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In reference to the batch mode, similar results were obtained with the bundle flow cell.
A cubic non-linear k ε model was used to simulate the typical rod bundle flow effects, such as secondary flow and non-isotropic turbulence.
Thereby the pin bundle flow is regarded as a porous medium flow that is characterized by a certain coolant volume fraction and an associated wet area.
In this paper a macroscopic continuum differential model of pin bundle flow is proposed and developed for computational fluid dynamics (CFD) simulations of a reactor core.
As an application of our results, we will give a complete classification of minimal sets for the projective bundle flow of an almost periodic, sl(2,R -valued, continuous or discrete cocycle.
This paper describes major improvements to the computational infrastructure of the CTF subchannel code so that full-core, pincell-resolved (i.e., one computational subchannel per real bundle flow channel) simulations can now be performed in much shorter run-times, either in stand-alone mode or as part of coupled-code multi-physics calculations.
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This paper presents results from an ongoing effort in determining the conditions favorable for occurrence of HTD in the supercritical bundle flows.
The bundle-flow velocity was ∼1.5 m/s and Reynolds number was ∼42,000.
In this paper, the effects of Siemens Memcor Memjet® hollow fibre membrane bundle on flow field were transferred to a porous media model.
Remaining practice bundles create flow of material and information (principle no. 3).
This research paves a way for studying the fatigue strength of planar elastic tube bundle by flow-induced vibration.
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