ECEN5817, ECEE Department, University of Colorado at Boulder Zero-voltage transition converters: the phase-shifted full bridge converter Buck-derived full-bridge converter A popular converter for server front- ECEN 5817 1 Zero-voltage switching of each half- bridge section Each half-bridge produces a square wave voltage. Phase-shifted control of converter output end power systems Efficiencies of 90% to 95% regularly attained Controller chips available Phase-shifted control Approximate waveforms and results (as predicted by analysis of the parent hard- switched converter) ECEN 5817 2
15
Embed
Zero-voltage transition converters: the phase-shifted full ...ecee.colorado.edu/~ecen5817/lectures/L40_ECEN5817_notes.pdf · ECEN5817, ECEE Department, Universi ty of Colorado at
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
ECEN5817, ECEE Department, University of Colorado at Boulder
Zero-voltage transition converters:the phase-shifted full bridge converter
Buck-derived full-bridge converter A popular converter for server front-
ECEN 58171
g
Zero-voltage switching of each half-bridge section
Each half-bridge produces a square wave voltage. Phase-shifted control of converter output
p pend power systems
Efficiencies of 90% to 95% regularly attained
Controller chips available
Phase-shifted control
Approximate waveforms ppand results
(as predicted by analysis of the parent hard-switched converter)
ECEN 58172
ECEN5817, ECEE Department, University of Colorado at Boulder
Actual waveforms, including resonant transitions
ECEN 58173
Result of analysisBasic configuration: full bridge ZVT
• Phase shift assumes the role of duty cycle d in converter equations
• Effective duty cycle is reduced by the resonant transition intervals
ECEN 58174
• Reduction in effective duty cycle can be expressed as a function of the form FPZVT(J), where PZVT(J) is a negative number similar in magnitude to 1. F is generally pretty small, so that the resonant transitions do not require a substantial fraction of the switching period
• Circuit looks symmetrical, but the control, and hence the operation, isn’t. One side of bridge loses ZVS before the other.
ECEN5817, ECEE Department, University of Colorado at Boulder
ZVT Analysis
ECEN 58175
Interval 1
ECEN 58176
ECEN5817, ECEE Department, University of Colorado at Boulder
Normalized state plane
ECEN 58177
Solution of state plane
ECEN 58178
ECEN5817, ECEE Department, University of Colorado at Boulder
Subintervals 2 and 3
ECEN 58179
Subinterval 4
ECEN 581710
ECEN5817, ECEE Department, University of Colorado at Boulder
Subinterval 5
ECEN 581711
ZVS: output current charges Cleg without requiring J > 1
Subinterval 6
• Current ic circulates around primary-side elements, causing conduction loss
• This current arises from stored energy in Lc
• The current is needed to induce ZVS during next subinterval
ECEN 581712
• To maxzimize efficiency, minimize the length of this subinterval by choosing the turns ratio n such that M = V/nVg is only slightly less than 1
ECEN5817, ECEE Department, University of Colorado at Boulder
Subintervals 7 to 11
Subintervals 7 to 11 and 0 are symmetrical to subintervals 1 to 6
Complete state plane trajectory:
ECEN 581713
Averaging
ECEN 581714
ECEN5817, ECEE Department, University of Colorado at Boulder
Phase-shift control
ECEN 581715
Phase shift control
ECEN 581716
ECEN5817, ECEE Department, University of Colorado at Boulder
Phase shift control: result
ECEN 581717
Effect of ZVT: reduction of effective duty cycle
ECEN 581718
ECEN5817, ECEE Department, University of Colorado at Boulder
Issues with this converter
It’s a good converter for many applications requiring isolation. But…
1. Secondary-side diodes operate with zero-current switching. They require snubbing or other protection to avoid failure associated with avalanche breakdown
2. The resonant transitions reduce the effective duty cycle and conversion ratio. To compensate, the transformer turns ratio must be increased, leading to increased reflected load current in the primary-side elements
3. During the D’Ts interval when both output diodes conduct, inductor Lc stores energy (needed for ZVS to initiate the next DTs interval) and its current circulates around the primary-side elements—causing conduction loss
ECEN 581719
p y g
Diode switching analysis
ECEN 581720
ECEN5817, ECEE Department, University of Colorado at Boulder
Diode commutation: intervals 3 and 4
ECEN 581721
ZCS of D6
ECEN 581722
ECEN5817, ECEE Department, University of Colorado at Boulder
Approaches to snub the diode ringing
ECEN 581723
Approaches to snub the diode ringing(a) conventional diode snubber
ECEN 581724
ECEN5817, ECEE Department, University of Colorado at Boulder
Approaches to snub the diode ringing(b) conventional passive voltage-clamp snubber
ECEN 581725
Approaches to snub the diode ringing(c) simplify to one passive voltage-clamp snubber
ECEN 581726
ECEN5817, ECEE Department, University of Colorado at Boulder
Approaches to snub the diode ringing(d) improvement of efficiency in voltage-clamp snubber
ECEN 581727
Approaches to snub the diode ringing(e) active clamp lossless snubber
ECEN 581728
ECEN5817, ECEE Department, University of Colorado at Boulder
Approaches to snub the diode ringing(f) primary-side lossless voltage clamp