Fairchild Semiconductor FSFR-Series Half-Bridge LLC Resonant Converter Design Handbook

This article introduces the design of a half-bridge LLC resonant converter using FSFR-Series Fairchild Power Switch (FPS™). Resonant switching techniques are used to reduce switching losses and enable high-frequency operation, leading to a significant reduction in noise.


Fairchild Semiconductor FSFR-Series Half-Bridge LLC Resonant Converter Design Handbook - cover page
Brand
Fairchild
Category
Other Electronics
Document type
Application Note
Language
English
Pages
17
File format
PDF
File size
1.1 MB
Published
01 August, 2012
Updated
28 September, 2023
MD5 checksum
5B09F679CEE44CCA4B58E5D4312AB523

About this manual

This document is an application note (AN-4151) from Fairchild Semiconductor Corporation that details the design of a half-bridge LLC resonant converter. It focuses on the FSFR-Series Fairchild Power Switch (FPS) as the primary switching component.

The text explains the operating principles of the LLC resonant converter, including the fundamental approximation, the role of the magnetizing inductance, and the rectifier network. It discusses the advantages of the topology, such as zero voltage switching (ZVS) and reduced switching losses at high frequencies. The document also covers the derivation of the voltage gain and equivalent load resistance.

What's inside

  • Introduction
  • LLC Resonant Converter and Fundamental Approximation
  • Square wave generator
  • Resonant network
  • Rectifier network
  • Equivalent Load Resistance
  • AC Equivalent Circuit
  • Voltage Gain Characteristics
  • Design Considerations

Frequently asked questions

What is the primary advantage of using an LLC resonant converter over a series resonant converter?

It can regulate the output voltage over wide line and load variations with only a relatively small variation in switching frequency.

How does an LLC resonant converter achieve zero voltage switching for its MOSFETs?

The current flowing through the anti-parallel diode ensures that the voltage across the MOSFET is zero when it turns on.

What happens to the peak gain frequency as the load increases?

The peak gain frequency moves toward the series resonant frequency (f_s), and the maximum achievable peak gain drops.

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