ZHCSIG0G April   2016  – May 2019 DLP5531-Q1

PRODUCTION DATA.  

  1. 特性
  2. 应用
  3. 说明
    1.     Device Images
      1.      DLP5531-Q1 DLP芯片组系统方框图
  4. 修订历史记录
  5. Pin Configuration and Functions
    1.     Pin Functions – Connector Pins
    2.     Pin Functions – Test Pads
  6. Specifications
    1. 6.1  Absolute Maximum Ratings
    2. 6.2  Storage Conditions
    3. 6.3  ESD Ratings
    4. 6.4  Recommended Operating Conditions
    5. 6.5  Thermal Information
    6. 6.6  Electrical Characteristics
    7. 6.7  Timing Requirements
    8. 6.8  Switching Characteristics
    9. 6.9  System Mounting Interface Loads
    10. 6.10 Physical Characteristics of the Micromirror Array
    11. 6.11 Micromirror Array Optical Characteristics
    12. 6.12 Window Characteristics
    13. 6.13 Chipset Component Usage Specification
  7. Detailed Description
    1. 7.1 Overview
    2. 7.2 Functional Block Diagram
    3. 7.3 Feature Description
      1. 7.3.1 Sub-LVDS Data Interface
      2. 7.3.2 Low Speed Interface for Control
      3. 7.3.3 DMD Voltage Supplies
      4. 7.3.4 Asynchronous Reset
      5. 7.3.5 Temperature Sensing Diode
        1. 7.3.5.1 Temperature Sense Diode Theory
    4. 7.4 System Optical Considerations
      1. 7.4.1 Numerical Aperture and Stray Light Control
      2. 7.4.2 Pupil Match
      3. 7.4.3 Illumination Overfill
    5. 7.5 DMD Image Performance Specification
    6. 7.6 Micromirror Array Temperature Calculation
      1. 7.6.1 Temperature Rise Through the Package for Heatsink Design
      2. 7.6.2 Monitoring Array Temperature Using the Temperature Sense Diode
    7. 7.7 Micromirror Landed-On/Landed-Off Duty Cycle
      1. 7.7.1 Definition of Micromirror Landed-On/Landed-Off Duty Cycle
  8. Application and Implementation
    1. 8.1 Application Information
    2. 8.2 Typical Application
      1. 8.2.1 Application Overview
      2. 8.2.2 Reference Design
      3. 8.2.3 Application Mission Profile Consideration
  9. Power Supply Recommendations
    1. 9.1 Power Supply Power-Up Procedure
    2. 9.2 Power Supply Power-Down Procedure
    3. 9.3 Power Supply Sequencing Requirements
  10. 10Layout
    1. 10.1 Layout Guidelines
  11. 11器件和文档支持
    1. 11.1 器件支持
      1. 11.1.1 器件命名规则
      2. 11.1.2 器件标记
    2. 11.2 相关链接
    3. 11.3 社区资源
    4. 11.4 商标
    5. 11.5 静电放电警告
    6. 11.6 DMD 处理
    7. 11.7 Glossary
  12. 12机械、封装和可订购信息

封装选项

请参考 PDF 数据表获取器件具体的封装图。

机械数据 (封装 | 引脚)
  • FYK|149
散热焊盘机械数据 (封装 | 引脚)
订购信息

Temperature Rise Through the Package for Heatsink Design

When designing the DMD heatsink solution, the package thermal resistance from array to reference ceramic temperature (thermocouple location TP1 in Figure 19)  can be used to determine the temperature rise through the package as given by the following equations:

Equation 1. TARRAY-TO-CERAMIC = QARRAY × RARRAY–TO–CERAMIC
Equation 2. QILLUMINATION = (QINCIDENT × DMD Absorption Constant)
Equation 3. QARRAY = QELECTRICAL + QILLUMINATION

where

  • TARRAY-TO-CERAMIC = temperature rise from array to thermal test point TP1 (°C/W)
  • TCERAMIC = measured ceramic temperature, at the TP1 location in Figure 19 (°C)
  • RARRAY–TO–CERAMIC = DMD package thermal resistance from array to thermal test point TP1 (°C/W)
    See Thermal Information
  • QARRAY = total power, electrical plus absorbed, on the DMD array (W)
  • QELECTRICAL = nominal electrical power dissipation by the DMD (W)
  • QILLUMINATION = absorbed illumination heat load (W)
  • QINCIDENT = incident power on the DMD (W)

The DMD package thermal resistance from array to ceramic (RARRAY–TO–CERAMIC) assumes a non-uniform illumination distribution on the DMD as shown in Figure 20. For illumination profiles more uniform than the one highlighted in Figure 20, the value provided here is valid.  However, for more non-uniform profiles (e.g. Gaussian distribution) the thermal resistance will be higher. Please contact TI to determine an accurate value for this case.

DLP5531-Q1 non_uniform_illum_profile.gifFigure 20. Non-Uniform Illumination Profile

The DMD absorption constant is a function of illumination distribution on the active array and the array border, angle of incidence (AOI), f number of the system, and operating state of the mirrors. The absorption constant is higher in the OFF state than in the ON state. Equations to calculate the absorption constant are provided for both ON and OFF mirror states. They assume an AOI of 34 degrees, an f/1.7 system, and they account for the distribution of light on the active array, POM, and array border.

Equation 4. DMD Absorption Constant (OFF state) = 0.895 – 0.004783 × (% of light on ActiveArray + POM)
Equation 5. DMD Absorption Constant (ON state) = 0.895 – 0.007208 × (% of light on ActiveArray + POM)

Electrical power dissipation of the DMD is variable and depends on the voltages, data rates, and operating frequencies.

The following sample calculations assume 10% of the total incident light falls outside of the active array and POM, and the mirrors are in the OFF state.

  1. DMD Absorption Constant = 0.895 – 0.004783 × 90 = 0.46
  2. QELECTRICAL = 0.4 W
  3. RARRAY–TO–CERAMIC = 1.3°C/W
  4. QINCIDENT = 10 W
  5. QARRAY = 0.4 W + (0.46 × 10 W) = 5 W
  6. TARRAY-TO-CERAMIC = 5 W × 1.3°C/W = 6.5°C