Class-E Silicon Carbide VHF Power Amplifier For Space … · · 2010-04-11SiC Class-E amplifier...
Transcript of Class-E Silicon Carbide VHF Power Amplifier For Space … · · 2010-04-11SiC Class-E amplifier...
Class-E Silicon Carbide
VHF Power Amplifier
For Space Applications
Marc J. Franco
N2UO
Presented by: Bob McGwier, N4HY
Outline
• High efficiency, class-E VHF power amplifiers
• Active device requirements and available
technologies
• Restrictions imposed by space applications
• Amplifier design with silicon carbide (SiC)
MESFET
• Simulated and experimental results
Motivation
• Switch-mode operation (i.e. class-E) involves high
peak drain/collector voltage
• GaAs transistors are inherently low voltage devices
• LDMOS devices are not suitable for flight (oxide layer
susceptible to total radiation dose)
• Silicon carbide (SiC) and gallium nitride (GaN) are
ideal for high efficiency space applications
Class-E amplifiers
• Very high dc to RF efficiency by operating the
active device as a switch
• High peak drain or collector voltage (almost
4x class AB)
• High breakdown voltage devices are ideal
candidates
• Linearity can be restored by amplitude
modulation of the drain voltage (HELAPS)
Flight hardware issues
• Radiation hardness becomes a concern
• GaAs is the dominant semiconductor in space
applications
• GaAs devices have a low breakdown voltage – hard
to operate in class-E
• LDMOS transistors have higher breakdown voltage,
but generally cannot be used in high radiation
environments (oxide layer)
SiC and GaN in space?
• No oxide layer
• SiC solar cells have been flown
• SiC has excellent temperature properties
• Both SiC and GaN are ideal for class-E operation
• Weatherford and Anderson, “Historical perspective
on radiation effects in III-V devices,” IEEE
Transactions on Nuclear Science
SiC Class-E amplifier design
• Classic class-E schematic (Sokal)
• SiC MESFET SiC60pr by Cree
• Q=2.27, Vds=30V, RL=18 ohms
1000 pf
V= -13.5 V
SiC60pr3 24 pf
470 pf 0 - 30 V
12 pf 56 pf
68 pf 47 pf 22 pf
47 nH
90 nH
90 nH
82 pf 47 nH 56 nH220 nH
47 nH OUT
IN
• Output low pass filter
• Decoupling allows drain modulation
• No tuning elements
Input match
Waveform shaping Impedance matching
Low pass filter
Output power vs. drain voltage
MEASURED
SIMULATED
0
5
10
15
20
25
2 6 10 14 18 22 26 30
Vds [V]
Po
[W
]
Drain efficiency vs. drain voltage
70
75
80
85
90
95
100
2 6 10 14 18 22 26 30
Vds [V]
Eff
[%
]
SIMULATED
MEASURED
Power added efficiency vs. drain voltage
SIMULATED
MEASURED
20
30
40
50
60
70
80
90
2 6 10 14 18 22 26 30
Vds [V]
PA
E [
%]
SIMULATED
MEASURED
RF output voltage vs. drain voltage
0
10
20
30
40
50
2 6 10 14 18 22 26 30
Vds [V]
Vo
[V
]
Output power vs. frequency
15
17
19
21
23
25
140 142 144 146 148 150
Freq. [MHz]
Po
[W
]
SIMULATED
MEASURED
Summary of results
Parameter Simulated Measured
Maximum Output Power 21.5 W 20.5 W
Nominal Input Power 27 dBm 27 dBm
Maximum Drain Efficiency 88 % 86.8 %
Maximum Power Added Efficiency 84.8 % 83.5 %
Maximum spurs and harmonics -58 dBc -58 dBc
Gain 16.3 dB 16.11 dB
Conclusion
• SiC devices can be successfully used in class-E VHF operation
• This amplifier can be used on AMSAT Eagle’s 2 meter downlink
phase array
• Very high efficiency can be achieved (~87%)
• Greater break-down voltage than GaAs allows for high power
amplifier designs
• No oxide layer – advantage over LDMOS for space applications
• Very high operating temperature (120 ºC case, 255 ºC junction)