Available at http://freescale.com/RFbroadcast Freescale Semiconductor Technical Data > Design Support > Reference Designs Rev. 0, 6/2011 High Ruggedness N--Channel Enhancement--Mode Lateral MOSFETs 170--230 MHz, 225 W AVG., 50 V VHF DIGITAL TV BROADCAST REFERENCE DESIGN VGG BIAS Reference Design Characteristics Solid--state broadcast transmitters require transistors that are broadband, highly efficient and very rugged. There is also demand for transistors with higher power capability to minimize device count and combining losses. This document describes the design and performance of a VHF DVB--T power amplifier using the MRFE6VP61K25H LDMOS transistor. • Frequency Band: 170--230 MHz • Output Power: 225 Watts Avg. DVB--T RF INPUT • Supply Voltage: 50 Vdc • Power Gain (Typ): 25 dB + The MRFE6VP61K25H device is capable of 1250 watts CW operation and suitable for high power applications between 1.8 and 600 MHz. The LDMOS technology used is designed to operate at 50 volts, thereby increasing the power capability per device and reducing the number of devices needed per system. A temperature compensation circuit has been included in the amplifier design to keep the quiescent current stable over temperature. M = Match M M RF OUTPUT + - M BIAS • Drain Efficiency (Typ): 30% VDD BIAS VHF Digital TV Broadcast Reference Design MRFE6VP61K25H MRFE6VP61K25HS VHF Broadcast VGG M BIAS RF Power Reference Design Library VDD VHF DIGITAL TV BROADCAST REFERENCE DESIGN This reference design is designed to demonstrate the RF performance characteristics of the MRFE6VP61K25H/HS devices when applied to the 170--230 MHz VHF broadcast frequency band. The reference design is tuned for performance at 225 watts avg. output power, VDD = 50 volts and IDQ = 2.0 A. own product or products. The reference design contains an easy--to--copy, fully functional amplifier design. It consists of “no tune” distributed element matching circuits designed to be as small as possible, and is designed to be used as a “building block” by our customers. REFERENCE DESIGN LIBRARY TERMS AND CONDITIONS When operating this fixture it is critical that adequate heatsinking is provided for the device. Excessive heating of the device may prevent duplication of the included measurements and/or destruction of the device. Freescale is pleased to make this reference design available for your use in development and testing of your HEATSINKING Figure 1. VHF Broadcast Reference Design Fixture © Freescale Semiconductor, Inc., 2011. All rights reserved. RF Reference Design Data Freescale Semiconductor MRFE6VP61K25H MRFE6VP61K25HS VHF Broadcast 1 MEASUREMENTS or over their rated temperature at such high power. Therefore a pulsed signal is used to measure power, gain and efficiency of the amplifier. As shown in Figure 3, the P1dB is more than 1250 watts with an IDQ of 150 mA. The results with IDQ = 2.0 A is shown in Figure 4. The power capability and P1dB with a pulsed signal gives an indication of the average DVB--T power that the amplifier is capable of with a PAR above 8 dB (0.01% probability, CCDF) and a (non--corrected) shoulder distance below --30 dBc. A rough estimation is that the available DVB--T average power is about 7 dB below the pulsed P1dB power. SMALL SIGNAL The amplifier is first measured with a small signal over a large frequency range to verify that there are no resonances or gain peaks due to the transistor matching or decoupling network. The small signal measurement can be seen in Figure 2. PULSED Although the MRFE6VP61K25H device is capable of 1250 watts CW operation, some of the matching components, e.g. capacitors used in this DVB--T amplifier, could be close to 40 30 20 Gps 20 10 0 IRL (dB) 10 --10 0 IRL --10 --20 --30 --20 VDD = 50 Vdc IDQ = 2.0 A --30 --40 --40 0 50 100 Gps, POWER GAIN (dB) 30 150 200 250 300 --50 400 350 f, FREQUENCY (MHz) Figure 2. Small Signal Characteristics 170 MHz 230 MHz 80 26.5 70 26 24 170 MHz 60 23 50 22 40 230 MHz 21 VDD = 50 Vdc, IDQ = 150 mA Pulse Width = 50 μsec Duty Cycle = 2.5% ηD 20 19 0 200 30 400 600 800 1000 1200 1400 1600 20 10 1800 Gps 230 MHz 170 MHz 25.5 80 200 MHz 70 60 200 MHz 170 MHz 25 230 MHz 24.5 50 40 24 30 23.5 23 20 VDD = 50 Vdc, IDQ = 2.0 A Pulse Width = 50 μsec Duty Cycle = 2.5% ηD 10 22.5 0 200 400 600 800 1000 ηD, DRAIN EFFICIENCY (%) Gps 200 MHz Gps, POWER GAIN (dB) Gps, POWER GAIN (dB) 25 200 MHz ηD, DRAIN EFFICIENCY (%) 26 1200 1400 1600 0 1800 Pout, OUTPUT POWER (WATTS) PULSED Pout, OUTPUT POWER (WATTS) PULSED Figure 3. Pulsed Power Gain and Drain Efficiency versus Output Power Figure 4. Pulsed Power Gain and Drain Efficiency versus Output Power MRFE6VP61K25H MRFE6VP61K25HS VHF Broadcast 2 RF Reference Design Data Freescale Semiconductor A DVB--T signal with a 9.6 dB peak--to--average (PAR) ratio at 0.01% probability on CCDF was used to quantify the broadband performance of the MRFE6VP61K25H device under a digital modulation scheme. The circuit is air--cooled and the device bolted down to the heatsink with thermal grease (Figure 1). Figure 5 illustrates typical broadband performance at 225 watts avg. DVB--T power. The PAR is above 8 dB across the VHF band of 170--230 MHz with a 30% efficiency and gain of 25 dB. 10 40 35 9.5 ηD 9 30 PAR 25 8 27 7.5 7 6.5 6 170 26 Gps 25 VDD = 50 Vdc IDQ = 2.0 A Pout = 225 W Avg. DVB--T 180 190 24 200 210 Gps, POWER GAIN (dB) PAR (dB) 8.5 ηD, DRAIN EFFICIENCY (%) The drive up data in Figures 6 and 7 shows that it is reasonable to use the device up to 250 watts avg. DVB--T power and still have a PAR above 8 and shoulder distance below --30 dBc. This is in line with the rough estimation that the average DVB--T power is about 7 dB below the pulsed P1dB. The shoulder distance is measured using delta marker at ±4.2 MHz offset. The device can be used at lower supply voltage for lower output power or to optimize the tradeoff between linearity and efficiency. Decreasing the supply voltage will improve efficiency and decrease the linearity. DVB--T 23 230 220 f, FREQUENCY (MHz) Figure 5. DVB--T Peak--to--Average Ratio, Power Gain and Drain Efficiency versus Frequency 9.5 9 230 MHz PAR (dB) 7.5 35 30 230 MHz 200 MHz 6.5 6 150 --22 40 ηD 7 55 45 200 MHz 8 --20 50 PAR 8.5 170 MHz 60 25 170 MHz 170 190 210 230 20 250 Pout, OUTPUT POWER (WATTS) DVB--T AVG. Figure 6. DVB--T Peak--to--Average Ratio and Drain Efficiency versus Output Power --24 SHOULDER (dBc) VDD = 50 Vdc IDQ = 2.0 A ηD, DRAIN EFFICIENCY (%) 10 --26 --28 --30 --32 +4.2 MHz --34 --4.2 MHz --36 --38 --40 150 160 170 180 190 200 210 220 230 240 250 Pout, OUTPUT POWER (WATTS) DVB--T AVG. Figure 7. Power Sweep DVB--T Signal Frequency @ 200 MHz MRFE6VP61K25H MRFE6VP61K25HS VHF Broadcast RF Reference Design Data Freescale Semiconductor 3 AMPLIFIER DESIGN MATCHING NETWORK The first element in the output matching is a LC network made of microstrip lines and capacitors. The LC section is followed by a 4:1 coaxial transformer. The impedance of the coaxial cable is 25 Ω, which is the optimum impedance for a transformation from 12.5 to 50 Ω, following the equation Z = Z in × Z out. A 1:1 balun made of a 50 Ω coaxial cable together with capacitors are finalizing the matching network to 50 Ω at the output of the demo board. Due to the relatively high power of the amplifier, several capacitors were used in parallel instead of using only one. By using multiple capacitors, the total ESR (Equivalent Series Resistance) will be lower which improves the current handling capability. A printed circuit board (PCB) with high thermal conductivity was also selected to improve the thermal capability of the amplifier and reduce the temperature of the components used in the matching network. The input matching network is made in a similar way. Simulation software was used to get a first approach of the values needed and to understand the impact of each matching element. In addition to the matching network, the decoupling circuits for gate and drain bias supply needs to be carefully designed. Small signal measurement and a low frequency probe was used to verify that the decoupling was adequate and without resonances. A nonlinear electro--thermal transistor model for the MRFE6VP61K25H transistor is available for customers to optimize their design. The model is available online from Freescale’s RF High Power Model Library at http://freescale.com/rf/models. Supported CAD tools include Agilent EEsof’s ADS and Microwave OfficeR from AWR Corporation. TEMPERATURE COMPENSATED BIAS CIRCUIT Temperature Coefficient of the Transistor The RF performance of a power amplifier depends on the quiescent current, IDQ. For a fixed gate bias voltage, VGS, the IDQ increases with temperature. A thermal tracking circuit is introduced to compensate for the quiescent current variation versus temperature. Figure 13 shows the PCB layout with components for the amplifier including the thermal tracking circuit. The tracking circuit is using a voltage regulator (U1) to provide a stable +5 volts.(1) A resistor network including a potentiometer (R7) sets VGS to the desired IDQ. The resistor values are selected to have a tuning range for the VGS to be between 1.1 and 3.2 volts, hence covering both Class AB and Class C operation. The bipolar NPN transistor (Q1) is used as a thermal tracking device. If the current through the transistor Q1 is kept constant, the base--emitter voltage decreases with increasing temperature. The temperature coefficient of the transistor (Q1) depends on the collector current, IC, and can be found in the data sheet for Q1. For IC = 4 mA, the temperature coefficient is around --2.1 mV/°C. This reduction in voltage is used to compensate for the increase in IDQ of the LDMOS device due to temperature. The temperature coefficient for the MRFE6VP61K25H was measured using a heat and cooling plate. The VHF amplifier with its copper heatsink was placed on the plate and the temperature varied between 0°C and 100°C. The temperature was measured close to the transistor. The gate voltage was adjusted to keep the quiescent current constant over temperature. The measurement was done for quiescent currents of 150 mA, 1.0 A and 2.0 A. The results are plotted in Figure 9. To keep the IDQ constant at 2.0 A, the gate voltage needs to be reduced with 2.1 mV/°C. The temperature coefficient of the device is depending on the bias point, which explains the difference in thermal coefficient for IDQ = 150 mA (--2.4 mV/°C), IDQ = 1.0 A (--2.3 mV/°C) and IDQ = 2.0 A (--2.1 mV/°C).(2) The next step is to measure the thermal compensation circuit when the temperature is varied between 0°C and 100°C. The temperature coefficient for the compensation circuit is --2.1 mV/°C. As can be seen in Figure 10, the circuit compensates well the thermal coefficient of the LDMOS device. Figure 11 shows the behavior for the amplifier with the temperature compensation circuit. The temperature variation is less than 5% between 25°C and 115°C. FIXTURE IMPEDANCE VDD = 50 Vdc, IDQ = 2.0 A, Pout = 225 W Avg. DVB--T f MHz Zsource Ω Zload Ω 170 1.1 + j4.5 2.7 -- j0.2 200 2.1 + j5.1 2.2 + j1.1 230 1.6 + j4.1 2.1 + j2.1 Zsource = Test circuit impedance as measured from gate to gate, balanced configuration. Zload = Test circuit impedance as measured from drain to drain, balanced configuration. Input Matching Network + Device Under Test -- -Z source Output Matching Network + Z load Figure 8. Series Equivalent Source and Load Impedance MRFE6VP61K25H MRFE6VP61K25HS VHF Broadcast 4 RF Reference Design Data Freescale Semiconductor TEMPERATURE COMPENSATED BIAS CIRCUIT 2.8 2.75 2.7 2.7 2.5 2.4 1.0 A 2.6 Compensation Circuit 2.55 2.3 150 mA 2.2 VGS to keep IDQ = 2.0 A 2.65 IDQ = 2.0 A VGS (V) VGS (V) 2.6 VDD = 50 Vdc IDQ = 2.0 A 2.5 2.1 2.45 0 20 40 60 TEMPERATURE (°C) 80 100 20 0 Figure 9. VGS versus Temperature to keep IDQ Constant 40 60 TEMPERATURE (°C) 80 100 Figure 10. Temperature Compensation Circuit versus VGS to keep IDQ = 2.0 A 2.5 2.4 IDQ (A) 2.3 2.2 2.1 2.0 1.9 1.8 20 VDD = 50 Vdc VGS = 2.65 V 40 60 80 100 120 TEMPERATURE (°C) Figure 11. IDQ Drift with Temperature Compensation Circuit MRFE6VP61K25H MRFE6VP61K25HS VHF Broadcast RF Reference Design Data Freescale Semiconductor 5 CIRCUIT DESCRIPTION U1 VGS C2 R3 C1 C4 R5 R4 R8 R7 R6 C3 C5 C6 C7 L1 R2 Q1 COAX2 R1 RF INPUT C9 COAX1 C12 C13 C11 C8 L3 C14 C15 C10 COAX3 C33 C34 C35 C36 C37 C38 VDD L2 COAX4 C19 C17 C16 C18 C20 C21 C22 C23 C24 C25 C26 C27 C28 COAX6 RF OUTPUT C29 C30 C31 C32 COAX5 Figure 12. VHF Broadcast Reference Design Schematic Diagram MRFE6VP61K25H MRFE6VP61K25HS VHF Broadcast 6 RF Reference Design Data Freescale Semiconductor R6 C3 R4 R7 C5 R5 C2 C6 R1 R8 R3 VGS R2 Q1 C35 C36 U1 C34 VDS C33 C1 C19 C20 C7 C13 C12 L1 COAX2 C9 COAX4 CUT OUT AREA C8 L3 C10 C11 C38 C37 C4 C14 C15 COAX1 L2 C16* C17* C26* C27* C28* C23* C29* C30* C18* C24* C21 C22 COAX5 COAX3 C25* C31* C32* COAX6 MRFE6VP61K25H_VHF Rev. 1 *C16, C17, C18, C23, C24, C25, C26, C27, C28, C29, C30, C31, C32 are mounted vertically. Figure 13. VHF Broadcast Reference Design Component Layout Table 1. VHF Broadcast Reference Design Component Designations and Values Part Description Part Number Manufacturer C1 2.2 μF, 100 V Chip Capacitor HMK432B7225KM--T Taiyo Yuden C2, C12, C13, C14, C15 1 μF Chip Capacitors GRM21BR71H105KA12L Murata C3 10 nF Chip Capacitor C0805C103J5RAC--TU Kemet C4 220 μF, 63 V Electrolytic Capacitor 227CKS050M Illinois Capacitor C5 100 nF Chip Capacitor CDR33BX104AKWS Kemet C6, C25, C26, C27, C28, C29, C30, C31, C32, C33 1000 pF Chip Capacitors ATC800B102JT50XT ATC C7 2.2 μF, 50 V Chip Capacitor C3225X7R1H225KT TDK C8 22 pF Chip Capacitor ATC800B220JT500XT ATC C9, C10 5.1 nF Chip Capacitors ATC700B512JT50XT ATC C11 36 pF Chip Capacitor ATC100B360JT500XT ATC C16, C17 39 pF Chip Capacitors ATC800B390JT500XT ATC C18 47 pF Chip Capacitor ATC800B470JT500XT ATC C19, C22 1 μF Chip Capacitors GRM32CR72A105KA35L Murata C20, C21, C36 2.2 μF Chip Capacitors HMK432B7225KM--T Taiyo Yuden C23, C24 8.2 pF Chip Capacitors ATC800B8R2CT500XT ATC C34 10 nF Chip Capacitor ATC200B103MT50XT ATC C35 100 nF Chip Capacitor C1812F104K1RAC Kemet C37, C38 470 μF, 63 V Electrolytic Capacitors MCGPR63V477M13X26--RH Multicomp L1 10 Turns, #22 AWG Magnetic Wire 8077 Belden L2 10 Turns, #16 AWG Magnetic Wire 8074 Belden L3 2.5 nH Inductor A01TKL Coilcraft (continued) MRFE6VP61K25H MRFE6VP61K25HS VHF Broadcast RF Reference Design Data Freescale Semiconductor 7 Table 1. VHF Broadcast Reference Design Component Designations and Values (continued) Part Description Part Number Manufacturer R1 2.2 kΩ, 1/8 W Chip Resistor CRCW08052K20FKEA Vishay R2 1.2 kΩ, 1/8 W Chip Resistor CRCW08051K20FKEA Vishay R3 10 Ω, 1/8 W Chip Resistor CRCW080510R0FKEA Vishay R4 1 kΩ, 1/8 W Chip Resistor CRCW08051K00FKEA Vishay R5 3.9 kΩ, 1/8 W Chip Resistor CRCW08053R90FKEA Vishay R6 200 Ω, 1/8 W Chip Resistor CRCW0805200RFKEA Vishay R7 5 kΩ Potentiometer CMS Cermet Multi--turn 3224W--1--502E Bourns R8 10 Ω, 1/4 W Chip Resistor CRCW120610R0FKEA Vishay Q1 Bipolar NPN Transistor BC847ALT1G On--Semiconductor U1 Voltage Regulator LP2951ACDMR2G On--Semiconductor Coax1 50 Ω, 5.11″ RG--316 Micro--Coax Coax2, Coax3 24 Ω, 2.75″ TC--24 RF Power Systems Coax4, Coax5 25 Ω, Semi Rigid RF Cable, .118″ Line, 2.56″ length. UT141--25 Micro--Coax Coax6 50 Ω, 4.72″ EC141--50 Quickform/Hand Formable NEXANS PCB* 0.030″, εr = 3.5 TC350 Arlon Heatsink NI--1230 Copper Heatsink C193X280T970 Machine Shop *PCB artwork for this reference design is available at http://freescale.com/RFbroadcast > Design Support > Reference Designs. FREESCALE RF POWER 50 V TECHNICAL ADVANTAGES ENHANCED VHV6 The MRFE6VP61K25H is fabricated using Freescale’s sixth--generation, very high voltage 50 V LDMOS process technology with enhanced ruggedness (VHV6E). The VHV6 technology was introduced by Freescale several years ago and was a breakthrough for high power devices used for broadcast and other applications like industrial, scientific and medical (ISM) and commercial aerospace, where high power density is required. The high power capability per device allows the MRFE6VP61K25H to reach more than 1.25 kW peak power over the entire VHF band. The VHV6E technology is a further development of the VHV6 technology with improved ruggedness. RUGGEDNESS Ruggedness, the ability of the transistor to withstand severe load mismatch conditions under high output power without device failure or degradation in device performance, is a very important parameter when designing a broadcast amplifier. Although the matching circuit plays a role in determining the ruggedness of the amplifier, the intrinsic LDMOS ruggedness of the device is the foundation for the overall amplifier ruggedness. The ruggedness failure of the MOSFET is the result of a drain breakdown (impact ionization) event. As described in Freescale’s 50 V RF LDMOS White Paper, there are three ruggedness failure mechanisms that can occur as a result of a drain impact ionization event.(3) The first two mechanisms involve the basic breakdown of the MOSFET drain junction, either laterally across the channel or vertically across the drain to source junction isolation. The third mechanism is triggered by an impact ionization event and is the self biasing “snapback” of the parasitic bipolar device. The MRFE6VP61K25H device has been designed to address the three failure mechanisms resulting in extremely rugged devices. The MRFE6VP61K25H is capable of handling a load mismatch of 65:1 VSWR @ 50 Vdc. RELIABILITY In addition to ruggedness, the MRFE6VP61K25H transistor has been developed to meet quality and reliability standards demanded by transmitter manufacturers and operators. There is an MTTF (Median--Time--To--Failure) calculator(4) available to assist the customers in estimating the MRFE6VP61K25H device reliability in terms of electromigration wear--out mechanism. The MTTF is more than 1000 years when operated at VDS = 50 V, Pout = 1250 W CW, efficiency = 75%, Tcase = 63°C and TJ = 128°C. The device is qualified for a maximum operating junction temperature, TJ, of 225°C. MRFE6VP61K25H MRFE6VP61K25HS VHF Broadcast 8 RF Reference Design Data Freescale Semiconductor Enhanced ESD Operational reliability is also an important aspect of design as reflected in stability of the device performance over its lifetime. All MOSFETs suffer from degradation due to hot carrier injection (HCI). In the case of NMOS FETs, high energy electrons are generated due to high electric fields near the drain corner of the gate. These “hot” carriers can be injected and trapped in the nearby oxide layers over time and impact device performance such as threshold voltage. A shift in threshold voltage will decrease the quiescent current (IDQ) and alter the RF performance. Several device design innovations have been incorporated into the 50 volt VHV6 platform to result in IDQ drift for the MRFE6VP61K25H of less than 5% over 20 years. 2.E--02 IESD (A) 1.E--02 5.E--03 0.E+00 --5.E--03 --1.E--02 --2.E--02 --15 --10 --5 0 5 10 VGS (V) 15 20 25 15 20 25 Standard ESD 2.E--02 1.E--02 IESD (A) ESD PROTECTION The MRFE6VP61K25H device incorporates enhanced protection against electrostatic discharge (ESD), which makes it less susceptible to damage during handling and manufacturing. As shown in Figure 14, the enhanced ESD protection also increases the maximum rating for the Gate--Source Voltage to --6.0 to +10 Vdc, which in turn allows a greater negative voltage swing without turning on the ESD structure. One example where this feature is very beneficial is Class C operation at high input RF power levels. 5.E--03 0.E+00 --5.E--03 --1.E--02 --2.E--02 --15 --10 --5 0 5 10 VGS (V) Figure 14. Gate Voltage Breakdown with ESD THERMAL BEHAVIOR THERMAL RESISTANCE Accurate thermal characterization of the RF power transistor as well as the circuit components is necessary to analyze the reliability of the system in which the device is used. To calculate the junction--to--case thermal resistance (RθJC), the maximum die surface temperature (TJ) during amplifier operation, the case temperature (TC) and the dissipated power (Pdiss) must be known. Total dissipated power is calculated as: Pdiss = [RF input power + DC power (ID*VD)] -- (RF output power + RF reflected power) Junction--to--case thermal resistance is calculated as: RθJC = (TJ --TC)/Pdiss The maximum die surface temperature, TJ, of the device is measured with infrared (IR) microscopy, and a thermocouple element is used to measure the case temperature, TC. The thermal resistance of the MRFE6VP61K25H measured under CW signal: Tcase = 63°C, Pout = 1250 W CW, RθJC = 0.15°C/W The thermal resistance, RθJC, depends on both test condition and method. The thermal measurement methodology used by Freescale is described in Freescale Application Note AN1955, Thermal Measurement Methodology of RF Power Amplifiers.(5) REFLOW MOUNTING All RF performance data in this reference design document is taken with an air cooled copper heatsink and the device bolted down using a clamp and thermal grease as interface material. Reflow mounting, i.e. the device soldered to the heatsink, can be used to lower the overall thermal resistance which reduces the junction temperature and improves RF performance and reliability. For Si--based devices, each 15°C to 20°C reduction in junction temperature typically results in a doubling of the MTTF. Reflow mounting also improves the electrical contact. Proper grounding makes the power amplifier less susceptible to oscillation type damage. The MRFE6VP61K25HS is a version of the transistor with an earless package for optimal reflow mounting. More information can be found in Freescale Application Note AN1908, Solder Reflow Attach Method for High Power RF Devices in Air Cavity Packages.(6) CONCLUSION The design and performance of a VHF DVB--T power amplifier using the MRFE6VP61K25H has been presented. The MRFE6VP61K25H is a 1250 watt device fabricated using Freescale’s sixth--generation VHV6E 50 V LDMOS process technology. Under a DVB--T signal using OFDM modulation, the MRFE6VP61K25H achieves 225 watts avg. power at --30 dBc shoulder performance (±4.2 MHz offset) with 30% efficiency and 25 dB gain across the VHF band of 170 to 230 MHz. In addition to very good RF performance, the transistor is also designed for excellent ruggedness and reliability. A thermal compensation circuit is included in the amplifier design to keep the quiescent current constant over temperature. MRFE6VP61K25H MRFE6VP61K25HS VHF Broadcast RF Reference Design Data Freescale Semiconductor 9 REFERENCES 1. “RF LDMOS Power Modules for GSM Base Station Application: Optimum Biasing Circuit.” (Document Number: AN1643) Application Note, 1998. 2. O. Lembeye and J. C. Nanan, “Effect of Temperature on High Power RF LDMOS Transistors,” Applied Microwave & Wireless (2002). 3. 50 V RF LDMOS White Paper: “An Ideal RF Power Technology for ISM, Broadcast and Radar Applications”. Ref. 50VRFLDMOSWP. Av ailable at http://freescale.com/RFpower. 4. MRFE6VP61K25H MTTF c alc ulator av ailable at http://freescale.com/RFpower > Software & Tools > Dev elopment Tools > Simulations and Models > Calculators. Enter the “part number” into the Search field for quickest results. 5. “Thermal Measurement Methodology of RF Power Amplifiers.” (Document Number: AN1955) Application Note, 2004. 6. “Solder Reflow Attach Method for High Power RF Devices in Air Cavity Packages.” (Document Number: AN1908) Application Note, 2011. Technical documentation, including data sheets and application notes, for Freescale RF Power product can be found at: http://freescale.com/RFpower. Enter the applicable Document Number into “Keyword” search for quickest results. MRFE6VP61K25H MRFE6VP61K25HS VHF Broadcast 10 RF Reference Design Data Freescale Semiconductor APPENDIX A 1.929 (48.98) 8x #4--40 0.300″ deep 2.737 (69.51) 0.41 (10.41) 1.813 (46.04) 2.719 (69.07) E F A D A B D A 2.882 (73.19) A D E 0.813 (20.64) 0.140 (3.56) 1.309 (33.26) B 0.611 (15.52) F D 1.668 (42.38) 1.489 (37.83) ∅0.188 (∅4.76) 1.129 (28.69) 0.950 (24.14) B A D 0.130 (3.32) 0.125 (3.17) 4.725 (120.02) 4.499 (114.28) 2.929 (74.38) 2.283 (57.98) 1.724 (43.78) 2.134 (54.19) AA 1.929 (48.99) 1.558 (39.58) 0.929 (23.59) 0.000 (0.00) 0.00 (0.00) 0.177 (4.50) 0.000 (0.00) A 2.011 (51.08) 0.000 (0.00) 0.128 (3.25) 0.324 (8.23) D 4.548 (115.52) Copper Heatsink for VHF Broadcast Fixture inches (mm) C, Device Channel 0.038 (0.97) 0 (0.00) 0.300 (7.62) 0.720 (18.29) E Gutter is 0.030 wide and 0.046 deep, both sides 2.929 (74.39) 0.929 (23.59) E 0.720″ Copper Heatsink Hole Details Designators Details A 2 places, both sides, drill and tap, #2--56 screw depth 0.300″ B 2 places, both sides, 0.1875″ diameter notch 0.020″ deep C NI--1230 channel 0.410″ wide by 0.0380″ deep D 2 places, both sides, drill depth 0.250″ and tap for #4--40 screw E Locator holes from bottom diameter = 0.257″, depth = 0.400″ F 2 places, drill through and tap for #4--40 screw Figure 15. NI--1230 Heatsink MRFE6VP61K25H MRFE6VP61K25HS VHF Broadcast RF Reference Design Data Freescale Semiconductor 11 How to Reach Us: Home Page: www.freescale.com Web Support: http://www.freescale.com/support USA/Europe or Locations Not Listed: Freescale Semiconductor, Inc. Technical Information Center, EL516 2100 East Elliot Road Tempe, Arizona 85284 1--800--521--6274 or +1--480--768--2130 www.freescale.com/support Europe, Middle East, and Africa: Freescale Halbleiter Deutschland GmbH Technical Information Center Schatzbogen 7 81829 Muenchen, Germany +44 1296 380 456 (English) +46 8 52200080 (English) +49 89 92103 559 (German) +33 1 69 35 48 48 (French) www.freescale.com/support Japan: Freescale Semiconductor Japan Ltd. Headquarters ARCO Tower 15F 1--8--1, Shimo--Meguro, Meguro--ku, Tokyo 153--0064 Japan 0120 191014 or +81 3 5437 9125 support.japan@freescale.com Asia/Pacific: Freescale Semiconductor China Ltd. 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Freescalet and the Freescale logo are trademarks of Freescale Semiconductor, Inc. All other product or service names are the property of their respective owners. © Freescale Semiconductor, Inc. 2011. All rights reserved. MRFE6VP61K25H MRFE6VP61K25HS VHF Broadcast Available at http://freescale.com/RFbroadcast > Design Support > Reference Designs 12 Rev. 0, 6/2011 RF Reference Design Data Freescale Semiconductor