SUBJECT: M.S. Thesis Presentation
   
BY: Keith Suda-Cederquist
   
TIME: Monday, March 12, 2007, 9:00 a.m.
   
PLACE: Love Building, 109
   
TITLE: Near-Wall Thermometry via Total Internal Reflection Fluorescent Micro-Thermometry (TIR-FMT)
   
COMMITTEE: Dr. Minami Yoda, Chair (ME)
Dr. Yogendra Joshi (ME)
Dr. Zhuomin Zhang (ME)
 

SUMMARY

To effectively design systems of microchannels it is necessary for scientists and engineers to understand thermal transport characteristics of microchannels, specifically the local convective heat transfer coefficient. Analytical solutions are not available due to the spatially and temporally varying heat fluxes typically generated by microelectronics. To experimentally determine the convective heat transfer coefficient of microchannels it is necessary to measure both the bulk and surface temperature fields. This investigation aims to develop a technique, named Total Internal Reflection Fluorescent Micro-Thermometry (TIR-FMT), to measure the temperature of water within several hundred nanometers of a wall--effectively, the surface temperature of the wall. In TIR-FMT, an evanescent-wave is generated in the water near the wall. The intensity of this evanescent-wave decays exponentially with distance from the wall. A fluorophore if illuminated by the evanescent-wave can absorb a photon. Excited fluorophores subsequently emit red-shifted photons, which are called fluorescence. The probability of a fluorescent emission is temperature-dependent. Therefore, by monitoring the intensity of the fluorescence a correlation can be made to the temperature of the region of illumination. Using the TIR-FMT technique the temperature dependence of the fluorescence intensity from buffered fluorescein (pH=9.2) was determined to be 1.35%/°C. TIR-FMT can be used to measure the temperature of a fluorophore solution within 600 nm of a wall across a temperature range of 12.5-55°C. The rms uncertainties (95% confidence) of the temperature measured was determined to be 2.4°C and 1.5°C for a single 1.5x1.5 μm pixel and the entire 715x950 μm viewfield. By spatial averaging, rms uncertainties of 2.0°C and 1.8°C were attained with spatial resolutions of 16x16 and 100x100 μm, respectively.