ZHCSE69E November 2014 – May 2025 DLP9500UV
PRODUCTION DATA
Active array temperature cannot be measured directly; therefore, it must be computed analytically from measurement points on the outside of the package, package thermal resistance, electrical power, and illumination heat load. The relationship between array temperature and the reference ceramic temperature (test point number 1 in Figure 7-11) is provided by the following equations:
TArray = Measured Ceramic temperature at location (test point number 3) + (Temperature increase due to power incident to the array × array-to-ceramic resistance)
= TCeramic+ (QArray × RArray-To-Ceramic)
where
where
The electrical power dissipation of the DMD is variable and depends on the voltages, data rates, and operating frequencies. The nominal electrical power dissipation of the DMD is variable and depends on the operating state of the mirrors and the intensity of the light source. The DMD absorption constant of 0.42 assumes nominal operation with an illumination distribution of 83.7% on the active array, 11.9% on the array border, and 4.4% on the window aperture. A system aperture may be required to limit the power incident on the package aperture since this area absorbs much more efficiently than the array.