612 research outputs found

    Onboard Plasmatron Hydrogen Production for Improved Vehicles

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    Energy Efficient Thermal Management for Natural Gas Engine Aftertreatment via Active Flow Control

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    Supervisory control of complex propulsion subsystems

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    Modern gasoline and diesel combustion engines are equipped with several subsystems with the goal to reduce fuel consumption and pollutant exhaust emissions. Subsystem synergies could be harnessed using the supervisory control approach. Look-ahead information can be used to potentially optimise power-train control for real time implementation. This thesis delves upon modelling the exhaust emissions from a combustion engine and developing a combined equivalent objective metric to propose a supervisory controller that uses look-ahead information with the objective to reduce fuel consumed and exhaust emissions. In the first part of the thesis, the focus is on diesel engine application control for emissions and fuel consumption reduction.\ua0Model of exhaust emissions in a diesel engine obtained from a combination of nominal engine operation and deviations are evaluated for transient drive cycles.\ua0The look ahead information as a trajectory of vehicle speed and load over time is considered.\ua0The supervisory controller considers a discrete control action set over the first segment of the trip ahead.\ua0The cost to optimise is defined and pre-computed off-line for a discrete set of operating conditions.\ua0A full factorial optimisation carried out off-line is stored on board the vehicle and applied in real-time.\ua0In a first proposal, the subsystem control of the after-treatment system comprising the lean NOx trap and the selective reduction catalyst is considered.\ua0As a next iteration, the combustion engine is added to the control problem.\ua0Simulation comparison of the controllers with the baseline controller offers a 1 % total fuel equivalent cost improvement while offering the flexibility to tailor the controller for different cost objective. In the second part of the thesis, the focus is on cold-start emissions control for modern gasoline engines.\ua0Emissions occurring when the engine is started until the catalyst is sufficiently warm, contribute to a significant proportion of tailpipe pollutant emissions.\ua0Electrically heated catalyst (EHC) in the three way catalyst (TWC) is a promising technology to reduce cold-start emissions where the catalyst can be warmed up prior to engine start and continued after start.\ua0A simulation framework for the engine, TWC with EHC with focus on modeling the thermal and chemical interactions during cold-start was developed.\ua0An evaluation framework with a proposed equivalent emissions approach was developed considering the challenges associated with cold-start emission control.\ua0An equivalent emission optimal post-heating time for the EHC is proposed that adapts to information which is available in a real-time on-line implementation.\ua0The proposed controller falls short of just 1 % equivalent emissions compared to the optimal case

    Diesel Engine

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    Diesel engines, also known as CI engines, possess a wide field of applications as energy converters because of their higher efficiency. However, diesel engines are a major source of NOX and particulate matter (PM) emissions. Because of its importance, five chapters in this book have been devoted to the formulation and control of these pollutants. The world is currently experiencing an oil crisis. Gaseous fuels like natural gas, pure hydrogen gas, biomass-based and coke-based syngas can be considered as alternative fuels for diesel engines. Their combustion and exhaust emissions characteristics are described in this book. Reliable early detection of malfunction and failure of any parts in diesel engines can save the engine from failing completely and save high repair cost. Tools are discussed in this book to detect common failure modes of diesel engine that can detect early signs of failure

    Onboard Plasmatron Hydrogen Production for Improved Vehicles

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    Low Emissions Aftertreatment and Diesel Emissions Reduction

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    Automotive Powertrain Control โ€” A Survey

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    This paper surveys recent and historical publications on automotive powertrain control. Control-oriented models of gasoline and diesel engines and their aftertreatment systems are reviewed, and challenging control problems for conventional engines, hybrid vehicles and fuel cell powertrains are discussed. Fundamentals are revisited and advancements are highlighted. A comprehensive list of references is provided.Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/72023/1/j.1934-6093.2006.tb00275.x.pd

    A Two Dimensional Numerical Soot Model for Advanced Design and Control of Diesel Particulate Filters

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    One of the most effective methods to control diesel particulate matter (PM) emissions from heavy duty diesel engines is to use wall flow diesel particulate filters (DPF). It is still a major challenge to get an accurate estimation of soot loading, which is crucial for the engine afterteratment assembly optimization. In the recent past, several advanced computational models of DPF filtration and regeneration have been presented to assess the cost effective optimization of future particulate trap systems. They are characterized by different degree of detail and computational costs, depending on the specific application (i.e diagnostics, control, system design, component design etc).;The objective of this study is to compare in detail a two dimensional (2-D) approach with a one dimensional (1-D) approach, thus giving a better insight of the variation of properties over the DPF length. This task has been archived by extending an in-house developed 1-D numerical soot model to the next dimension to understand the impact of 2-D representation to predict both steady state and transient behavior of a catalyzed diesel particulate filter (CDPF). Performance of the model was evaluated using three key parameters: pressure drop, filter outlet temperature and soot mass retained in the filter during both active and continuous regeneration events. Quasi-steady state conservation of mass, momentum and energy equations were solved numerically using finite difference methods adopting a spatially uniform mesh. The results obtained from the current model were compared with the 1-D code to evaluate the general validity of assumptions made in the latter, especially DPF loading status prediction.;The model was validated using the data gathered at the West Virginia University Engine and Emissions Research Laboratory (WVU-EERL) using a model year 2004 Mack MP7-355E Diesel engine coupled to a Johnson Matthey catalyzed diesel particulate filter (CDPF) exercised over a 13 mode European stationary cycle (ESC) followed by two federal transient cycles (FTP). A constant set of model tuning parameters were maintained for the sake of general validation of simplifying assumptions of the 1-D code.;The analysis shows that the predicted pressure drop across the DPF is in good agreement with the data obtained at EERL in both steady state and transient cycles. It is also shown that the soot accumulates mainly in the frontal and rear parts across the filter length under given soot concentrations. The model is capable of tracking DPF soot mass satisfactorily with a maximum discrepancy of 3.47g during steady state cycle. A 7.95% decrease in soot layer thickness can be seen in the front portion of the DPF during the transient cycle mainly due to O2 assisted regeneration at elevated temperatures. Both 1-D and 2-D models produce similar results during the loading phase. However, the current model is able to capture regeneration phase of the FTP cycle more descriptively than the 1-D model. The discrepancy of the reported total soot mass estimation between two models was 2.12%. The distribution corresponding to the 1-D model is representative of soot layer distribution given by the 2-D model at one tenth distance away from the DPF front face. 1-D model representation is effective towards PM prediction, although presenting considerable axial effects at higher DPF temperatures

    ๋””์ ค ์—”์ง„์—์„œ ๊ฐ€์ƒ ์งˆ์†Œ์‚ฐํ™”๋ฌผ ์„ผ์„œ์— ๊ด€ํ•œ ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€, 2013. 8. ๋ฏผ๊ฒฝ๋•.thus, this model can be applied to engines and after-treatment systems as a useful tool to control the engine-out NO without the use of a NOx sensor. In addition to being a virtual NO sensor, the estimation model can be applied to 1-D simulations, such as GT-SUITE and AMESIM, and demonstrate improved NO estimation results as the model is able to predict the NO level as same standard as the 3-D CFD simulation. Then, a newly developed NO estimation model was implemented on the embedded system bypassed from a conventional engine control unit for real-time estimation of NO during steady-states and transient engine operations. The results of the model were compared to real-time measurement of engine-out NO of a conventional Diesel engine at representative steady state operating points which cover the entire NEDC region. Also, EGR rate and main injection timing were varied to verify the predictability of the model under various conditions. The results showed that the model predicts steady state results well with R2 value of 0.96 for 76 HP-EGR cases. In addition, to verify transient estimation of NO, the engine-out NO was measured by a fast NO analyzer and compared with the results of the model during simple ramp transition conditions. Additionally, the engine-out NO emissions measured by a fast NOx analyzer and the estimated NO emissions were compared during ECE-15 and EUDC cycles. Furthermore, to extend the NO model to a complete NOx estimation model, an empirical NO2 estimation model was proposed based on the experiments under steady-state conditions. The in-house EGR estimation model was also applied in the NOx estimation model for accurate cycle-by-cycle estimation and used as an input during transient engine operations. This systematic research on the development of a virtual NOx sensor contributes to real-time NOx monitoring for transient NOx control and after-treatment system control.however, there were several limiting factors, such as complexity of the model for a real-time application, the necessity of various calibration constants, fitting processes for empirical equations and the demand for training for numerical models. In this study, to overcome the limits of previous studies, a real-time nitric oxide estimation model was developed based on the in-cylinder pressure and on data available from the ECU. As computational fluid dynamics can describe the process of NO formation which is not directly obtainable from experiments on a physical basis, the NO formation model was developed based on both the analysis of CFD results as well as on a physical model. Furthermore, the in-cylinder pressure is used to predict the amount of NO formation under various engine operating conditions as the pressure reflects the change in the combustion characteristics. The estimation model consisted of a simple calculation processTo meet the stringent emission regulations on diesel engines, engine-out emissions have been lowered by adapting new combustion concepts such as low-temperature combustion and after-treatment systems have also been used to reduce tailpipe emissions. To optimize the control of both in-cylinder combustion and the efficiency of an after treatment system to reduce NOx, the amount of real-time NOx emissions should be determined. Thus, many studies on a virtual NOx sensor using physical and phenomenological models have been reported. Previous studies have shown reliable NOx estimationstherefore, the model could predict the cycle-by-cycle NO in real-time. The validation results show that the model presented can predict engine-out NO well๋””์ ค ์—”์ง„์— ๋Œ€ํ•œ ๋ฐฐ๊ธฐ ๊ทœ์ œ๊ฐ€ ๊ฐ•ํ™”๋จ์— ๋”ฐ๋ผ ์ƒˆ๋กœ์šด ์—ฐ์†Œ ๊ธฐ๋ฒ•์„ ์ด์šฉํ•˜์—ฌ ์—”์ง„ ์ž์ฒด์˜ ๋ฐฐ์ถœ๋ฌผ์„ ์ค„์ด๊ฑฐ๋‚˜ ํ›„์ฒ˜๋ฆฌ ์žฅ์น˜ ๋“ฑ์„ ์ด์šฉํ•˜์—ฌ ์ตœ์ข… ๋ฐฐ์ถœ๋ฌผ์„ ์ค„์ด๋Š” ๋“ฑ์˜ ๋…ธ๋ ฅ์ด ์ด๋ฃจ์–ด์ง€๊ณ  ์žˆ๋‹ค. ํŠนํžˆ, ์งˆ์†Œ ์‚ฐํ™”๋ฌผ (NOx) ๊ฐ์†Œ๋ฅผ ์œ„ํ•œ ์‹ค๋ฆฐ๋” ๋‚ด ์—ฐ์†Œ์ œ์–ด, ๋™์‹œ์— ํ›„์ฒ˜๋ฆฌ ์žฅ์น˜์˜ ํšจ์œจ์„ ์ตœ์ ํ™”ํ•˜๊ธฐ ์œ„ํ•ด์„œ๋Š” ์‹ค์‹œ๊ฐ„์œผ๋กœ ๋ฐฐ์ถœ๋˜๋Š”NOx ๋ฐฐ์ถœ๋Ÿ‰์— ๋Œ€ํ•œ ์ •๋ณด๊ฐ€ ํ•„์š”ํ•˜๋‹ค. ๋”ฐ๋ผ์„œ ๋ฌผ๋ฆฌ์ , ํ˜„์ƒํ•™์  ๋ชจ๋ธ์„ ์‚ฌ์šฉํ•œ ๊ฐ€์ƒ NOx ์„ผ์„œ์— ๋Œ€ํ•œ ๋งŽ์€ ์—ฐ๊ตฌ๊ฐ€ ๋ณด๊ณ ๋˜๊ณ  ์žˆ๋‹ค. ๊ธฐ์กด ์—ฐ๊ตฌ๋“ค์€ ๋น„๊ต์  ์ •ํ™•ํ•˜๊ฒŒ NOx ๋ฐฐ์ถœ๋Ÿ‰์„ ์˜ˆ์ธกํ•˜๊ณ  ์žˆ์ง€๋งŒ ์‹ค์‹œ๊ฐ„ ์• ํ”Œ๋ฆฌ์ผ€์ด์…˜์œผ๋กœ์จ ํ™œ์šฉํ•˜๊ธฐ์—๋Š” ํ˜„์žฌ ์ฐจ๋Ÿ‰์— ์žฅ์ฐฉ ์ค‘์ธ ์—”์ง„ ์ œ์–ด ์žฅ์น˜์˜ ๊ณ„์‚ฐ ๋Šฅ๋ ฅ์— ๋น„ํ•ด ๋ชจ๋ธ์ด ๋„ˆ๋ฌด ๋ณต์žกํ•˜๊ฑฐ๋‚˜, ๊ฒฝํ—˜์‹์„ ํ”ผํŒ…ํ•˜๊ธฐ ์œ„ํ•ด ๋งŽ์€ ๋ณด์ • ์ƒ์ˆ˜๊ฐ€ ์‚ฌ์šฉ๋˜๊ณ , ํ†ต๊ณ„์  ์ˆ˜ํ•™์  ๋ชจ๋ธ ๋“ฑ์˜ ๊ฒฝ์šฐ์—๋Š” ๋งŽ์€ ํŠธ๋ ˆ์ด๋‹์ด ํ•„์š”ํ•œ ๋“ฑ์˜ ์—ฌ๋Ÿฌ ๊ฐ€์ง€ ์ œํ•œ ์š”์ธ์ด ์žˆ์—ˆ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์„ ํ–‰ ์—ฐ๊ตฌ์˜ ํ•œ๊ณ„๋ฅผ ๊ทน๋ณตํ•˜๊ธฐ ์œ„ํ•ด ์‹ค์‹œ๊ฐ„ ์‹ค๋ฆฐ๋” ์••๋ ฅ๊ณผ ECU์—์„œ ์–ป์„ ์ˆ˜ ์žˆ๋Š” ๋ฐ์ดํ„ฐ์— ๊ธฐ๋ฐ˜ํ•œ ์‹ค์‹œ๊ฐ„ NOx ์˜ˆ์ธก ๋ชจ๋ธ์„ ๊ฐœ๋ฐœํ•˜์˜€๋‹ค. CFD ๋Š” ์‹คํ—˜ ๊ณผ์ •์—์„œ ์ง์ ‘ ์–ป์„ ์ˆ˜ ์—†๋Š” NO์˜ ํ˜•์„ฑ ๊ณผ์ •์„ ์ž์„ธํžˆ ์„ค๋ช… ํ•  ์ˆ˜ ์žˆ๊ธฐ ๋•Œ๋ฌธ์—, ๋ฌผ๋ฆฌ์  ๋ถ„์„๊ณผ ํ•จ๊ป˜ CFD ๊ฒฐ๊ณผ์˜ ๋ถ„์„์„ ํ†ตํ•ด ๋ชจ๋ธ์„ ๊ฐœ๋ฐœํ•˜์˜€๋‹ค. ๋˜ํ•œ ์‹ค๋ฆฐ๋” ๋‚ด ์••๋ ฅ์ด ์—”์ง„ ์—ฐ์†ŒํŠน์„ฑ์˜ ๋ณ€ํ™”๋ฅผ ์ž˜ ๋ฐ˜์˜ํ•˜๊ธฐ ๋•Œ๋ฌธ์—, ๋‹ค์–‘ํ•œ ์—”์ง„์˜ ์ž‘๋™ ์กฐ๊ฑด์—์„œ NO์˜ ๋ฐฐ์ถœ๋Ÿ‰์„ ์˜ˆ์ธกํ•  ์ˆ˜ ์žˆ๋„๋ก ์—ฐ์†Œ์••๋ ฅ์ด ์‚ฌ์šฉ๋˜์—ˆ๋‹ค. ๊ฐœ๋ฐœ๋œ NO ์˜ˆ์ธก ๋ชจ๋ธ์€ ๊ฐ„๋‹จํ•œ ๊ณ„์‚ฐ ๊ณผ์ •์œผ๋กœ ์ด๋ฃจ์–ด์กŒ๊ธฐ ๋•Œ๋ฌธ์— ์‹ค์‹œ๊ฐ„์œผ๋กœ ์‚ฌ์ดํด ๋ณ„ NO๋ฅผ ์˜ˆ์ธกํ•  ์ˆ˜ ์žˆ์—ˆ๋‹ค. ๊ฒ€์ฆ ๊ฒฐ๊ณผ๋Š” ์ œ์•ˆ๋œ ๋ชจ๋ธ์ด ์—”์ง„์—์„œ ๋ฐฐ์ถœ๋˜๋Š” NO ๋ฅผ ์ž˜ ์˜ˆ์ธกํ•˜๋Š” ๊ฒƒ์„ ๋ณด์—ฌ์ฃผ์—ˆ๊ณ , ๋”ฐ๋ผ์„œ ๊ฐœ๋ฐœ๋œ ๋ชจ๋ธ์ด NO์„ผ์„œ ๋Œ€์šฉ์œผ๋กœ์จ ์—”์ง„๊ณผ ํ›„์ฒ˜๋ฆฌ ์žฅ์น˜์˜ ์ œ์–ด๋ฅผ ์œ„ํ•œ ์œ ์šฉํ•œ ๋„๊ตฌ๋กœ์จ ์‹œ์Šคํ…œ์— ์ ์šฉ๋  ์ˆ˜ ์žˆ์Œ์„ ํ™•์ธํ•˜์˜€๋‹ค. ๊ฐ€์ƒ NO ์„ผ์„œ๋กœ ์‚ฌ์šฉ๋  ์ˆ˜ ์žˆ๋Š” ๊ฒƒ ์ด์™ธ์—๋„, ๊ฐœ๋ฐœ๋œ NO ์˜ˆ์ธก ๋ชจ๋ธ์€ GT-SUITE์™€ AMESim ๊ณผ ๊ฐ™์€ 1 ์ฐจ์› ์‹œ๋ฎฌ๋ ˆ์ด์…˜์— ์ ์šฉ๋˜์–ดCFD ๋ชจ๋ธ๊ณผ ๋™์ผํ•œ ์ˆ˜์ค€์œผ๋กœ NO ์ˆ˜์ค€์„ ์˜ˆ์ธกํ•  ์ˆ˜ ์žˆ๋Š” ๊ฐ€๋Šฅ์„ฑ์„ ๊ฐ€์ง€๊ณ  ์žˆ๋‹ค. ์ดํ›„, ๊ฐœ๋ฐœ ๋œ NO์˜ˆ์ธก ๋ชจ๋ธ์€ ์ •์ƒ ์ƒํƒœ์™€ ๊ณผ๋„ ์—”์ง„ ์ž‘๋™ ์ƒํƒœ์—์„œ NO์˜ ์‹ค์‹œ๊ฐ„ ์ถ”์ •์„ ์œ„ํ•œ ๊ธฐ์กด์˜ ์—”์ง„ ์ œ์–ด ์žฅ์น˜๋ฅผ ์šฐํšŒํ•œ ์ž„๋ฒ ๋””๋“œ ์‹œ์Šคํ…œ์— ๊ตฌํ˜„๋˜์—ˆ๋‹ค. ๋ชจ๋ธ์˜ ๊ฒฐ๊ณผ๋Š” NEDC ์ „ ์˜์—ญ์„ ์ปค๋ฒ„ํ•˜๋Š” ๋Œ€ํ‘œ์ ์ธ ์ •์ƒ ์ƒํƒœ์˜ ๋™์ž‘ ์ ์—์„œ ์—”์ง„์—์„œ ๋ฐฐ์ถœ๋˜๋Š” ์‹ค์‹œ๊ฐ„ NO ์ธก์ •๊ฐ’๊ณผ ๋น„๊ต๋˜์—ˆ๋‹ค. ๋˜ํ•œ ๋‹ค์–‘ํ•œ ์กฐ๊ฑด์—์„œ ๋ชจ๋ธ์˜ ์˜ˆ์ธก์„ฑ์„ ๊ฒ€์ฆํ•˜๊ธฐ ์œ„ํ•ด ๋ฐฐ๊ธฐ๊ฐ€์Šค ์žฌ์ˆœํ™˜์œจ๊ณผ ์ฃผ๋ถ„์‚ฌ์‹œ๊ธฐ๋ฅผ ๋ฒ ์ด์Šค ์กฐ๊ฑด ๋Œ€๋น„ ๋ณ€ํ™”์‹œ์ผฐ๋‹ค. ์ •์ƒ์ƒํƒœ ๊ฒ€์ฆ ๊ฒฐ๊ณผ HP-EGR 76 ์ผ€์ด์Šค์—์„œ ์‹คํ—˜ ๊ฒฐ๊ณผ์™€ R2=0.96 ์˜ ๋†’์€ ์˜ˆ์ธก ์ •๋„๋ฅผ ํ™•์ธํ•  ์ˆ˜ ์žˆ์—ˆ๋‹ค. ๋˜ํ•œ ๊ณผ๋„์ƒํƒœ์—์„œ์˜ NO ์˜ˆ์ธก ์ •๋„๋ฅผ ๊ฒ€์ฆํ•˜๊ธฐ ์œ„ํ•ด ๊ณ ์† NOx ๋ถ„์„๊ธฐ๋ฅผ ์‚ฌ์šฉํ•˜์—ฌ ์—”์ง„ ์†๋„, ๋ถ€ํ•˜ ๋ณ€๊ฒฝ ๋“ฑ์˜ ๊ฐ„๋‹จํ•œ ๋žจํ”„ ์กฐ๊ฑด์—์„œ ๋ชจ๋ธ ๊ฒฐ๊ณผ์™€ ๋น„๊ตํ•˜์˜€๋‹ค. ๋˜ํ•œ ์œ ๋Ÿฝ์˜ ๋ฐฐ์ถœ๊ฐ€์Šค ์ธก์ • ๋ชจ๋“œ์ธ ECE-15 ์™€ EUDC ์‚ฌ์ดํด์—์„œ ๊ณ ์† NOx ๋ถ„์„๊ธฐ ๊ฒฐ๊ณผ๋ฅผ ์‚ฌ์šฉํ•˜์—ฌ ๋ชจ๋ธ์„ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ์ถ”๊ฐ€์ ์œผ๋กœ, NO ๋งŒ์ด ์•„๋‹Œ ์ „์ฒด NOx๋ฅผ ์˜ˆ์ธกํ•  ์ˆ˜ ์žˆ๋„๋ก ์ •์ƒ์ƒํƒœ ์‹คํ—˜ ๊ฒฐ๊ณผ ๊ธฐ๋ฐ˜์˜ ๊ฒฝํ—˜์‹์„ ์‚ฌ์šฉํ•œ NO2 ์˜ˆ์ธก ๋ชจ๋ธ์„ ์ œ์•ˆํ•˜์˜€๋‹ค. ์‹ค์‹œ๊ฐ„ NOx ์˜ˆ์ธก ๋ชจ๋ธ์— ์ •ํ™•ํ•œ ๊ณผ๋„์ƒํƒœ EGR ๊ฐ’์„ ์ œ๊ณตํ•˜๊ธฐ ์œ„ํ•ด ์‹คํ—˜์‹ค์—์„œ ๊ฐœ๋ฐœ๋œ EGR ์˜ˆ์ธก ๋ชจ๋ธ ๋˜ํ•œ ์ ์šฉ ๋˜์—ˆ๋‹ค.Acknowledgements iii Abstract iv Contents vii List of Tables x List of Figures xi Acronym xiv Chapter 1. Introduction 1 1.1 Background and Motivation 1 1.1.1 Nitrogen oxides formation 1 1.1.2 The effect of nitrogen oxides on health and environment 2 1.1.3 Nitrogen oxides emission from diesel engines 3 1.1.4 Emission regulations for NOx from diesel engines 4 1.1.5 NOx reduction technologies and challenges in diesel engines 6 1.2 Literature Review on virtual NOx sensors 23 1.3 Objectives 28 Chapter 2. Development of NO estimation model with in-cylinder pressure measurement 29 2.1 Computational model and validation 30 2.1.1 Computational model for the CFD simulation 30 2.1.2 Validation of the computational models 30 2.2 NO estimation model 36 2.2.1 Basic assumptions for the NO estimation model 36 2.2.2 Physical model for NO formation 36 2.2.3 Determination of the duration of NO formation 39 2.2.4 Determination of averaged NO formation rate 39 2.2.5 Calculation of the maximum NO formation rate 40 2.2.6 Summary of the NO estimation model 43 2.3 Model validation with CFD results 53 Chapter 3. Experimental Apparatus 55 3.1 Engine setup 55 3.2 In-cylinder pressure measurement 61 3.3 EGR measurement 63 3.4 NO and NOx measurement 65 3.5 Real-time calculation of NO 68 Chapter 4. The effect of EGR rate on NO estimation model 72 4.1 Sensitivity analysis 72 4.2 Cylinder-to-cylinder measurement of EGR 74 4.3 EGR estimation model 76 Chapter 5. NO estimation during steady state and simple ramp transition using a real-time virtual NO sensor 82 5.1 Experimental cases 83 5.1.1 Steady state cases 83 5.1.2 Simple ramp transition cases 83 5.2 Experimental results 85 5.2.1 Steady state results 85 5.2.2 Simple ramp transition results 85 5.2.2.1 EGR rate change 85 5.2.2.2 Engine speed change 86 5.2.2.3 Simultaneous engine speed and load change 86 5.2.3 Source of error 86 5.2.4 Improvement of model accuracy using modified R and k 87 5.2.5 Cycle-by-cycle & cylinder-by-cylinder NO estimation 89 Chapter 6. NOx estimation during transient state using a real-time virtual NOx sensor 99 6.1 Extend to NOx (NO2) estimation model 100 6.2 Experimental conditions 105 6.3 Results and discussions 107 Chapter 7. Conclusion 113Docto
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