851 research outputs found

    Machine Learning and Artificial Intelligence-Driven Multi-Scale Modeling for High Burnup Accident-Tolerant Fuels for Light Water-Based SMR Applications

    Full text link
    The concept of small modular reactor has changed the outlook for tackling future energy crises. This new reactor technology is very promising considering its lower investment requirements, modularity, design simplicity, and enhanced safety features. The application of artificial intelligence-driven multi-scale modeling (neutronics, thermal hydraulics, fuel performance, etc.) incorporating Digital Twin and associated uncertainties in the research of small modular reactors is a recent concept. In this work, a comprehensive study is conducted on the multiscale modeling of accident-tolerant fuels. The application of these fuels in the light water-based small modular reactors is explored. This chapter also focuses on the application of machine learning and artificial intelligence in the design optimization, control, and monitoring of small modular reactors. Finally, a brief assessment of the research gap on the application of artificial intelligence to the development of high burnup composite accident-tolerant fuels is provided. Necessary actions to fulfill these gaps are also discussed

    Non-Intrusive Uncertainty Quantification for U3Si2 and UO2 Fuels with SiC/SiC Cladding using BISON for Digital Twin-Enabling Technology

    Full text link
    U.S. Nuclear Regulatory Committee (NRC) and U.S. Department of Energy (DOE) initiated a future-focused research project to assess the regulatory viability of machine learning (ML) and artificial intelligence (AI)-driven Digital Twins (DTs) for nuclear applications. Advanced accident tolerant fuel (ATF) is one of the priority focus areas of the DOE/ NRC. DTs have the potential to transform the nuclear energy sector in the coming years by incorporating risk-informed decision-making into the Accelerated Fuel Qualification (AFQ) process for ATF. A DT framework can offer game-changing yet practical and informed solutions to the complex problem of qualifying advanced ATFs. However, novel ATF technology suffers from a couple of challenges, such as (i) Data unavailability; (ii) Lack of data, missing data; and (iii) Model uncertainty. These challenges must be resolved to gain the trust in DT framework development. In addition, DT-enabling technologies consist of three major areas: (i) modeling and simulation (M&S), covering uncertainty quantification (UQ), sensitivity analysis (SA), data analytics through ML/AI, physics-based models, and data-informed modeling, (ii) Advanced sensors/instrumentation, and (iii) Data management. UQ and SA are important segments of DT-enabling technologies to ensure trustworthiness, which need to be implemented to meet the DT requirement. Considering the regulatory standpoint of the modeling and simulation (M&S) aspect of DT, UQ and SA are paramount to the success of DT framework in terms of multi-criteria and risk-informed decision-making. In this study, the adaptability of polynomial chaos expansion (PCE) based UQ/SA in a non-intrusive method in BISON was investigated to ensure M&S aspects of the AFQ for ATF. This study introduces the ML-based UQ and SA methods while exhibiting actual applications to the finite element-based nuclear fuel performance code

    Stochastic process design kits for photonic circuits based on polynomial chaos augmented macro-modelling

    Get PDF
    Fabrication tolerances can significantly degrade the performance of fabricated photonic circuits and process yield. It is essential to include these stochastic uncertainties in the design phase in order to predict the statistical behaviour of a device before the final fabrication. This paper presents a method to build a novel class of stochastic-based building blocks for the preparation of Process Design Kits for the analysis and design of photonic circuits. The proposed design kits directly store the information on the stochastic behaviour of each building block in the form of a generalized-polynomial-chaos-based augmented macro-model obtained by properly exploiting stochastic collocation and Galerkin methods. Using these macro-models, only a single deterministic simulation is required to compute the stochastic moments of any arbitrary photonic circuit, without the need of running a large number of time-consuming circuit simulations thereby dramatically improving simulation efficiency. The effectiveness of the proposed approach is verified by means of classical photonic circuit examples with multiple uncertain variables

    Iterative learning control of crystallisation systems

    Get PDF
    Under the increasing pressure of issues like reducing the time to market, managing lower production costs, and improving the flexibility of operation, batch process industries thrive towards the production of high value added commodity, i.e. specialty chemicals, pharmaceuticals, agricultural, and biotechnology enabled products. For better design, consistent operation and improved control of batch chemical processes one cannot ignore the sensing and computational blessings provided by modern sensors, computers, algorithms, and software. In addition, there is a growing demand for modelling and control tools based on process operating data. This study is focused on developing process operation data-based iterative learning control (ILC) strategies for batch processes, more specifically for batch crystallisation systems. In order to proceed, the research took a step backward to explore the existing control strategies, fundamentals, mechanisms, and various process analytical technology (PAT) tools used in batch crystallisation control. From the basics of the background study, an operating data-driven ILC approach was developed to improve the product quality from batch-to-batch. The concept of ILC is to exploit the repetitive nature of batch processes to automate recipe updating using process knowledge obtained from previous runs. The methodology stated here was based on the linear time varying (LTV) perturbation model in an ILC framework to provide a convergent batch-to-batch improvement of the process performance indicator. In an attempt to create uniqueness in the research, a novel hierarchical ILC (HILC) scheme was proposed for the systematic design of the supersaturation control (SSC) of a seeded batch cooling crystalliser. This model free control approach is implemented in a hierarchical structure by assigning data-driven supersaturation controller on the upper level and a simple temperature controller in the lower level. In order to familiarise with other data based control of crystallisation processes, the study rehearsed the existing direct nucleation control (DNC) approach. However, this part was more committed to perform a detailed strategic investigation of different possible structures of DNC and to compare the results with that of a first principle model based optimisation for the very first time. The DNC results in fact outperformed the model based optimisation approach and established an ultimate guideline to select the preferable DNC structure. Batch chemical processes are distributed as well as nonlinear in nature which need to be operated over a wide range of operating conditions and often near the boundary of the admissible region. As the linear lumped model predictive controllers (MPCs) often subject to severe performance limitations, there is a growing demand of simple data driven nonlinear control strategy to control batch crystallisers that will consider the spatio-temporal aspects. In this study, an operating data-driven polynomial chaos expansion (PCE) based nonlinear surrogate modelling and optimisation strategy was presented for batch crystallisation processes. Model validation and optimisation results confirmed this approach as a promise to nonlinear control. The evaluations of the proposed data based methodologies were carried out by simulation case studies, laboratory experiments and industrial pilot plant experiments. For all the simulation case studies a detailed mathematical models covering reaction kinetics and heat mass balances were developed for a batch cooling crystallisation system of Paracetamol in water. Based on these models, rigorous simulation programs were developed in MATLABยฎ, which was then treated as the real batch cooling crystallisation system. The laboratory experimental works were carried out using a lab scale system of Paracetamol and iso-Propyl alcohol (IPA). All the experimental works including the qualitative and quantitative monitoring of the crystallisation experiments and products demonstrated an inclusive application of various in situ process analytical technology (PAT) tools, such as focused beam reflectance measurement (FBRM), UV/Vis spectroscopy and particle vision measurement (PVM) as well. The industrial pilot scale study was carried out in GlaxoSmithKline Bangladesh Limited, Bangladesh, and the system of experiments was Paracetamol and other powdered excipients used to make paracetamol tablets. The methodologies presented in this thesis provide a comprehensive framework for data-based dynamic optimisation and control of crystallisation processes. All the simulation and experimental evaluations of the proposed approaches emphasised the potential of the data-driven techniques to provide considerable advances in the current state-of-the-art in crystallisation control

    ๋ณต์žกํ•œ ๋™ํŠน์„ฑ์„ ๊ฐ–๋Š” ๋‹ค์ƒ ๋ฐ˜์‘๊ธฐ์˜ ์„ค๊ณ„๋ฅผ ์œ„ํ•œ ๊ณ„์‚ฐ ํšจ์œจ์ ์ธ ๋ชจ์‚ฌ ๋ฐ ์ตœ์ ํ™” ์ „๋žต

    Get PDF
    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :๊ณต๊ณผ๋Œ€ํ•™ ํ™”ํ•™์ƒ๋ฌผ๊ณตํ•™๋ถ€,2020. 2. ์ด์ข…๋ฏผ.๋ณธ ๋ฐ•์‚ฌํ•™์œ„๋…ผ๋ฌธ์—์„œ๋Š” ๋ฉ€ํ‹ฐ ์Šค์ผ€์ผ ๋ชจ๋ธ๋ง, ์‹คํ—˜ ๊ฒฐ๊ณผ๋ฅผ ์ด์šฉํ•œ ๋ชจ๋ธ ๋ณด์ •๋ฒ•, ์ตœ์ ํ™” ์ˆœ์œผ๋กœ ์ง„ํ–‰๋˜๋Š” ์‚ฐ์—…์šฉ ํ™”ํ•™ ๋ฐ˜์‘๊ธฐ์˜ ์„ค๊ณ„ ์ „๋žต์„ ์ œ์‹œํ•œ๋‹ค. ๋ฐ˜์‘๊ธฐ๋Š” ํ™”ํ•™ ๊ณต์ •์—์„œ ์ œ์ผ ์ค‘์š”ํ•œ ๋‹จ์œ„์ด์ง€๋งŒ, ๊ทธ ์„ค๊ณ„์— ์žˆ์–ด์„œ๋Š” ์ตœ์‹  ์ˆ˜์น˜์  ๊ธฐ๋ฒ•๋“ค๋ณด๋‹ค๋Š” ์—ฌ์ „ํžˆ ๊ฐ„๋‹จํ•œ ๋ชจ๋ธ์ด๋‚˜ ์‹คํ—˜ ๋ฐ ๊ฒฝํ—˜ ๊ทœ์น™์— ์˜์กดํ•˜๊ณ  ์žˆ๋Š” ํ˜„์‹ค์ด๋‹ค. ์‚ฐ์—… ๊ทœ๋ชจ์˜ ๋ฐ˜์‘๊ธฐ๋Š” ๋ฌผ๋ฆฌ, ํ™”ํ•™์ ์œผ๋กœ ๋ชน์‹œ ๋ณต์žกํ•˜๊ณ , ๊ด€๋ จ ๋ณ€์ˆ˜ ๊ฐ„์˜ ์Šค์ผ€์ผ์ด ํฌ๊ฒŒ ์ฐจ์ด๋‚˜๋Š” ๊ฒฝ์šฐ๊ฐ€ ๋งŽ์•„ ์ˆ˜ํ•™์  ๋ชจ๋ธ๋ง ๋ฐ ์ˆ˜์น˜์  ํ•ด๋ฒ•์„ ๊ตฌํ•˜๊ธฐ๊ฐ€ ์–ด๋ ต๋‹ค. ๋ชจ๋ธ์„ ๋งŒ๋“ค๋”๋ผ๋„ ๋ถ€์ •ํ™•ํ•˜๊ฑฐ๋‚˜ ์‹œ๋ฎฌ๋ ˆ์ด์…˜ ์‹œ๊ฐ„์ด ๋„ˆ๋ฌด ๊ธด ๋ฌธ์ œ๊ฐ€ ์žˆ์–ด ์ตœ์ ํ™” ์•Œ๊ณ ๋ฆฌ์ฆ˜์— ์ ์šฉํ•˜๊ธฐ๊ฐ€ ํž˜๋“ค๋‹ค. ๋ฐ˜์‘๊ธฐ ๋‚ด ํ˜„์ƒ์˜ ๋ณต์žก์„ฑ๊ณผ ์Šค์ผ€์ผ ์ฐจ์ด ๋ฌธ์ œ๋Š” ๋ฉ€ํ‹ฐ ์Šค์ผ€์ผ ๋ชจ๋ธ๋ง์„ ํ†ตํ•ด ์ ‘๊ทผํ•  ์ˆ˜ ์žˆ๋‹ค. ์ „์‚ฐ์œ ์ฒด์—ญํ•™ ๊ธฐ๋ฐ˜ ๊ตฌํš ๋ชจ๋ธ(CFD-based compartmental model)์„ ์ด์šฉํ•˜๋ฉด, ๋ถˆ๊ท ์ผํ•œ ํ˜ผํ•ฉ ํŒจํ„ด์„ ๋ณด์ด๋Š” ๋Œ€ํ˜• ๋ฐ˜์‘๊ธฐ์—์„œ๋„ ๊ธด ์‹œ๊ฐ„ ๋™์•ˆ์˜ ๋™์  ๋ชจ์‚ฌ๊ฐ€ ๊ฐ€๋Šฅํ•˜๋‹ค. ์ด ๋ชจ๋ธ์€ ํฐ ๋ฐ˜์‘๊ธฐ๋ฅผ ์™„๋ฒฝํ•˜๊ฒŒ ๊ท ์ผํ•œ ์ž‘์€ ๊ตฌํš๋“ค์˜ ๋„คํŠธ์›Œํฌ๋กœ ๊ฐ„์ฃผํ•˜๊ณ , ๊ฐ ๊ตฌํš์„ ๋ฐ˜์‘ ์†๋„์‹๋“ค๊ณผ CFD ๊ฒฐ๊ณผ๋กœ๋ถ€ํ„ฐ ๊ฐ€์ ธ์˜จ ์œ ๋™ ์ •๋ณด๊ฐ€ ํฌํ•จ๋œ ์งˆ๋Ÿ‰ ๋ฐ ์—๋„ˆ์ง€ ๊ท ํ˜• ๋ฐฉ์ •์‹์œผ๋กœ ํ‘œํ˜„ํ•œ๋‹ค. ๊ธฐ์ฒด, ์•ก์ฒด, ๊ณ ์ฒด 3์ƒ์ด ์ƒํ˜ธ์ž‘์šฉํ•˜๋ฉฐ ๋ณต์žกํ•œ ์œ ๋™์„ ๋ณด์ด๋Š” ์ˆ˜์„ฑ ๊ด‘๋ฌผ ํƒ„์‚ฐํ™” ๋ฐ˜์‘๊ธฐ๋ฅผ ์ด ๋ฐฉ๋ฒ•์„ ์‚ฌ์šฉํ•ด ๋ชจ๋ธ๋งํ•˜์˜€๋‹ค. ์ด ๋•Œ ๋ชจ๋ธ์€ ๋ฏธ๋ถ„ ๋Œ€์ˆ˜ ๋ฐฉ์ •์‹(DAE)์˜ ํ˜•ํƒœ๋ฅผ ๋ ๋ฉฐ, ๋ฉ”์ปค๋‹ˆ์ฆ˜ ์ƒ ๋ชจ๋“  ๋ฐ˜์‘๋“ค(๊ธฐ-์•ก ๊ฐ„ ๋ฌผ์งˆ ์ „๋‹ฌ ๋ฐ˜์‘, ๊ณ ์ฒด ์šฉํ•ด ๋ฐ˜์‘, ์ด์˜จ ๊ฐ„ ๋ฐ˜์‘, ์•™๊ธˆ ์นจ์ „ ๋ฐ˜์‘)๊ณผ ์œ ์ฒด ์—ญํ•™, ๋ฐ˜์‘์—ด, ์—ด์—ญํ•™์  ๋ณ€ํ™” ๋ฐ ์šด์ „ ์ƒ์˜ ์ด๋ฒคํŠธ ๋ฐœ์ƒ์„ ๋ชจ๋‘ ๊ณ ๋ คํ•  ์ˆ˜ ์žˆ๋‹ค. ๋ชจ๋ธ์„ ์ด์šฉํ•ด ์ด์‚ฐํ™”ํƒ„์†Œ ์ œ๊ฑฐ ํšจ์œจ, pH ๋ฐ ์˜จ๋„ ๋ณ€ํ™”๋ฅผ ์˜ˆ์ธกํ•˜์—ฌ ์‹ค์ œ ์šด์ „ ๋ฐ์ดํ„ฐ์™€ ๋น„๊ตํ•œ ๊ฒฐ๊ณผ, ํŒŒ๋ผ๋ฏธํ„ฐ๋ฅผ ํ†ตํ•œ ๋ณด์ •์ด ์ „ํ˜€ ์—†์ด๋„ 7 % ์ด๋‚ด์˜ ์˜ค์ฐจ๋ฅผ ๋ณด์—ฌ์ฃผ์—ˆ๋‹ค. ๋ชจ๋ธ์˜ ๋ถ€์ •ํ™•์„ฑ ๋ฌธ์ œ๋Š” ๋ชจ๋ธ๋ง ํ›„ ์‹คํ—˜ ๊ฒฐ๊ณผ๋ฅผ ์ด์šฉํ•œ ๋ชจ๋ธ ๋ณด์ •์œผ๋กœ ๊ทน๋ณต ํ•  ์ˆ˜ ์žˆ๋‹ค. ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ๊ด‘๋ฌผ ํƒ„์‚ฐํ™” ๋ฐ˜์‘๊ธฐ ๋ชจ๋ธ์„ ๋ฒ ์ด์ง€์•ˆ ๋ณด์ •(Bayesian calibration)์„ ํ†ตํ•ด ๊ฐ•ํ™”ํ•˜๋Š” ๋ฐฉ๋ฒ•์„ ์ œ์‹œํ•œ๋‹ค. ๋จผ์ € ๋ชจ๋ธ ์ค‘ ๋ถˆํ™•์‹คํ•œ ๋ถ€๋ถ„์— 8๊ฐœ์˜ ํŒŒ๋ผ๋ฏธํ„ฐ๋ฅผ ๋„์ž…ํ•œ ํ›„, ๋ฒ ์ด์ง€์•ˆ ํŒŒ๋ผ๋ฏธํ„ฐ ์ถ”์ •๋ฒ•(Bayesian parameter estimation) ๋ฐ ์‹คํ—˜์‹ค ๊ทœ๋ชจ์—์„œ์˜ ์‹คํ—˜ ๊ฒฐ๊ณผ๋“ค์„ ์ด์šฉํ•˜์—ฌ ํŒŒ๋ผ๋ฏธํ„ฐ๋“ค์˜ ์‚ฌํ›„ ํ™•๋ฅ  ๋ถ„ํฌ๋ฅผ ์ถ”์ •ํ•˜์˜€๋‹ค. ์–ป์–ด์ง„ ํŒŒ๋ผ๋ฏธํ„ฐ์˜ ํ™•๋ฅ  ๋ถ„ํฌ๋“ค์€ ๋ชจ๋ธ ๋ฐ ์‹คํ—˜์˜ ๋ถˆ์™„์ „์„ฑ์œผ๋กœ ์ธํ•ด ๋‚˜ํƒ€๋‚˜๋Š” ํŒŒ๋ผ๋ฏธํ„ฐ์˜ ๋ถˆํ™•์‹ค์„ฑ ๋ฐ ๋‹ค์ค‘ ๋ด‰์šฐ๋ฆฌ ํŠน์„ฑ์„ ๋ฐ˜์˜ํ•˜๊ณ  ์žˆ๋‹ค. ์ด๋ฅผ ์ด์šฉํ•˜์—ฌ ์‹คํ—˜ ๊ฒฐ๊ณผ๋ฅผ ์ž˜ ๋”ฐ๋ผ๊ฐ€๋Š” ํ™•๋ฅ ๋ก ์  ๋ชจ๋ธ ์˜ˆ์ธก์น˜(stochastic model response)๋ฅผ ์–ป์„ ์ˆ˜ ์žˆ์—ˆ๋‹ค. 16๊ฐœ์˜ ์‹คํ—˜ ๋ฐ์ดํ„ฐ์…‹ ๋ฐ ํ…Œ์ŠคํŠธ์…‹์˜ ํ”ผํŒ… ์—๋Ÿฌ(fitting error)๋Š” ๊ฒฐ์ •๋ก ์ ์ธ ์ตœ์ ํ™” ์•Œ๊ณ ๋ฆฌ์ฆ˜(deterministic optimization)์„ ์‚ฌ์šฉํ•  ๋•Œ๋ณด๋‹ค ๋น„์Šทํ•˜๊ฑฐ๋‚˜ ๋‚ฎ์€ ๊ฒƒ์œผ๋กœ ์ธก์ •๋˜์—ˆ๋‹ค. ์ˆ˜ํ•™์  ์ตœ์ ํ™”์— ์“ฐ์ด๊ธฐ์— ๋„ˆ๋ฌด ๊ธด ์‹œ๋ฎฌ๋ ˆ์ด์…˜ ์‹œ๊ฐ„ ๋ฌธ์ œ๋Š” ๋ฒ ์ด์ง€์•ˆ ์ตœ์ ํ™” ์•Œ๊ณ ๋ฆฌ์ฆ˜์„ ์ ์šฉํ•˜์—ฌ ํ•ด๊ฒฐํ•  ์ˆ˜ ์žˆ๋‹ค. ํ™”ํ•™ ๋ฐ˜์‘๊ธฐ ์„ค๊ณ„ ์ตœ์ ํ™”๋ฅผ ์œ„ํ•ด ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ๋‹ค์ค‘ ๋ชฉ์  ๋ฒ ์ด์ง€์•ˆ ์ตœ์ ํ™”(Multi-objective Bayesian Optimization, MBO)๋ฅผ ์‚ฌ์šฉํ•ด ์‹œ๋ฎฌ๋ ˆ์ด์…˜ ํšŸ์ˆ˜๋ฅผ ์ตœ์†Œํ™” ํ•˜๋Š” CFD ๊ธฐ๋ฐ˜ ์ตœ์  ์„ค๊ณ„ ๋ฐฉ๋ฒ•์„ ์ œ์•ˆํ•˜์˜€๋‹ค. ์—ฌ์„ฏ ๊ฐ€์ง€ ์„ค๊ณ„ ๋ณ€์ˆ˜๋ฅผ ๊ฐ€์ง€๋Š” ๊ธฐ-์•ก ๊ต๋ฐ˜ ํƒฑํฌ ๋ฐ˜์‘๊ธฐ์—์„œ ์ „๋ ฅ ์†Œ๋น„๋ฅผ ์ตœ์†Œํ™”ํ•˜๊ณ  ๊ฐ€์Šค ๋ถ„์œจ(gas holdup)๋ฅผ ๊ทน๋Œ€ํ™”ํ•˜๊ธฐ ์œ„ํ•ด ์ด ๋ฐฉ๋ฒ•์„ ์ด์šฉํ•œ ๊ฒฐ๊ณผ, ๋‹จ 100 ํšŒ์˜ ์‹œ๋ฎฌ๋ ˆ์ด์…˜ ๋งŒ์œผ๋กœ ์ตœ์  ํŒŒ๋ ˆํ†  ์ปค๋ธŒ(Pareto curve)๋ฅผ ์–ป์„ ์ˆ˜ ์žˆ์—ˆ๋‹ค. ์ œ์•ˆ๋œ ์ตœ์  ์„ค๊ณ„์•ˆ๋“ค์€ ๋ฌธํ—Œ์— ๋ณด๊ณ ๋œ ๊ธฐ์กด ๋ฐ˜์‘๊ธฐ๋“ค๊ณผ ๋น„๊ตํ•ด ๋›ฐ์–ด๋‚œ ์„ฑ๋Šฅ์„ ๋ณด์—ฌ์ฃผ์—ˆ๋‹ค. . ๋ณธ ๋…ผ๋ฌธ์„ ํ†ตํ•ด ์ œ์•ˆ๋œ CFD ๊ธฐ๋ฐ˜ ๊ตฌํš ๋ชจ๋ธ๋ง๋ฒ•, ๋ฒ ์ด์ง€์•ˆ ๋ชจ๋ธ ๋ณด์ •๋ฒ• ๋ฐ ๋ฒ ์ด์ง€์•ˆ ์ตœ์ ํ™” ๋ฐฉ๋ฒ•์€ ๋ณต์žกํ•œ ๋ฌผ๋ฆฌ์  ๋ฐ ํ™”ํ•™์  ํŠน์ง•์„ ๊ฐ–๋Š” ์‚ฐ์—… ๊ทœ๋ชจ์˜ ํ™”ํ•™ ๋ฐ˜์‘๊ธฐ์— ์ ์šฉ๋  ์ˆ˜ ์žˆ์„ ๊ฒƒ์œผ๋กœ ๊ธฐ๋Œ€๋œ๋‹ค.This thesis presents a design strategy for industrial-scale chemical reactors which consists of multi-scale modeling, post-modeling calibration, and optimization. Although the reactor design problem is a primary step in the development of most chemical processes, it has been relied on simple models, experiments and rules of thumbs rather than taking advantage of recent numerical techniques. It is because industrial-size reactors show high complexity and scale differences both physically and chemically, which makes it difficult to be mathematically modeled. Even after the model is constructed, it suffers from inaccuracies and heavy simulation time to be applied in optimization algorithms. The complexity and scale difference problem in modeling can be solved by introducing multi-scale modeling approaches. Computational fluid dynamics (CFD)-based compartmental model makes it possible to simulate hours of dynamics in large size reactors which show inhomogeneous mixing patterns. It regards the big reactor as a network of small zones in which perfect mixing can be assumed and solves mass and energy balance equations with kinetics and flow information adopted from CFD hydrodynamics model at each zone. An aqueous mineral carbonation reactor with complex gasโ€“liquidโ€“solid interacting flow patterns was modeled using this method. The model considers the gas-liquid mass transfer, solid dissolution, ionic reactions, precipitations, hydrodynamics, heat generation and thermodynamic changes by the reaction and discrete operational events in the form of differential algebraic equations (DAEs). The total CO2 removal efficiency, pH, and temperature changes were predicted and compared to real operation data. The errors were within 7 % without any post-adjustment. The inaccuracy problem of model can be overcome by post-modeling approach, such as the calibration with experiments. The model for aqueous mineral carbonation reactor was intensified via Bayesian calibration. Eight parameters were intrduced in the uncertain parts of the rigorous reactor model. Then the calibration was performed by estimating the parameter posterior distribution using Bayesian parameter estimation framework and lab-scale experiments. The developed Bayesian parameter estimation framework involves surrogate models, Markov chain Monte Carlo (MCMC) with tempering, global optimization, and various analysis tools. The obtained parameter distributions reflected the uncertain or multimodal natures of the parameters due to the incompleteness of the model and the experiments. They were used to earn stochastic model responses which show good fits with the experimental results. The fitting errors of all the 16 datasets and the unseen test set were measured to be comparable or lower than when deterministic optimization methods are used. The heavy simulation time problem for mathematical optimization can be resolved by applying Bayesian optimizaion algorithm. CFD based optimal design tool for chemical reactors, in which multi-objective Bayesian optimization (MBO) is utilized to reduce the number of required CFD runs, is proposed. The developed optimizer was applied to minimize the power consumption and maximize the gas holdup in a gas-sparged stirred tank reactor, which has six design variables. The saturated Pareto front was obtained after only 100 iterations. The resulting Pareto front consists of many near-optimal designs with significantly enhanced performances compared to conventional reactors reported in the literature. It is anticipated that the suggested CFD-based compartmental modeling, post-modeling Bayesian calibration, and Bayesian optimization methods can be applied in general industrial-scale chemical reactors with complex physical and chemical features.1. Introduction 1 1.1. Industrial-scale chemical reactor design 1 1.2. Role of mathematical models in reactor design 2 1.3. Intensification of reactor models through calibration 5 1.3.1. Bayesian parameter estimation 6 1.4. Optimization of the reactor models 7 1.4.1. Bayesian optimization 9 1.5. Aqueous mineral carbonation process : case study subject 10 1.6. Outline of the thesis 12 2. Multi-scale modeling of industrial-scale aqueous mineral carbonation reactor for long-time dynamic simulation 14 2.1. Objective 14 2.2. Experimental setup 15 2.3. Mathematical models 19 2.3.1. Reactor model 19 2.3.2. CFD model 28 2.3.3. Numerical setting 30 2.4. Results and discussions 32 2.4.1. CFD-based compartmental model for industrial-scale reactor. 32 2.4.2. Design and simulation of higher-scale reactors 42 2.5. Conclusions 47 3. Model intensification of aqueous mineral carbonation kinetics via Bayesian calibration 50 3.1. Objective 50 3.2. Experimental methods 51 3.2.1. Solution and gas preparation 51 3.2.2. Laboratory-scale mineral carbonation process 53 3.3. Mathematical models 56 3.3.1. Kinetics of aqueous mineral carbonation process 56 3.3.2. Differential algebraic equation (DAE) model for the reactor 65 3.3.3. Discrete events for simulation procedure 71 3.3.4. Numerical setting 72 3.4. Bayesian parameter estimation 72 3.4.1. Problem formulation 73 3.4.2. Bayesian posterior inference 76 3.4.3. Sampling 81 3.5. Results and discussions 82 3.5.1. Stochastic output response 82 3.5.2. Quality of parameter estimtates 86 3.5.3. Assessment of parameter uncertainties 91 3.5.4. Kinetics study with the proposed model parameters 99 3.6. Conclusions 103 4. Multi-objective optimization of chemical reactor design using computational fluid dynamics 106 4.1. Objective 106 4.2. Problem Formulation 107 4.3. Optimization scheme 113 4.3.1. Multi-objective optimization algorithm 113 4.3.2. CFD-MBO optimizer 120 4.4. CFD modeling 125 4.4.1. Tank specifications 125 4.4.2. Governing equations 125 4.4.3. Simulation methods 127 4.5. Results and discussion 128 4.5.1. CFD model validation 128 4.5.2. Optimization results 130 4.5.3. Analysis of optimal designs 139 4.6. Conclusions 144 5. Concluding Remarks 146 Bibliography 149 Abstract in Korean (๊ตญ๋ฌธ์ดˆ๋ก) 163Docto

    Classification Algorithms based on Generalized Polynomial Chaos

    Get PDF
    Classification is one of the most important tasks in process system engineering. Since most of the classification algorithms are generally based on mathematical models, they inseparably involve the quantification and propagation of model uncertainty onto the variables used for classification. Such uncertainty may originate from either a lack of knowledge of the underlying process or from the intrinsic time varying phenomena such as unmeasured disturbances and noise. Often, model uncertainty has been modeled in a probabilistic way and Monte Carlo (MC) type sampling methods have been the method of choice for quantifying the effects of uncertainty. However, MC methods may be computationally prohibitive especially for nonlinear complex systems and systems involving many variables. Alternatively, stochastic spectral methods such as the generalized polynomial chaos (gPC) expansion have emerged as a promising technique that can be used for uncertainty quantification and propagation. Such methods can approximate the stochastic variables by a truncated gPC series where the coefficients of these series can be calculated by Galerkin projection with the mathematical models describing the process. Following these steps, the gPC expansion based methods can converge much faster to a solution than MC type sampling based methods. Using the gPC based uncertainty quantification and propagation method, this current project focuses on the following three problems: (i) fault detection and diagnosis (FDD) in the presence of stochastic faults entering the system; (ii) simultaneous optimal tuning of a FDD algorithm and a feedback controller to enhance the detectability of faults while mitigating the closed loop process variability; (iii) classification of apoptotic cells versus normal cells using morphological features identified from a stochastic image segmentation algorithm in combination with machine learning techniques. The algorithms developed in this work are shown to be highly efficient in terms of computational time, improved fault diagnosis and accurate classification of apoptotic versus normal cells

    Sensitivity and Uncertainty Analysis of Multiphysics Nuclear Reactor Core Depletion

    Full text link
    Nuclear reactor simulation is a complex process described by the neutronic, thermal-hydraulic, and fuel thermo-mechanical behavior of the core components. In current generation reactor physics analysis these three areas are at best loosely coupled. Within this work, a methodology for tightly coupling the core neutronics code PARCS, thermal-hydraulics code PATHS, and fuel rod simulator code FRAPCON was developed. This coupled code package was applied to two fuel depletion problems. The behavior of the fuel-cladding gap and associated temperature drop was found to be important. The code package was then applied to the pin cell calculation to evaluate the uncertainty and sensitivity of the nuclear performance of the core due to the influence of fuel thermo-mechanical models available for manipulation in FRAPCON. A sensitivity study was conducted to determine which fuel models were influential on the neutronics outputs; we determined that fuel thermal conductivity, fuel thermal expansion, cladding creep, fuel swelling and heat transfer coefficient had an important influence on some neutronics parameters. The package was integrated within the DAKOTA uncertainty package. Two sampling-based methods and two stochastic expansion methods were used to evaluate the uncertainty in the nuclear parameters throughout core depletion. We found that the uncertainty in the core reactivity was approximately 60 pcm at the beginning of depletion, reducing to approximately 15 pcm by the end of life, due to the effect of plutonium buildup reducing the importance of fuel uncertainty on high-burnup fuel. We found that the response statistics could be well-estimated by a first-order tensor-product PCE expansion, only requiring 32 calculations. Using variance-based decomposition, we found that initially the most important models contributing to nuclear variance were the thermal conductivity and fuel thermal expansion models. Once the fuel-clad gap closes, however, fuel thermal conductivity uncertainty dominates the overall variance in the output. We also found that the importance of input interactions on overall variance is negligible; at worst case, interaction effects contribute ~3% of the overall variance in both Doppler temperature and reactivity.PhDNuclear Engineering and Radiological SciencesUniversity of Michigan, Horace H. Rackham School of Graduate Studieshttp://deepblue.lib.umich.edu/bitstream/2027.42/111444/1/asbiele_1.pd
    • โ€ฆ
    corecore