A Computational Information Criterion for Particle-Tracking with Sparse or Noisy Data

被引:2
|
作者
Tran, Nhat Thanh, V [1 ]
Benson, David A. [2 ]
Schmidt, Michael J. [3 ]
Pankavich, Stephen D. [4 ]
机构
[1] Univ Calif Irvine, Dept Math, Irvine, CA 92697 USA
[2] Colorado Sch Mines, Dept Geol & Geol Engn, Hydrol Sci & Engn Program, Golden, CO 80401 USA
[3] Sandia Natl Labs, Ctr Comp Res, Albuquerque, NM 87185 USA
[4] Colorado Sch Mines, Dept Appl Math & Stat, Golden, CO 80401 USA
关键词
Computational Information Criterion; Lagrangian Modeling; Particle Methods; Diffusion-reaction Equation; Non-Gaussian Error Distribution; LAGRANGIAN SIMULATION; MODELS;
D O I
10.1016/j.advwatres.2021.103893
中图分类号
TV21 [水资源调查与水利规划];
学科分类号
081501 ;
摘要
Traditional probabilistic methods for the simulation of advection-diffusion equations (ADEs) often overlook the entropic contribution of the discretization, e.g., the number of particles, within associated numerical methods. Many times, the gain in accuracy of a highly discretized numerical model is outweighed by its associated computational costs or the noise within the data. We address the question of how many particles are needed in a simulation to best approximate and estimate parameters in one-dimensional advective-diffusive transport. To do so, we use the well-known Akaike Information Criterion (AIC) and a recently-developed correction called the Computational Information Criterion (COMIC) to guide the model selection process. Random-walk and mass transfer particle tracking methods are employed to solve the model equations at various levels of discretization. Numerical results demonstrate that the COMIC provides an optimal number of particles that can describe a more efficient model in terms of parameter estimation and model prediction compared to the model selected by the AIC even when the data is sparse or noisy, the sampling volume is not uniform throughout the physical domain, or the error distribution of the data is non-IID Gaussian.
引用
收藏
页数:8
相关论文
共 50 条
  • [21] Microscale, scanning defocusing volumetric particle-tracking velocimetry
    Guo, Tianqi
    Ardekani, Arezoo M.
    Vlachos, Pavlos P.
    EXPERIMENTS IN FLUIDS, 2019, 60 (06)
  • [22] Phagocytosis of Dictyostelium discoideum studied by the particle-tracking method
    Ishikawa, J
    Okano, J
    Ohki, K
    Amagai, A
    Maeda, Y
    Miyata, H
    EXPERIMENTAL CELL RESEARCH, 2003, 288 (02) : 268 - 276
  • [23] Particle-Tracking Microrheology of Living Cells: Principles and Applications
    Wirtz, Denis
    ANNUAL REVIEW OF BIOPHYSICS, 2009, 38 : 301 - 326
  • [24] Iterative particle matching for three-dimensional particle-tracking velocimetry
    A. Rubbert
    W. Schröder
    Experiments in Fluids, 2020, 61
  • [25] Microscale, scanning defocusing volumetric particle-tracking velocimetry
    Tianqi Guo
    Arezoo M. Ardekani
    Pavlos P. Vlachos
    Experiments in Fluids, 2019, 60
  • [26] A particle-tracking approach to simulating transport in a complex fracture
    Tsang, CF
    Doughty, C
    WATER RESOURCES RESEARCH, 2003, 39 (07)
  • [27] Nonparametric, data-based kernel interpolation for particle-tracking simulations and kernel density estimation
    Benson, David A.
    Bolster, Diogo
    Pankavich, Stephen
    Schmidt, Michael J.
    ADVANCES IN WATER RESOURCES, 2021, 152
  • [28] Determination of Nanoparticle Size Using a Flow Particle-Tracking Method
    Matsuura, Yusuke
    Nakamura, Ayako
    Kato, Haruhisa
    ANALYTICAL CHEMISTRY, 2018, 90 (06) : 4182 - 4187
  • [29] Particle-tracking method applied to transport problems in water bodies
    Mascarenhas, F. C. B.
    Trento, A. E.
    MANAGEMENT OF NATURAL RESOURCES, SUSTAINABLE DEVELOPMENT AND ECOLOGICAL HAZARDS, 2007, 99 : 503 - 513
  • [30] Combining particle-tracking and geochemical data to assess public supply well vulnerability to arsenic and uranium
    Hinkle, Stephen R.
    Kauffman, Leon J.
    Thomas, Mary Ann
    Brown, Craig J.
    McCarthy, Kathy A.
    Eberts, Sandra M.
    Rosen, Michael R.
    Katz, Brian G.
    JOURNAL OF HYDROLOGY, 2009, 376 (1-2) : 132 - 142