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Fig. 5 Geometry of the heat pipe problem.
For the non-isothermal benchmark, we simulated the heat pipe problem and verified our result against the semi-analytical solution ('Benchmark II: heat pipe problem' section).
Furthermore, our numerical model extended the original heat pipe problem to include the phase change behavior.
Fig. 5 Geometry of the heat pipe problem q w ·ν=q h ·ν=0 on Γ imp.
Therefore, we compared our simulation result of the classical heat pipe problem to the semi-analytical solution from Udell and Fitch (1985).
In Benchmark I ('Benchmark I: isothermal injection of H 2 gas' section), we choose gamma(S =0 In Benchmark II ('Benchmark II: heat pipe problem' section), we choose gamma(S =S^{2} When one phase disappears, its volume converges to zero, making the P value equal to the pressure of the remaining phase.
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The second one models the non-isothermal multiphase flow of heat-pipe problem.
This type of heat pipe adsorber solves the problem of incompatibility between ammonia, copper, seawater and steel.
Optimization problem of the heat pipe is formed considering minimization of the thermal resistance and total mass of heat pipe and solved using the heat transfer search algorithm.
In the case of the classical problem of a cylindrical heat pipe heated on one side and cooled on the other side, the simplification of the general solution enables to establish the well-known theory of heat pipe modeling, which validates the approach.
To overcome this problem, a storage tank may be coupled to the loop heat pipe.
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