Fundamental spray and combustion measurements of soy methyl-ester biodiesel

Although biodiesel has begun to penetrate the fuel market, its effect on injection processes, combustion and emission formation under diesel engine conditions remains somewhat unclear. Typical exhaust measurements from engines running biodiesel indicate that particulate matter, carbon monoxide and unburnt hydrocarbons are decreased, whereas nitrogen oxide emissions tend to be increased. However, these observations are the result of complex interactions between physical and chemical processes occurring in the combustion chamber, for which understanding is still needed. To characterize and decouple the physical and chemical influences of biodiesel on spray mixing, ignition, combustion and soot formation, a soy methyl-ester (SME) biodiesel is injected into a constant-volume combustion facility under diesel-like operating conditions. A range of optical diagnostics is performed, comparing biodiesel to a conventional #2 diesel at the same injection and ambient conditions. Schlieren high-speed imaging shows virtually the same vapour-phase penetration for the two fuels, while simultaneous Mie-scatter imaging shows that the maximum liquid-phase penetration of biodiesel is higher than diesel. Differences in the liquid-phase penetration are expected because of the different boiling-point temperatures of the two fuels. However, the different liquid-phase penetration does not affect overall mixing rate and downstream vapour-phase penetration because each fuel spray has similar momentum and spreading angle. For the biodiesel and diesel samples used in this study, the ignition delay and lift-off length are only slightly less for biodiesel compared to diesel, consistent with the fuel cetane number (51 for biodiesel, 46 for diesel). Because of the similarity in lift-off length, the differences in equivalence ratio distribution at the lift-off length are mainly affected by the oxygen content of the fuels. For biodiesel, the equivalence ratio is reduced, which, along with the fuel molecular structure and oxygen content, significantly affects soot formation downstream. Spatially resolved soot volume fraction measurements obtained by combining line-of-sight laser extinction measurements with planar laser-induced incandescence imaging show that the soot concentration can be reduced by an order of magnitude for biodiesel. These integrated measurements of spray mixing, combustion and quantitative soot concentration provide new validation data for the development of computational fluid dynamics spray, combustion and soot formation models suitable for the latest biofuels.This work was supported by the Spanish Ministry of Science and Innovation for Jean-Guillaume Nerva's visiting research, through the OPTICOMB project [TRA2007-67961-C03-01].Nerva, J.; Genzale, CL.; Kook, S.; García Oliver, JM.; Pickett, LM. (2013). Fundamental spray and combustion measurements of soy methyl-ester biodiesel. International Journal of Engine Research. 14(4):373-390. https://doi.org/10.1177/1468087412456688S373390144(2009). World Energy Outlook 2009. World Energy Outlook. doi:10.1787/weo-2009-enMonyem, A., & H. Van Gerpen, J. (2001). The effect of biodiesel oxidation on engine performance and emissions. Biomass and Bioenergy, 20(4), 317-325. doi:10.1016/s0961-9534(00)00095-7LAPUERTA, M., ARMAS, O., & RODRIGUEZFERNANDEZ, J. (2008). Effect of biodiesel fuels on diesel engine emissions. Progress in Energy and Combustion Science, 34(2), 198-223. doi:10.1016/j.pecs.2007.07.001Fisher, B. T., Knothe, G., & Mueller, C. J. (2010). Liquid-Phase Penetration under Unsteady In-Cylinder Conditions: Soy- and Cuphea-Derived Biodiesel Fuels Versus Conventional Diesel. Energy & Fuels, 24(9), 5163-5180. doi:10.1021/ef100594pFang, T., Lin, Y.-C., Foong, T. M., & Lee, C. (2009). Biodiesel combustion in an optical HSDI diesel engine under low load premixed combustion conditions. Fuel, 88(11), 2154-2162. doi:10.1016/j.fuel.2009.02.033Pastor, J. V., García-Oliver, J. M., Nerva, J.-G., & Giménez, B. (2011). Fuel effect on the liquid-phase penetration of an evaporating spray under transient diesel-like conditions. Fuel, 90(11), 3369-3381. doi:10.1016/j.fuel.2011.05.006Fisher, B. T., & Mueller, C. J. (2010). Liquid penetration length of heptamethylnonane and trimethylpentane under unsteady in-cylinder conditions. Fuel, 89(10), 2673-2696. doi:10.1016/j.fuel.2010.04.024Kim, H. J., Park, S. H., Suh, H. K., & Lee, C. S. (2009). Atomization and Evaporation Characteristics of Biodiesel and Dimethyl Ether Compared to Diesel Fuel in a High-Pressure Injection System. Energy & Fuels, 23(3), 1734-1742. doi:10.1021/ef800811gSuh, H. K., Roh, H. G., & Lee, C. S. (2008). Spray and Combustion Characteristics of Biodiesel∕Diesel Blended Fuel in a Direct Injection Common-Rail Diesel Engine. Journal of Engineering for Gas Turbines and Power, 130(3). doi:10.1115/1.2835354Pickett, L. M., & Siebers, D. L. (2006). Soot Formation in Diesel Fuel Jets Near the Lift-Off Length. International Journal of Engine Research, 7(2), 103-130. doi:10.1243/146808705x57793Pickett, L. M., Kook, S., Persson, H., & Andersson, Ö. (2009). Diesel fuel jet lift-off stabilization in the presence of laser-induced plasma ignition. Proceedings of the Combustion Institute, 32(2), 2793-2800. doi:10.1016/j.proci.2008.06.082Yoo, C. S., Richardson, E. S., Sankaran, R., & Chen, J. H. (2011). A DNS study on the stabilization mechanism of a turbulent lifted ethylene jet flame in highly-heated coflow. Proceedings of the Combustion Institute, 33(1), 1619-1627. doi:10.1016/j.proci.2010.06.147Pastor, J. V., Payri, R., Gimeno, J., & Nerva, J. G. (2009). Experimental Study on RME Blends: Liquid-Phase Fuel Penetration, Chemiluminescence, and Soot Luminosity in Diesel-Like Conditions. Energy & Fuels, 23(12), 5899-5915. doi:10.1021/ef9007328Benajes, J., Molina, S., Novella, R., & Amorim, R. (2010). Study on Low Temperature Combustion for Light-Duty Diesel Engines. Energy & Fuels, 24(1), 355-364. doi:10.1021/ef900832cPickett, L. M., & Siebers, D. L. (2002). An investigation of diesel soot formation processes using micro-orifices. Proceedings of the Combustion Institute, 29(1), 655-662. doi:10.1016/s1540-7489(02)80084-0Siebers, D. L., & Pickett, L. M. (2004). Injection Pressure and Orifice Diameter Effects on Soot in DI Diesel Fuel Jets. Thermo- and Fluid Dynamic Processes in Diesel Engines 2, 109-132. doi:10.1007/978-3-662-10502-3_7Pickett, L. M., & Siebers, D. L. (2004). Soot in diesel fuel jets: effects of ambient temperature, ambient density, and injection pressure. Combustion and Flame, 138(1-2), 114-135. doi:10.1016/j.combustflame.2004.04.006Cheng, A. S., Upatnieks, A., & Mueller, C. J. (2006). Investigation of the impact of biodiesel fuelling on NOx emissions using an optical direct injection diesel engine. International Journal of Engine Research, 7(4), 297-318. doi:10.1243/14680874jer05005Cheng, A. S. (Ed), Upatnieks, A., & Mueller, C. J. (2007). Investigation of Fuel Effects on Dilute, Mixing-Controlled Combustion in an Optical Direct-Injection Diesel Engine. Energy & Fuels, 21(4), 1989-2002. doi:10.1021/ef0606456Klein-Douwel, R. J. H., Donkerbroek, A. J., van Vliet, A. P., Boot, M. D., Somers, L. M. T., Baert, R. S. G., … ter Meulen, J. J. (2009). Soot and chemiluminescence in diesel combustion of bio-derived, oxygenated and reference fuels. Proceedings of the Combustion Institute, 32(2), 2817-2825. doi:10.1016/j.proci.2008.06.140Fang, T., & Lee, C. F. (2009). Bio-diesel effects on combustion processes in an HSDI diesel engine using advanced injection strategies. Proceedings of the Combustion Institute, 32(2), 2785-2792. doi:10.1016/j.proci.2008.07.031Payri, F., Pastor, J. V., Nerva, J.-G., & Garcia-Oliver, J. M. (2011). Lift-Off Length and KL Extinction Measurements of Biodiesel and Fischer-Tropsch Fuels under Quasi-Steady Diesel Engine Conditions. SAE International Journal of Engines, 4(2), 2278-2297. doi:10.4271/2011-24-0037Kook, S., & Pickett, L. M. (2012). Liquid length and vapor penetration of conventional, Fischer–Tropsch, coal-derived, and surrogate fuel sprays at high-temperature and high-pressure ambient conditions. Fuel, 93, 539-548. doi:10.1016/j.fuel.2011.10.004Settles, G. S. (2001). Schlieren and Shadowgraph Techniques. doi:10.1007/978-3-642-56640-0Pickett, L. M., Manin, J., Genzale, C. L., Siebers, D. L., Musculus, M. P. B., & Idicheria, C. A. (2011). Relationship Between Diesel Fuel Spray Vapor Penetration/Dispersion and Local Fuel Mixture Fraction. SAE International Journal of Engines, 4(1), 764-799. doi:10.4271/2011-01-0686MUSCULUS, M., & PICKETT, L. (2005). Diagnostic considerations for optical laser-extinction measurements of soot in high-pressure transient combustion environments. Combustion and Flame, 141(4), 371-391. doi:10.1016/j.combustflame.2005.01.013Williams, T. C., Shaddix, C. R., Jensen, K. A., & Suo-Anttila, J. M. (2007). Measurement of the dimensionless extinction coefficient of soot within laminar diffusion flames. International Journal of Heat and Mass Transfer, 50(7-8), 1616-1630. doi:10.1016/j.ijheatmasstransfer.2006.08.024Kook, S., & Pickett, L. M. (2011). Soot volume fraction and morphology of conventional and surrogate jet fuel sprays at 1000-K and 6.7-MPa ambient conditions. Proceedings of the Combustion Institute, 33(2), 2911-2918. doi:10.1016/j.proci.2010.05.073De Francqueville, L., Bruneaux, G., & Thirouard, B. (2010). Soot Volume Fraction Measurements in a Gasoline Direct Injection Engine by Combined Laser Induced Incandescence and Laser Extinction Method. SAE International Journal of Engines, 3(1), 163-182. doi:10.4271/2010-01-0346Musculus, M. P. B., & Kattke, K. (2009). Entrainment Waves in Diesel Jets. SAE International Journal of Engines, 2(1), 1170-1193. doi:10.4271/2009-01-1355Desantes, J. M., Pastor, J. V., García-Oliver, J. M., & Pastor, J. M. (2009). A 1D model for the description of mixing-controlled reacting diesel sprays. Combustion and Flame, 156(1), 234-249. doi:10.1016/j.combustflame.2008.10.008Idicheria, C. A., & Pickett, L. M. (2011). Ignition, soot formation, and end-of-combustion transients in diesel combustion under high-EGR conditions. International Journal of Engine Research, 12(4), 376-392. doi:10.1177/1468087411399505Aizawa, T., & Kosaka, H. (2008). Investigation of early soot formation process in a diesel spray flame via excitation—emission matrix using a multi-wavelength laser source. International Journal of Engine Research, 9(1), 79-97. doi:10.1243/14680874jer01407Bruneaux, G. (2008). Combustion structure of free and wall-impinging diesel jets by simultaneous laser-induced fluorescence of formaldehyde, poly-aromatic hydrocarbons, and hydroxides. International Journal of Engine Research, 9(3), 249-265. doi:10.1243/14680874jer0010

Geometry and field theory in multi-fractional spacetime

We construct a theory of fields living on continuous geometries with fractional Hausdorff and spectral dimensions, focussing on a flat background analogous to Minkowski spacetime. After reviewing the properties of fractional spaces with fixed dimension, presented in a companion paper, we generalize to a multi-fractional scenario inspired by multi-fractal geometry, where the dimension changes with the scale. This is related to the renormalization group properties of fractional field theories, illustrated by the example of a scalar field. Depending on the symmetries of the Lagrangian, one can define two models. In one of them, the effective dimension flows from 2 in the ultraviolet (UV) and geometry constrains the infrared limit to be four-dimensional. At the UV critical value, the model is rendered power-counting renormalizable. However, this is not the most fundamental regime. Compelling arguments of fractal geometry require an extension of the fractional action measure to complex order. In doing so, we obtain a hierarchy of scales characterizing different geometric regimes. At very small scales, discrete symmetries emerge and the notion of a continuous spacetime begins to blur, until one reaches a fundamental scale and an ultra-microscopic fractal structure. This fine hierarchy of geometries has implications for non-commutative theories and discrete quantum gravity. In the latter case, the present model can be viewed as a top-down realization of a quantum-discrete to classical-continuum transition.Comment: 1+82 pages, 1 figure, 2 tables. v2-3: discussions clarified and improved (especially section 4.5), typos corrected, references added; v4: further typos correcte

Human skin commensals augment Staphylococcus aureus pathogenesis

All bacterial infections occur within a polymicrobial environment, from which a pathogen population emerges to establish disease within a host. Emphasis has been placed on prevention of pathogen dominance by competing microflora acting as probiotics1. Here we show that the virulence of the human pathogen Staphylococcus aureus is augmented by native, polymicrobial, commensal skin flora and individual species acting as ‘proinfectious agents’. The outcome is pathogen proliferation, but not commensal. Pathogenesis augmentation can be mediated by particulate cell wall peptidoglycan, reducing the S. aureus infectious dose by over 1,000-fold. This phenomenon occurs using a range of S. aureus strains and infection models and is not mediated by established receptor-mediated pathways including Nod1, Nod2, Myd88 and the NLPR3 inflammasome. During mouse sepsis, augmentation depends on liver-resident macrophages (Kupffer cells) that capture and internalize both the pathogen and the proinfectious agent, leading to reduced production of reactive oxygen species, pathogen survival and subsequent multiple liver abscess formation. The augmented infection model more closely resembles the natural situation and establishes the role of resident environmental microflora in the initiation of disease by an invading pathogen. As the human microflora is ubiquitous2, its role in increasing susceptibility to infection by S. aureus highlights potential strategies for disease prevention