4.7 Article

Numerical investigation of a high pressure hydrogen jet of 82 MPa with adaptive mesh refinement: Concentration and velocity distributions

Journal

INTERNATIONAL JOURNAL OF HYDROGEN ENERGY
Volume 43, Issue 18, Pages 9094-9109

Publisher

PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.ijhydene.2018.03.089

Keywords

Underexpanded free jet; Hydrogen concentration; Adaptive mesh refinement; Numerical simulation; Turbulent oscillation

Funding

  1. NASA/AISR project [NNG04GP79G]
  2. Department of Energy
  3. Advanced Simulation and Computing Program

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To investigate the safety properties of high-pressure hydrogen discharge or leakage, an under-expanded hydrogen jet flow with a storage pressure of 82 MPa from a small jet orifice with a diameter of 0.2 mm is studied by three-dimensional (3D) numerical calculations. The full 3D compressible Navier-Stokes equations are utilized in a domain with a size of about 3 x 3 x 6 m which is discretized by employing an adaptive mesh refinement (AMR) technology to reduce the number of grid cells. By AMR, the local mesh resolutions can narrowly cover the Taylor microscale l(T) and direct numerical simulations (DNS) are performed. Both the instantaneous and mean hydrogen concentration distributions in the present jet are discussed. The instantaneous concentrations of hydrogen <(C)over-bar>(H2) on the axis presents significant turbulent pulsating oscillations. The centerline value of the intensity of concentration fluctuation <(sigma)over-cap>H-2 asymptotically comes to 0.23, which is in a good agreement with the existing experimental results. It substantiates the conclusion that the asymptotic centerline value of <(sigma)over-cap>H-2 is independent of jet density ratio. The probability distributions function (PDF) of instantaneous axial <(C)over-bar>(H2) agree approximately with the Gaussian distribution while skewing a little to the higher range. The time averaged hydrogen concentration <(C)over-bar>(H2) along the radial directions can also be described as a Gaussian distribution. The axial <(C)over-bar>(H2) of 82 MPa hydrogen jet tends to obey the distribution discipline approximated with <(C)over-bar>(2) = 4200/(z theta 0) where z is the axial distance from the nozzle and theta 0 is the effective ejection diameter, which is consistent with the experimental results. In addition, the hydrogen tip penetration (tip) is found to be in a linear relationship with the square root of jet flow time root/t. Meanwhile, the jet's velocity half-width L-Vh approximately gains an linear (C) 2018 Hydrogen Energy Publications LLC. Published by Elsevier Ltd. All rights reserved.

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