Fig. 8
Temperature distributions for the bidirectional heat flow geometry consisting of transparent substrate/100 nm Al/polymer where laser irradiation occurs at the Al surface adjacent to the transparent substrate. For the case of this transparent substrate being (a) Al2O3 and (b) SiO2, the steady-state (unmodulated) temperature profile is displayed as a contour in radius and depth, while the solid line is the magnitude of modulated temperature at r = 0 μm for a modulation frequency of 10 MHz. In both cases, positive depth depicts the Al/polymer side, while negative depth depicts the transparent substrate side. (c) depicts the steady-state surface temperature rise for the same bidirectional heat flow geometry where the transparent substrate is varied to span a wide range of thermal conductivities from Si (140 W m−1 K−1) to complete insulation. All thermal parameters used for these calculations are listed in Table 1.

Temperature distributions for the bidirectional heat flow geometry consisting of transparent substrate/100 nm Al/polymer where laser irradiation occurs at the Al surface adjacent to the transparent substrate. For the case of this transparent substrate being (a) Al2O3 and (b) SiO2, the steady-state (unmodulated) temperature profile is displayed as a contour in radius and depth, while the solid line is the magnitude of modulated temperature at r = 0 μm for a modulation frequency of 10 MHz. In both cases, positive depth depicts the Al/polymer side, while negative depth depicts the transparent substrate side. (c) depicts the steady-state surface temperature rise for the same bidirectional heat flow geometry where the transparent substrate is varied to span a wide range of thermal conductivities from Si (140 W m−1 K−1) to complete insulation. All thermal parameters used for these calculations are listed in Table 1.

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