2009
DOI: 10.1016/j.ijheatmasstransfer.2009.03.048
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Immersed boundary method for the simulation of flows with heat transfer

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Cited by 93 publications
(53 citation statements)
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References 29 publications
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“…13 In the IB-LBM proposed by Suzuki and Inamuro, the distribution function f k and velocity field u are updated only once in steps 11 and 12 after the iterative process between steps 5 and 9.…”
Section: Computeũmentioning
confidence: 99%
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“…13 In the IB-LBM proposed by Suzuki and Inamuro, the distribution function f k and velocity field u are updated only once in steps 11 and 12 after the iterative process between steps 5 and 9.…”
Section: Computeũmentioning
confidence: 99%
“…By using the sum of the forceG n for all the iteration times in Equation 23e, the IB-TLBM successfully satisfies the nonslip boundary condition. The maximum number of iterations N m = 20, following Wang et al 13 …”
Section: Computeũmentioning
confidence: 99%
See 1 more Smart Citation
“…Several works exist in the literature regarding extending IBM approaches to solve the energy equation around complex geometries by imposing Dirichlet and Neumann boundary conditions [19][20][21][22][23][24][25][26][27]. Conjugate heat transfer simulations, where the energy equation is also solved inside the immersed body, using IBM were also reported in [28][29][30][31].…”
Section: Introductionmentioning
confidence: 99%
“…Typically the LBM uses a bounceback (BB) method to implement the no-slip BC, which requires a Cartesian grid system. For a circular geometry, the BB scheme requires the use of stair-case type profiles to approximate the curved surface, which can lead to the loss of geometric integrity and numerical inaccuracy [12][13][14]. He and Doolen [15] successfully simulated the 2D vortex shedding behind a circular cylinder in a channel at low Re using an interpolation supplemented lattice Boltzmann equation (ISLBE).…”
Section: Introductionmentioning
confidence: 99%