tailieunhanh - Heat Conduction Basic Research Part 9

Tham khảo tài liệu 'heat conduction basic research part 9', kỹ thuật - công nghệ, cơ khí - chế tạo máy phục vụ nhu cầu học tập, nghiên cứu và làm việc hiệu quả | Time Varying Heat Conduction in Solids 189 Modulation Frequency Hz a b Fig. 2. a Normalized signal amplitude as a function of f. Circles experimental points. Solid curve and b Result of theoretical simulation using Eq. 37 . Reproduced from Central Eur. J. Phys 2010 8 4 634-638 . approach could be helpful not only in the field of PA and PT techniques but it can be also used for the analysis of the phenomenon of heat transfer in the presence of modulated heat sources in multilayer structures which appear frequently in men s made devices for example semiconductor heterostructures lasers and LEDs driven by pulsed periodical electrical current sources . A finite sample exposed to a finite duration heat pulse Considering a semi-infinite homogeneous medium exposed to a sudden temperature change at its surface at x 0 from To to Tp For the calculation of the temperature field created by a heat pulse at t 0 one has to solve the homogeneous heat diffusion equation 19 with the boundary conditions T x 0 t 0 T1 T x 0 t 0 To. 38 The solution for t 0 is Carlslaw Jaeger 1959 T x Í n To - Tf erf 39 where erf is the error function. Using Fourier s law Ec. 9 one may obtain from the above equation for the heat flow s T -T q z ế 4ĩìi exp rf 40 This expression describes a Gaussian spread of thermal energy with characteristic width 2fat 41 This characteristic distance is the thermal diffusion length for pulsed excitation and has a similar meaning as the thermal diffusion length defined by Eq. 23 . 190 Heat Conduction - Basic Research If Eq. 40 is scaled to three dimensions one can show that after a time t has elapsed the heat outspread over a sphere of radius . Suppose that a spherical particle of radius R is heated in the form described above by a heat pulse at its surface. The particle requires for cooling a time similar to that the necessary for the heat to diffuse throughout its volume. The heat flux at the opposite surface of the particle could be expressed as q r 2fl qoexp -

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