ZHCSHO1D November   2018  – January 2019 LMG1210

PRODUCTION DATA.  

  1. 特性
  2. 应用
  3. 说明
    1.     Device Images
      1.      简化的典型应用
  4. 修订历史记录
  5. Pin Configuration and Functions
    1.     Pin Functions
  6. Specifications
    1. 6.1 Absolute Maximum Ratings
    2. 6.2 ESD Ratings
    3. 6.3 Recommended Operating Conditions
    4. 6.4 Thermal Information
    5. 6.5 Electrical Characteristics
    6. 6.6 Switching Characteristics
    7. 6.7 Typical Characteristics
    8. 6.8 Timing Diagrams
  7. Detailed Description
    1. 7.1 Overview
    2. 7.2 Functional Block Diagram
    3. 7.3 Feature Description
      1. 7.3.1 Bootstrap Diode Operation
      2. 7.3.2 LDO Operation
      3. 7.3.3 Dead Time Selection
      4. 7.3.4 Overtemperature Protection
      5. 7.3.5 High-Performance Level Shifter
      6. 7.3.6 Negative HS Voltage Handling
    4. 7.4 Device Functional Modes
  8. Application and Implementation
    1. 8.1 Application Information
    2. 8.2 Typical Application
      1. 8.2.1 Design Requirements
      2. 8.2.2 Detailed Design Procedure
        1. 8.2.2.1 Bypass Capacitor
        2. 8.2.2.2 Bootstrap Diode Selection
        3. 8.2.2.3 Handling Ground Bounce
        4. 8.2.2.4 Independent Input Mode
        5. 8.2.2.5 Computing Power Dissipation
      3. 8.2.3 Application Curves
    3. 8.3 Do's and Don'ts
  9. Power Supply Recommendations
  10. 10Layout
    1. 10.1 Layout Guidelines
    2. 10.2 Layout Example
  11. 11器件和文档支持
    1. 11.1 文档支持
      1. 11.1.1 相关文档
    2. 11.2 接收文档更新通知
    3. 11.3 社区资源
    4. 11.4 商标
    5. 11.5 静电放电警告
    6. 11.6 术语表
  12. 12机械、封装和可订购信息

Bootstrap Diode Operation

An internal low impedance switch enables the bootstrap only when the low-side GaN FET is on. If used in a converter where the low-side FET operates in third quadrant conduction during the dead times, this provides two main benefits. First, it stops the bootstrap diode from overcharging the high-side bootstrap rail. Second, if using a p-n junction diode with Qrr as the bootstrap diode, it decreases the Qrr losses of the diode. There is a 1 kΩ resistor connected between the drain and source of this internal bootstrap switch to allow the bootstrap capacitor to slowly charge at start-up before the low-side FET is turned on.

The part does not have an actual clamp on the high-side bootstrap supply. The bootstrap switch disables conduction during the dead times, and the actual bootstrap capacitor voltage is set by the operating conditions of the circuit during the low-side on-time. The bootstrap voltage can be approximately calculated in Equation 1 through Equation 3.

The bootstrap voltage is given by Equation 1:

Equation 1. VBST = VDD – VF – VHS

where

  • VF is the forward voltage drop of the bootstrap diode and series bootstrap switch.

VHS is calculated in Equation 2:

Equation 2. VHS = –IL × RDSON

where

  • IL is the inductor current defined as flowing out of the half-bridge
  • and RDSON is the FET on resistance.

Substituting (2) into (1) gives the expression for the bootstrap voltage as Equation 3:

Equation 3. VBST = VDD – VF + IL × RDSON

From (3) one can determine that in an application where the current flows out of the half-bridge (IL is positive) the bootstrap voltage can be charged up to a voltage higher than VDD if IL × RDSON is greater than VF. Take care not to overcharge the bootstrap too much in this application by choosing a diode with a larger VF or limiting the IL × RDSON product.

In an application where IL is negative, the IL × RDSON product subtracts from the available bootstrap cap voltage. In this case using a smaller VF diode is recommended if IL × RDSON is large.