Loss Model for Gallium Nitride DC-DC Buck Converter · Student: Rushi Patel Faculty Advisor: Dr....
Transcript of Loss Model for Gallium Nitride DC-DC Buck Converter · Student: Rushi Patel Faculty Advisor: Dr....
Student: Rushi PatelFaculty Advisor: Dr. Daniel Costinett
Final Presentation7/14/2016
University of Tennessee
Loss Model for Gallium Nitride DC-DC Buck Converter
Applications
2
•Mobile phone charger
•Electric vehicles
•Solar energy
•Wind energy
•Loss model canbe use for different topologies of converters
Background
3
Type Silicon Carbide
Vin 12V
Vout 1.2V
fsw 300kHz
Vdd 12V
L 1uH
DCR 1mΩ
Type Gallium Nitride
Vin 12V
Vout 1.2V
fsw 1MHz
Vdd 10V
L 280nH
DCR .29mΩ
Compare
Objective
4
•Compare theoretical, LTspice simulation and experimental efficiency data
•Develop a theoretical and experimental loss model for 500kHz and 1MHz
• Find the constant variables that causes difference in theoretical and experimental loss model to reduce the iterative process of hardware prototyping
Method
5
• eGaN DC-DC buck converter
• Take measurements at the input and
output terminals for currents and voltages
• Plot efficiency vs output current graph to
compare with theoretical data
Experimental
EPC 9036 Development Board
Method
6
Theoretical
•To evaluate different losses, input and output
power using datasheets for transistors, inductor
and capacitor.
•Plot efficiency vs output current graph to
compare with experimental data
Different Types of Losses• Switching loss on high side
• Conduction loss on high side and low side
• Inductor loss
• Capacitor loss
• Gate drive loss
• Dead-time loss
• Output capacitance loss on high side and low side
• Core loss
Method
7
Simulation
•Model all the parts with its
parasitic components
• Plot efficiency vs output
current graph to verify
experimental data
Results
8
•At lower current, experimental efficiency is higher than theoretical efficiency
Results
9
•Efficiency is about 90% at higher current and higher frequency for eGaN buck converter compare to silicon carbide buck converter.
Results
10
• Approximately at 10A, the loss difference approaches 0 watts
Results
11
• Second order Polynomial fits best in both cases
Results
12
• All the equations of second order:
• Conduction loss on high side: Rds_on_HS*Irms_HS^2
• Conduction loss on low side: Rds_on_LS*Irms_LS^2
• Inductor loss : Irms_L^2*DCR
• Capacitor loss: Iripple^2*ESR
Results
13
• Rds_on_LS : Measured between 5mΩ and 7mΩ. Theoretical: 6mΩ
• Rds_on_HS: Measured between 1mΩ and 2.2mΩ. Theoretical: 1.5mΩ
• DCR: Measured between 1mΩ and 3mΩ. Theoretical: .29mΩ
• ESR: Requires precise measurement. Theoretical: 2mΩ
Results
14
• DCR value for theoretical data changed from .29mΩ to 2mΩ
Results
15
• DCR value for theoretical data changed from .29mΩ to 2mΩ
Conclusion/Future work
16
• DCR in the inductor causes the difference between theoretical and experimental loss model
•Different frequencies give loss model of same trends
• Complex experiments can be done to get precise measurements for future work
• Analyze the initial difference between experimental and theoretical efficiency
• Create new designs with different inductor and capacitor value to compare
Acknowledgements
This work was supported primarily by the ERC Program of the National Science Foundation and DOE under NSF Award Number EEC-1041877.
Other US government and industrial sponsors of CURENT research are also gratefully acknowledged.
17
Questions and Answers
18