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1

Gross, Günter. Numerical simulation ofcanopy flows. Berlin: Springer-Verlag, 1993.

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2

Center, NASA Glenn Research, ed. 2000 Numerical Propulsion System Simulation Review. [Cleveland, Ohio]: National Aeronautics and Space Administration, Glenn Research Center, 2001.

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3

Center, NASA Glenn Research, ed. 2000 Numerical Propulsion System Simulation Review. [Cleveland, Ohio]: National Aeronautics and Space Administration, Glenn Research Center, 2001.

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4

Center, NASA Glenn Research, ed. 2000 Numerical Propulsion System Simulation Review. [Cleveland, Ohio]: National Aeronautics and Space Administration, Glenn Research Center, 2001.

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5

Numerical simulation of canopy flows. Berlin: Springer-Verlag, 1993.

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6

Ahuja, J. K. Numerical simulation of shock-induced combustion in a superdetonative hydrogen-air system. Washington, D. C: American Institute of Aeronautics and Astronautics, 1993.

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7

Xu, Da Quan. Numerical simulation of weak blast waves in air using a linear analysis. Japan: [s.n.], 1989.

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8

S, Sato, Kamata M, Yamamoto K, and SpringerLink (Online service), eds. Advanced Monitoring and Numerical Analysis of Coastal Water and Urban Air Environment. Tokyo: Springer Japan, 2010.

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9

Nishikawa, Tracy. Numerical simulation of ground-water flow and land subsidence at Edwards Air Force Base, Antelope Valley, California. Sacramento, Calif: U.S. Dept. of the Interior, U.S. Geological Survey, 2001.

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10

Nishikawa, Tracy. Numerical simulation of ground-water flow and land subsidence at Edwards Air Force Base, Antelope Valley, California. Sacramento, Calif: U.S. Dept. of the Interior, U.S. Geological Survey, 2001.

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11

Nishikawa, Tracy. Numerical simulation of ground-water flow and land subsidence at Edwards Air Force Base, Antelope Valley, California. Sacramento, Calif: U.S. Dept. of the Interior, U.S. Geological Survey, 2001.

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12

Singh, D. J. Numerical simulation of shock-induced combustion/detonation in a premixed H2-air mixture using Navier-Stokes equations. Washington, D. C: American Institute of Aeronautics and Astronautics, 1991.

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13

Nishikawa, Tracy. Numerical simulation of ground-water flow and land subsidence at Edwards Air Force Base, Antelope Valley, California. Sacramento, Calif: U.S. Dept. of the Interior, U.S. Geological Survey, 2001.

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14

Bartolino, James R. Numerical simulation of vertical ground-water flux of the Rio Grande from ground-water temperature profiles, central New Mexico. Albuquerque, N.M: U.S. Dept. of the Interior, U.S. Geological Survey, 1999.

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15

Bartolino, James R. Numerical simulation of vertical ground-water flux of the Rio Grande from ground-water temperature profiles, Central New Mexico. Albuquerque, N.M. (5338 Montgomery NE, Suite 400, Albuquerque 87109-1311) : U.S. Dept. of the Interior, U.S. Geolgocial Survey: U.S. Geological Survey, Branch of Information Services [distributor], 1999.

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16

P, van Dam Cornelis, Duque Earl P. N, and United States. National Aeronautics and Space Administration., eds. Numerical simulation of helicopter engine plume in forward flight: Final report cooperative agreement #NCC2-5061. [Washington, DC: National Aeronautics and Space Administration, 1994.

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17

P, Van Dam C., Duque Earl P. N, and United States. National Aeronautics and Space Administration., eds. Numerical simulation of helicopter engine plume in forward flight: Final report cooperative agreement #NCC2-5061. [Washington, DC: National Aeronautics and Space Administration, 1994.

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18

M, Kwicklis E., United States. Dept. of Energy. Nevada Operations Office., and Geological Survey (U.S.), eds. Numerical simulation of air- and water-flow experiments in a block of variably saturated, fractured tuff from Yucca Mountain, Nevada. Denver, CO: U.S. Geological Survey, 1998.

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19

M, Kwicklis E., United States. Dept. of Energy. Nevada Operations Office., and Geological Survey (U.S.), eds. Numerical simulation of air- and water-flow experiments in a block of variably saturated, fractured tuff from Yucca Mountain, Nevada. Denver, CO: U.S. Dept. of the Interior, U.S. Geological Survey, 1998.

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20

Workshop on "Large-scale Scientific Computations" (2nd 1999 Sozopol, Bulgaria). Large-scale scientific computations of engineering and environmental problems II: Proceedings of the second workshop on "Large-scale scientific computations", Sozopol, Bulgaria, June 2-6, 1999. Braunschweig: Vieweg, 2000.

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21

Jayashree, Moorthy, and Langley Research Center, eds. Numerical simulation of the nonlinear response of composite plates under combined thermal and acoustic loading: Final report, for the period ended March 15, 1995. Norfolk, Va: Old Dominion University, 1995.

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22

Jayashree, Moorthy, and Langley Research Center, eds. Numerical simulation of the nonlinear response of composite plates under combined thermal and acoustic loading: Final report, for the period ended March 15, 1995. Norfolk, Va: Old Dominion University, 1995.

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23

Geological Survey (U.S.), ed. Numerical Simulation of Vertical Ground-Water Flux of the Rio Grande from Ground-Water Temperature Profiles, Central New Mexico, U.S. Geological Survey, Water-Resources Investigations Report 99-4212, etc., 1999. [S.l: s.n., 1999.

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24

Geological Survey (U.S.), ed. Numerical Simulation of Vertical Ground-Water Flux of the Rio Grande from Ground-Water Temperature Profiles, Central New Mexico, U.S. Geological Survey, Water-Resources Investigations Report 99-4212, etc., 1999. [S.l: s.n., 1999.

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25

Numerical Simulation of Canopy Flows. Springer, 2011.

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26

Dyckhoff, Harald, and Günter Groß. Numerical Simulation of Canopy Flows. Springer, 2011.

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27

Groß, Günter. Numerical Simulation of Canopy Flows. Springer London, Limited, 2012.

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28

Evaluation of temperature gradient in Advanced Automated Directional Solidification Furnace (AADSF) by numerical simulation. Bellingham, Wash: Society of Photo-Optical Instrumentation Engineers, 1996.

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29

Schumacher, Jurgen. Numerical simulation of cantilevered RAMP injector flow fields for hypervelocity fuel/air mixing enhancement. 2000.

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30

Tibaldi, Stefano, and Franco Molteni. Atmospheric Blocking in Observation and Models. Oxford University Press, 2018. http://dx.doi.org/10.1093/acrefore/9780190228620.013.611.

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The atmospheric circulation in the mid-latitudes of both hemispheres is usually dominated by westerly winds and by planetary-scale and shorter-scale synoptic waves, moving mostly from west to east. A remarkable and frequent exception to this “usual” behavior is atmospheric blocking. Blocking occurs when the usual zonal flow is hindered by the establishment of a large-amplitude, quasi-stationary, high-pressure meridional circulation structure which “blocks” the flow of the westerlies and the progression of the atmospheric waves and disturbances embedded in them. Such blocking structures can have lifetimes varying from a few days to several weeks in the most extreme cases. Their presence can strongly affect the weather of large portions of the mid-latitudes, leading to the establishment of anomalous meteorological conditions. These can take the form of strong precipitation episodes or persistent anticyclonic regimes, leading in turn to floods, extreme cold spells, heat waves, or short-lived droughts. Even air quality can be strongly influenced by the establishment of atmospheric blocking, with episodes of high concentrations of low-level ozone in summer and of particulate matter and other air pollutants in winter, particularly in highly populated urban areas.Atmospheric blocking has the tendency to occur more often in winter and in certain longitudinal quadrants, notably the Euro-Atlantic and the Pacific sectors of the Northern Hemisphere. In the Southern Hemisphere, blocking episodes are generally less frequent, and the longitudinal localization is less pronounced than in the Northern Hemisphere.Blocking has aroused the interest of atmospheric scientists since the middle of the last century, with the pioneering observational works of Berggren, Bolin, Rossby, and Rex, and has become the subject of innumerable observational and theoretical studies. The purpose of such studies was originally to find a commonly accepted structural and phenomenological definition of atmospheric blocking. The investigations went on to study blocking climatology in terms of the geographical distribution of its frequency of occurrence and the associated seasonal and inter-annual variability. Well into the second half of the 20th century, a large number of theoretical dynamic works on blocking formation and maintenance started appearing in the literature. Such theoretical studies explored a wide range of possible dynamic mechanisms, including large-amplitude planetary-scale wave dynamics, including Rossby wave breaking, multiple equilibria circulation regimes, large-scale forcing of anticyclones by synoptic-scale eddies, finite-amplitude non-linear instability theory, and influence of sea surface temperature anomalies, to name but a few. However, to date no unique theoretical model of atmospheric blocking has been formulated that can account for all of its observational characteristics.When numerical, global short- and medium-range weather predictions started being produced operationally, and with the establishment, in the late 1970s and early 1980s, of the European Centre for Medium-Range Weather Forecasts, it quickly became of relevance to assess the capability of numerical models to predict blocking with the correct space-time characteristics (e.g., location, time of onset, life span, and decay). Early studies showed that models had difficulties in correctly representing blocking as well as in connection with their large systematic (mean) errors.Despite enormous improvements in the ability of numerical models to represent atmospheric dynamics, blocking remains a challenge for global weather prediction and climate simulation models. Such modeling deficiencies have negative consequences not only for our ability to represent the observed climate but also for the possibility of producing high-quality seasonal-to-decadal predictions. For such predictions, representing the correct space-time statistics of blocking occurrence is, especially for certain geographical areas, extremely important.
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31

Preliminary control system design and analysis for the space station furnace facility thermal control system. [Marshall Space Flight Center, Ala: National Aeronautics and Space Administration, George C. Marshall Space Flight Center, 1995.

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32

Numerical simulation of air- and water-flow experiments in a block of variably saturated, fractured tuff from Yucca Mountain, Nevada. Denver, Colo: U.S. Geological Survey, 1998.

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33

Chapman, Kirby S. Develop simplified methodology to incorporate thermal comfort factors for temperature setback/setup into in-space heating and cooling design calculations: Final project report : research project 1114. [Atlanta, GA] : American Society of Heating, Refrigerating and Air-Conditioning Engineers, 1994.

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34

Numerical simulation of the nonlinear response of composite plates under combined thermal and acoustic loading: Final report, for the period ended March 15, 1995. Norfolk, Va: Old Dominion University, 1995.

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35

Xue, Yongkang, Yaoming Ma, and Qian Li. Land–Climate Interaction Over the Tibetan Plateau. Oxford University Press, 2017. http://dx.doi.org/10.1093/acrefore/9780190228620.013.592.

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The Tibetan Plateau (TP) is the largest and highest plateau on Earth. Due to its elevation, it receives much more downward shortwave radiation than other areas, which results in very strong diurnal and seasonal changes of the surface energy components and other meteorological variables, such as surface temperature and the convective atmospheric boundary layer. With such unique land process conditions on a distinct geomorphic unit, the TP has been identified as having the strongest land/atmosphere interactions in the mid-latitudes.Three major TP land/atmosphere interaction issues are presented in this article: (1) Scientists have long been aware of the role of the TP in atmospheric circulation. The view that the TP’s thermal and dynamic forcing drives the Asian monsoon has been prevalent in the literature for decades. In addition to the TP’s topographic effect, diagnostic and modeling studies have shown that the TP provides a huge, elevated heat source to the middle troposphere, and that the sensible heat pump plays a major role in the regional climate and in the formation of the Asian monsoon. Recent modeling studies, however, suggest that the south and west slopes of the Himalayas produce a strong monsoon by insulating warm and moist tropical air from the cold and dry extratropics, so the TP heat source cannot be considered as a factor for driving the Indian monsoon. The climate models’ shortcomings have been speculated to cause the discrepancies/controversies in the modeling results in this aspect. (2) The TP snow cover and Asian monsoon relationship is considered as another hot topic in TP land/atmosphere interaction studies and was proposed as early as 1884. Using ground measurements and remote sensing data available since the 1970s, a number of studies have confirmed the empirical relationship between TP snow cover and the Asian monsoon, albeit sometimes with different signs. Sensitivity studies using numerical modeling have also demonstrated the effects of snow on the monsoon but were normally tested with specified extreme snow cover conditions. There are also controversies regarding the possible mechanisms through which snow affects the monsoon. Currently, snow is no longer a factor in the statistic prediction model for the Indian monsoon prediction in the Indian Meteorological Department. These controversial issues indicate the necessity of having measurements that are more comprehensive over the TP to better understand the nature of the TP land/atmosphere interactions and evaluate the model-produced results. (3) The TP is one of the major areas in China greatly affected by land degradation due to both natural processes and anthropogenic activities. Preliminary modeling studies have been conducted to assess its possible impact on climate and regional hydrology. Assessments using global and regional models with more realistic TP land degradation data are imperative.Due to high elevation and harsh climate conditions, measurements over the TP used to be sparse. Fortunately, since the 1990s, state-of-the-art observational long-term station networks in the TP and neighboring regions have been established. Four large field experiments since 1996, among many observational activities, are presented in this article. These experiments should greatly help further research on TP land/atmosphere interactions.
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36

Sobczyk, Eugeniusz Jacek. Uciążliwość eksploatacji złóż węgla kamiennego wynikająca z warunków geologicznych i górniczych. Instytut Gospodarki Surowcami Mineralnymi i Energią PAN, 2022. http://dx.doi.org/10.33223/onermin/0222.

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Hard coal mining is characterised by features that pose numerous challenges to its current operations and cause strategic and operational problems in planning its development. The most important of these include the high capital intensity of mining investment projects and the dynamically changing environment in which the sector operates, while the long-term role of the sector is dependent on factors originating at both national and international level. At the same time, the conditions for coal mining are deteriorating, the resources more readily available in active mines are being exhausted, mining depths are increasing, temperature levels in pits are rising, transport routes for staff and materials are getting longer, effective working time is decreasing, natural hazards are increasing, and seams with an increasing content of waste rock are being mined. The mining industry is currently in a very difficult situation, both in technical (mining) and economic terms. It cannot be ignored, however, that the difficult financial situation of Polish mining companies is largely exacerbated by their high operating costs. The cost of obtaining coal and its price are two key elements that determine the level of efficiency of Polish mines. This situation could be improved by streamlining the planning processes. This would involve striving for production planning that is as predictable as possible and, on the other hand, economically efficient. In this respect, it is helpful to plan the production from operating longwalls with full awareness of the complexity of geological and mining conditions and the resulting economic consequences. The constraints on increasing the efficiency of the mining process are due to the technical potential of the mining process, organisational factors and, above all, geological and mining conditions. The main objective of the monograph is to identify relations between geological and mining parameters and the level of longwall mining costs, and their daily output. In view of the above, it was assumed that it was possible to present the relationship between the costs of longwall mining and the daily coal output from a longwall as a function of onerous geological and mining factors. The monograph presents two models of onerous geological and mining conditions, including natural hazards, deposit (seam) parameters, mining (technical) parameters and environmental factors. The models were used to calculate two onerousness indicators, Wue and WUt, which synthetically define the level of impact of onerous geological and mining conditions on the mining process in relation to: —— operating costs at longwall faces – indicator WUe, —— daily longwall mining output – indicator WUt. In the next research step, the analysis of direct relationships of selected geological and mining factors with longwall costs and the mining output level was conducted. For this purpose, two statistical models were built for the following dependent variables: unit operating cost (Model 1) and daily longwall mining output (Model 2). The models served two additional sub-objectives: interpretation of the influence of independent variables on dependent variables and point forecasting. The models were also used for forecasting purposes. Statistical models were built on the basis of historical production results of selected seven Polish mines. On the basis of variability of geological and mining conditions at 120 longwalls, the influence of individual parameters on longwall mining between 2010 and 2019 was determined. The identified relationships made it possible to formulate numerical forecast of unit production cost and daily longwall mining output in relation to the level of expected onerousness. The projection period was assumed to be 2020–2030. On this basis, an opinion was formulated on the forecast of the expected unit production costs and the output of the 259 longwalls planned to be mined at these mines. A procedure scheme was developed using the following methods: 1) Analytic Hierarchy Process (AHP) – mathematical multi-criteria decision-making method, 2) comparative multivariate analysis, 3) regression analysis, 4) Monte Carlo simulation. The utilitarian purpose of the monograph is to provide the research community with the concept of building models that can be used to solve real decision-making problems during longwall planning in hard coal mines. The layout of the monograph, consisting of an introduction, eight main sections and a conclusion, follows the objectives set out above. Section One presents the methodology used to assess the impact of onerous geological and mining conditions on the mining process. Multi-Criteria Decision Analysis (MCDA) is reviewed and basic definitions used in the following part of the paper are introduced. The section includes a description of AHP which was used in the presented analysis. Individual factors resulting from natural hazards, from the geological structure of the deposit (seam), from limitations caused by technical requirements, from the impact of mining on the environment, which affect the mining process, are described exhaustively in Section Two. Sections Three and Four present the construction of two hierarchical models of geological and mining conditions onerousness: the first in the context of extraction costs and the second in relation to daily longwall mining. The procedure for valuing the importance of their components by a group of experts (pairwise comparison of criteria and sub-criteria on the basis of Saaty’s 9-point comparison scale) is presented. The AHP method is very sensitive to even small changes in the value of the comparison matrix. In order to determine the stability of the valuation of both onerousness models, a sensitivity analysis was carried out, which is described in detail in Section Five. Section Six is devoted to the issue of constructing aggregate indices, WUe and WUt, which synthetically measure the impact of onerous geological and mining conditions on the mining process in individual longwalls and allow for a linear ordering of longwalls according to increasing levels of onerousness. Section Seven opens the research part of the work, which analyses the results of the developed models and indicators in individual mines. A detailed analysis is presented of the assessment of the impact of onerous mining conditions on mining costs in selected seams of the analysed mines, and in the case of the impact of onerous mining on daily longwall mining output, the variability of this process in individual fields (lots) of the mines is characterised. Section Eight presents the regression equations for the dependence of the costs and level of extraction on the aggregated onerousness indicators, WUe and WUt. The regression models f(KJC_N) and f(W) developed in this way are used to forecast the unit mining costs and daily output of the designed longwalls in the context of diversified geological and mining conditions. The use of regression models is of great practical importance. It makes it possible to approximate unit costs and daily output for newly designed longwall workings. The use of this knowledge may significantly improve the quality of planning processes and the effectiveness of the mining process.
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