A 45W Amplifier for 23Cm LDMOS Technology Offers Easy and Economical Microwave Power

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A 45W Amplifier for 23Cm LDMOS Technology Offers Easy and Economical Microwave Power RADCOM ♦ JUNE 2009 DR JOHN C WORSNOP, CENG, MIET, G4BAO ♦ E-MAIL: [email protected] TECHNICAL FEATURE A 45W amplifier for 23cm LDMOS technology offers easy and economical microwave power. smaller heatsink with a fan can be used, as shown in Photo 1 . A mini kit consisting of the PCB and MRF9045 is available [3] . This project uses small surface mount devices and requires some experience to construct and set up. It is therefore not suitable for novice constructors. CIRCUIT DESCRIPTION. Researching designs for the MRF9045 and similar devices it seemed that matching these devices to 50Ω at 1.3GHz requires a relatively simple microstrip network with low impedance (ie wide) lines on the input and output. Half a day playing with Appcad [4] and a Smith chart program [5] allowed me to get a reasonable handle on the required matching networks. Figure 1 shows the complete circuit diagram. In order to reduce losses, the final circuit avoids using trimmers and shunt capacitors. Device input and output impedances are matched to 50Ω using series low impedance lines TRL2, 4 and 5. ‘Shunt’ lines facilitate the final tuning. The open circuit shunt lines TRL3, TRL6 perform the function of the shunt capacitors of lumped element designs and there is a short circuited shunt line on the input, TRL1, grounded at PHOTO 1: A prototype 23cm power amplifier fitted to small aluminium heatsink with fins running the end by C5. horizontally. A small black fan gives enough airflow to keep the heatsink cool (Photo: Colin, G8LBS). The 28 volt supply is connected to the drain via an isolating quarter wave high describes a 45W Class impedance line, TRL7 and decoupled over TABLE 1 - COMPONENT LIST AB Power amplifier a wide range of frequencies by C3, C4, C5 Component Value Type Farnell reference covering the 1.3GHz and C6. band that requires only Positive gate bias is fed via a similar high R1, R3, R4 820Ω SMD 0805 9334890 a few watts of drive for impedance line, TRL8, from a 5V regulator R2 10k SMD preset 1173884 C1, C2, C3 100pF Np0 ceramic 0805 1414655 full output. It is a and potential divider to set the standing drain C8 47pF Np0 ceramic 1206 1414734 modern, safe current to 350mA. The gate supply is C11 47pF Np0 ceramic 0805 1414692 replacement for a single decoupled by C7, C8 and C10. The C4, C7 1nF Np0 ceramic 0805 718567 2C39A valve amplifier connection to the gate is via ‘stopper resistor’ C5, C9 10µF 35V SMD electrolytic 8823120 and does not require a R1. This is essential to the design, as it vastly C6 100nF X7 ceramic 0805 9406387 hazardous high voltage improve low frequency stability of the amplifier. C10 47µF 16V SMD electrolytic 498762 power supply. It is ideal LDMOS devices are remarkably robust but they U1 MRF9045 LDMOS power FET www.g4bao.com for use with a DB6NT are susceptible to too much gate voltage. The U2 TS2937CW SMD 5V regulator 7261365 or similar transverter, only time I've destroyed a device during TRL1-8 Microstrip matching lines on PCB a Kenwood TS2000X development is when I omitted this resistor. or similar transceiver, Without gate bias the amplifier takes very reaching a power level little current. Switching the 5V regulator from INTRODUCTION. For many years I operated where the 1.3GHz band becomes interesting. the press to talk (PTT) line is a convenient on 23cm with just 2 watts RF output but The design is very simple and based way to switch the amplifier in and out of never experienced the aircraft scatter and around a single Freescale [1] MRF9045 28 standby, minimising standby power consistent over-the-horizon contacts that I volt LDMOS device. The PCB is designed to fit consumption and heat generation. knew the band could support. Increasing the in to a readily available 72 x 55 x 30mm power by 13dB or so opened up the band in tinplate box [2] , and should be bolted to a CONSTRUCTION. The PA is built on a ways I didn’t think possible. This article suitable large, heatsink. Alternatively, a special 0.8mm thick low loss Teflon PCB, the 63 TECHNICAL FEATURE JUNE 2009 ♦ RADCOM overlay for which is shown +12 V bi as sup ply FIGURE 1: 23cm power amplifier circuit diagram. in Figure 2 . I developed the (optionally PTT switched) design using RF35 from R3 U2 Taconic Advanced Dielectrics 820Ω TS2937C W Division in Ireland [6] to In Ou t whom I gratefully Gn d 1 acknowledge the sample C9 C10 2 R2 of material that allowed the 10μ 47μ 10k +28 V 3 development. C8 My first attempt at the C7 820Ω 47p 1n design, using cheap FR4 C3 C4 C5 C6 material, worked after a R1 100p 1n 10μ 0μ1 fashion, but produced much 820Ω less power and, more TRL 7 importantly, eventually failed, TRL 5 Outpu t as the losses in the board TRL 8 caused the output microstrip 47 p Inpu t C1 TRL 2 TRL 4 U1 line to heat up alarmingly MRF904 5 TRL 6 and produce smoke after 100p about 5 minutes! TRL 1 TRL 3 Table 1 shows the component list for the C2 amplifier. The only really 100p critical component is the 1206 capacitor for the output coupling. The MRF9045 used in the design is the drain and gate tabs go, bolted the Connect the amplifier output to in a TO270 solder-down plastic package. spreader and PCB tightly together. I then a power meter/ dummy load capable of These are now becoming more popular and dropped the module, spreader side down, dissipating and measuring at least 50W. eliminate the need for hazardous beryllium on the kitchen ceramic hob, turned it on Connect the drain to 28 volts via an oxide in the package. and waited for the solder to melt. It duly ammeter on the 1A range. Connect the The device is soldered to a piece of copper did, leaving a shallow ‘pool’ of solder in the gate bias supply, starting with minimum plate approximately 27mm square and 1mm rectangular hole in the PCB. I carefully placed volts on the gate and very carefully increase thick, which acts as a heat spreader between the device into the hole, pressing down with the gate voltage until the device begins to the MRF9045 and the heatsink. (Actually I the tweezers. I then quickly slid the module take current. This onset is very sharp, so be used one face cut from a piece of waveguide off the heat, keeping the pressure on the very careful, as the drain current can easily 16). The spreader is soldered to the device until the solder set. Once the device is swing up to many amps if you are not careful. underside of the PCB and has two holes fitted you can solder in the other components. Set the drain current to 350mA. Switch off drilled in it to allow the spreader to be bolted I have used this technique many times now power and then switch the ammeter to the to the heatsink. with no ill effects on the devices. If you have 10A range. Switch back on. Apply 0.5W Applications note AN1907 [7] from a proper hotplate, all the better; I have now drive and check the input VSWR. It should Freescale gives very strict guidelines on gone ‘upmarket’, using an old dry clothes be better than about 1.7:1. temperatures for soldering these devices but iron, that I clamp upside down in a vice; If the input VSWR and output power are I thought, "what the heck, I can’t afford a that does the trick just as well. about right you’re finished, so leave well soldering oven, but I can afford to sacrifice No special precautions or techniques alone! If not, switch off. Remove one section a couple of devices if it doesn’t work". So I are required for fitting the other components, of one input tab at a time until the VSWR is tinned the underside of the PCB, the mating apart from good microwave practice. Be less than 1.7:1 and check the output power surface of the spreader and the topside where particularly careful to avoid excess solder, and current. If necessary, trim the output whiskers or excessive flux tabs in the same way for maximum power. residues as these can Do NOT try to make these adjustments affect performance. with the amplifier operating. Turn up the drive in 3dB steps to 2W and check that ALIGNMENT. Bolt the the power increases about 3dB each time assembled board and until it saturates. Now trim the output tab for heat spreader to a large minimum current consistent with maximum heatsink. The input and output power. It goes without saying, I hope, output matching tabs are that you disconnect both the drain and source split so that you can bias supplies before you trim the tabs. lengthen or shorten them by bridging them with RESULTS. Test results for a prototype solder, if necessary. Start amplifier are shown in Figures 3 and 4. with all the tabs linked for maximum length. CONCLUSIONS. This is an inexpensive PA Connect the input from and is relatively easy to build, with readily your 1.3GHz transmitter to available components and produces a useful FIGURE 2: PCB overlay. the amplifier input via a increase in output power for transverters and suitable SWR meter. transceivers. 64 RADCOM ♦ JUNE 2009 TECHNICAL FEATURE FIGURE 3: Measured FIGURE 4: gain and Typical efficiency for power a prototype output and amplifier.
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