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Energies 2022, 15, x FOR PEER REVIEW 8 of 15 Energies 2022, 15, x FOR PEER REVIEW 8 of 15 Energies 2022, 15, 6347 channel, reflecting that the flow temperature distribution in the channel depends on its channel, reflecting that the flow temperature distribution in the channel depends on its velocity distribution. 8 of 15 velocity distribution. Figure 4. Velocity distribution of different cross-sections along the flow direction. Figure 4. Velocity distribution of different cross-sections along the flow direction. Figure 4. Velocity distribution of different cross-sections along the flow direction. Figure 5. Temperature distribution of different cross-sections along the flow direction. Figure 5. Temperature distribution of different cross-sections along the flow direction. Figure 5. Temperature distribution of different cross-sections along the flow direction. It is well known that a regular associated movement named secondary flow can be It is well known that a regular associated movement named secondary flow can be genIteriastewdewllhkenothwenvitshcoautsaflrueigdumlaorveassaolocniagtaedwamvyovcheamnenneltantamfixeeddsmecaoinfldoawryvfellowcityc.an be generated when the viscous fluid moves along a wavy channel at a fixed main flow veloc- The secondary flow in the wavy channel is mainly named the Dean vortex, which is a pair generated when the viscous fluid moves along a wavy channel at a fixed main flow veloc- ity. The secondary flow in the wavy channel is mainly named the Dean vortex, which is a of antisymmetric vortices generated due to the centrifugal force when incompressible fluid ity. The secondary flow in the wavy channel is mainly named the Dean vortex, which is a pair of antisymmetric vortices generated due to the centrifugal force when incompressible flows in the wavy channel. The Dean vortex can significantly promote the heat transfer pair of antisymmetric vortices generated due to the centrifugal force when incompressible fludiduefltowthseincotnhveewctiaovnyacnhdasnhneearl.fTuhncetDioneain vthoerflteuxidcaflnowsig[2n9i]f.icInanatdlydiptiroonm, tohetestehcoenhdeartytrans- fluid flows in the wavy channel. The Dean vortex can significantly promote the heat trans- flow at different cross-sections is distributed similarly at the same incline angle, leading to fer due to the convection and shear function in the fluid flow [29]. In addition, the second- fer due to the convection and shear function in the fluid flow [29]. In addition, the second- a similar distribution of the accelerating core. ary flow at different cross-sections is distributed similarly at the same incline angle, lead- ary flow at different cross-sections is distributed similarly at the same incline angle, lead- Figure 6 shows the secondary flow of different cross-sections. It can be seen that the ing to a similar distribution of the accelerating core. ing to a similar distribution of the accelerating core. Dean vortex appeared in several cross-sections except for the inlet cross-sections of the Figure 6 shows the secondary flow of different cross-sections. It can be seen that the colFdiganudreh6otsflhuoiwds. tThheesdeicsotrnibduatriyonfsloowf thoef Ddiefafenrvenorttecrxoastsd-sieffcetrieontsi.nIctlicnaenabneglseesewnetrheat the Dean vortex appeared in several cross-sections except for the inlet cross-sections of the cold Dean vortex appeared in several cross-sections except for the inlet cross-sections of the cold and hot fluids. The distributions of the Dean vortex at different incline angles were different. and hot fluids. The distributions of the Dean vortex at different incline angles were different.PDF Image | Thermal–Hydraulic Performance of a Printed Circuit Heat Exchanger
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