_Russell

[3] Copi, Irving, Symbolic Logic, 5th ed., Pearson, 1 Jan 2015.

[4] Copi, Irving, https://en.wikipedia.org/wiki/Irving_Copi

[5] Rote Learning, https://en.wikipedia.org/wiki/Rote_learning

[6] Sputnik, https://news.harvard.edu/gazette/story/2007/10/how-sputnik-changed-u-s-education/

[7] Lehrer, Tom, https://en.wikipedia.org/wiki/Tom_Lehrer

[8] Boole, George, https://en.wikipedia.org/wiki/George_Boole

[9] Scott, Rick, N3FJZ, Circuit6040 website, http://www.remmepark.com/circuit6040/

[10] Scott, Rick, N3FJZ, Circuit6040 YouTube Channel, https://www.youtube.com/results?search_query=circuit6040

[11] Scott, Rick, N3FJZ, Circuit6040 YouTube, Module # 110 Front Panel MEGA Quick Start – MAX-SSB Transceiver Project, https://www.youtube.com/watch?v=5a9tlg8SIrk

[12] EasyEDA,  https://easyeda.com/

[13] JLCPCB,  https://JLCPCB.com/

Disclaimers

These circuit designs are provided for informational and educational purposes only and are supplied “as is” and without warranties of any kind, express, implied, or statutory. No representations or warranties are made regarding the accuracy, adequacy, completeness, legality, reliability, or usefulness of this information, either in isolation or in the aggregate. These circuit designs may contain links to or information based on external sources or third-party content. Endorsement and responsibility for the accuracy or reliability of such third-party information or for the content of any linked websites are not taken.

 

 

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