113 research outputs found

    Sugarcane Energy Use: Accounting Of Feedstock Energy Considering Current Agro-industrial Trends And Their Feasibility

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    The sugarcane agro-industry is seen as a great opportunity for economic and industrial development in many sugarcane-producing countries. Important changes happening in recent decades have converted the sugar mill from being just a food producer into a diversified production factory. The sugar mill has become a multipurpose factory since it produces food, energy, and biofuels at present. The key cause of this change is the use of sugarcane agro-industrial residues as feedstock for energy cogeneration and biofuel production. The main aim of this paper is to carry out an assessment on sugarcane feedstock availability and its energy use in the sugar mill. The trade-off on sugarcane bagasse energy use (electricity cogeneration vs. bioethanol production), considering the agro-industrial development level, is analyzed in this work, too. The better options in each case are highlighted. The main environmental and techno-economic aspects concerning the sugarcane agro-industry were taken into account during the assessment process. The most promising trends of the sugarcane agro-industry and the barriers to overcome in its implementation are pointed out. © 2013 Pippo and Luengo; licensee Springer.41113Zanzi, R., Sjöström, K., Björnbom, E., Rapid high-temperature pyrolysis of biomass in a free fall reactor (1996) Fuel, 75 (5), pp. 545-550Jenkins, B.M., Baxter, L.L., Miles Jr., T.R., Miles, T.R., Combustion properties of biomass (1998) Fuel Process Technol, 54 (1-3), pp. 17-46Dermibas, A., Combustion characteristic of different biomass fuels (2004) Prog. Energy Combust. Sci, 30, pp. 219-230Alonso, P.W., Luengo, C.A., Alonsoamador, M.A.L., Garzone, P., Cornacchia, G., Energy recovery from sugarcane-trash in the light of second generation biofuels. Part 1: Current situation and environmental aspects (2011) Waste Biomass Valor, 2, pp. 1-16Eddine, B.T., Salah, M.M., Solid waste as renewable source of energy: Current and future possibility in Algeria (2012) Int. J. Energy Env. Eng, 3, p. 17Pandyaswargo, A.H., Onoda, H., Nagata, K., Energy recovery potential and life cycle impact assessment of municipal solid waste management technologies in Asian countries using ELP model (2012) Int. J. Energy Env. Eng, 3, p. 28Goldemberg, J., Ethanol for a sustainable energy future (2007) Science, 315, pp. 808-810Moreira, J., Goldemberg, J., The alcohol program (1999) Energy Policy, 27 (4), pp. 229-245LĂšbre, L.R.E., Pereira, A.S., Simoes, A.F., Biofuels and sustainable energy development in Brazil (2011) World Dev, 39 (6), pp. 1026-1036Macedo, I.C., (2005) Sugarcane's Energy: Twelve Studies On Brazilian Sugarcane Agribusiness and Its Sustainability (Original In Portuguese), , 1st edition. UNICA, Sao Paulo(2006) Biofuels In Brazil: Realities and Perspectives. (Original In Portuguese). BiocombustĂ­veis No Brasil Realidades E Perspectivas, p. 21. , http://www.itamaraty.gov.br/imagens-e-textos/temas-brasileiros-1/portugues/biocombustiveis-nobrasil, Ferraz-Dias-de-Moraes MA Considerations on ethanol industry of Brazil, Accessed NovBorges, J.M.M., Lecture: Original in Portuguese (1986) Proceeding Sopral, SĂŁo Paulo, BrasĂ­lia, 1986, pp. 18-20Larson, E.D., Jin, H., Celik, F.E., (2005) Gasification-based Fuels and Electricity Production From Biomass, , Without and with carbon capture and storage. Biofuels, Princeton(1989) ProĂĄlcool: Fundamentals and Perspectives, , COPERSUCAR, (Original in Portuguese) [PROÀLCOOL FUNDAMENTOS E PERSPECTIVAS]. COPERSUCAR, Maio(2008) Profile of Productions Units By States and Profile of Sugar and Ethanol Sector In Brazil: Situation Observed From November 2007 to April 2008, pp. 13-16. , National Company of Supply (CONAB), (original in Portuguese). National Company of Supply, BrasiliaFrança, R., Nogueira, L.A.H., Seventy questions to understand ethanol. (Original in Portuguese) [Setenta questĂ”es para entender o etanol] (2008) Revista Veja, 2052, pp. 104-114Suleiman, J.H., (2005) Manoel Regis Lima Verde L, de Carvalho Macedo I, , PNUD-CTC, Piracicaba, BrazilMerola, S.S., Tornatore, C., Marchitto, L., Valentino, G., Corcione, F.E., Experimental investigations of butanol-gasoline blends effects on the combustion process in a SI engine (2012) Int. J. Energy Env Eng, 3, p. 6(2010), http://www.indiansugar.com/SugarMap.aspx, ISMA Atlas of sugar mills in India, Accessed 09 Nov 2012(2012), http://www.sugartech.co.za/factories/index.php, Sugar Engineers Sugar factories of the world, Accessed 09 Nov 2012Alonso, P.W., Garzone, P., Cornacchia, G., Agro-industry sugarcane residues disposal: The trends of their conversion into energy carriers in Cuba (2007) Waste Manage, 27, pp. 869-885Alonso-Pippo, W., Luengo, C.A., Koehlinger, J., Garzone, P., Cornacchia, G., Sugarcane energy use: The Cuban case (2008) Energy Policy, 36 (6), p. 21632181Alonso, P.W., Luengo, C.A., Alonsoamador, M.A.L., Garzone, P., Cornacchia, G., Energy recovery from sugarcane-trash in the light of 2nd generation biofuels. Part 2: Socio-economic aspects and techno economic analysis (2011) Waste Biomass Valor, 2, pp. 257-266Larson, E.D., Williams, R.H., Leal, L.V., Regis, M., A review of biomass integrated-gasifier/gas turbine combined cycle technology and its application in sugarcane industries with an analysis for Cuba (2001) Energy For Sustainable Development, 5 (1), pp. 54-76SĂĄnchez, T.O., Cardona, A.C.A., Fuel ethanol production (Original in Spanish) (2007) Tizan (ed) [ProducciĂłn De Alcohol Carburante Una Alternative Para El Desarrollo Agro-industrial], p. 380. , Manizales, Caldas, ColombiaFernĂĄndez, R.J., PĂ©rez, J.A., PĂ©rez, S.O., Alonso, P.W., Characterization of industrial and agricultural residues of sugarcane for obtaining Biooil (2004) International Conference of Sugarcane Derivates. Diversification, , [Conferencia Internacional de Derivados de la caña de azĂșcar. DiversificaciĂłn 2004.], ICIDCA, La HabanaHugot, E., (1986) Handbook of Cane Sugar Engineering, , 3rd edition. Elsevier Science, New YorkStefano, M., Johan, M., Guido, Z., Techno-economic evaluation of 2nd generation bioethanol production from sugar cane bagasse and leaves integrated with sugar-based ethanol process (2012) Biotechnol. Biofuels, 5, p. 22Dias, M.O.S., Junqueira, T.L., Cavalet, O., Cunha, M.P., Jesus, C.D.F., Rosell, C.E.V., Filho, R.M., Bonomi, A., Integrated versus stand-alone second generation ethanol production from sugarcane bagasse and trash (2012) Bioresource Technol, 103, pp. 152-161Walter, A., Dolzan, P., QuilodrĂĄn, O., de Oliveira, J.G., da Silva, C., Piacente, F., Segerstedt, A., Sustainability assessment of bio-ethanol production in Brazil considering land use change. GHG emissions and socio-economic aspects (2011) Energy Policy, 39, pp. 5703-5716(2012) Statistics division, p. 12. , http://faostat.fao.org/site/567/DesktopDefault.aspx?PageID=567#ancor, Accessed July FAOSTAT CROPS(2012), http://www.oil-price.net/?gclid=CIai0Ym_ubECFQgEnQodjTgAwA, Oil-price.net, Accessed 27 July 201

    Biopitch produced from eucalyptus wood pyrolysis liquids as a renewable binder for carbon electrode manufacture

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    Interest in biomass as a clean source of fuel, chemicals and materials is growing fast. What is attractive about biomass is its renewability and that it is CO2 balanced and sulfur-free. Biomass pyrolysis produces charcoal, bio-oil and gases in different proportions, depending on the technology and raw material used. In this study biopitch, a substitute for fossil pitches in electrodes, was produced from bio-oil distillation in bench-scale equipment. Biopitch and charcoal were mixed and thermically modified to give prebaked electrodes. The physico-chemical and mechanical properties of the biopitch and final electrodes were measured and compared with those of coal tar and petroleum materials. Despite their similar application, biomaterials are structurally and chemically different from minerals. The oxygen content in biopitch is ca 20 wt% and in mineral pitches it is no more than 2 wt%. Characterization experiments for electrode samples measured electrical resistivity, Young's modulus, rupture strength, density, porosity and proximate analysis.127132Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP

    Natural clusters of tuberous sclerosis complex (TSC)-associated neuropsychiatric disorders (TAND): new findings from the TOSCA TAND research project.

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    BACKGROUND: Tuberous sclerosis complex (TSC)-associated neuropsychiatric disorders (TAND) have unique, individual patterns that pose significant challenges for diagnosis, psycho-education, and intervention planning. A recent study suggested that it may be feasible to use TAND Checklist data and data-driven methods to generate natural TAND clusters. However, the study had a small sample size and data from only two countries. Here, we investigated the replicability of identifying natural TAND clusters from a larger and more diverse sample from the TOSCA study. METHODS: As part of the TOSCA international TSC registry study, this embedded research project collected TAND Checklist data from individuals with TSC. Correlation coefficients were calculated for TAND variables to generate a correlation matrix. Hierarchical cluster and factor analysis methods were used for data reduction and identification of natural TAND clusters. RESULTS: A total of 85 individuals with TSC (female:male, 40:45) from 7 countries were enrolled. Cluster analysis grouped the TAND variables into 6 clusters: a scholastic cluster (reading, writing, spelling, mathematics, visuo-spatial difficulties, disorientation), a hyperactive/impulsive cluster (hyperactivity, impulsivity, self-injurious behavior), a mood/anxiety cluster (anxiety, depressed mood, sleep difficulties, shyness), a neuropsychological cluster (attention/concentration difficulties, memory, attention, dual/multi-tasking, executive skills deficits), a dysregulated behavior cluster (mood swings, aggressive outbursts, temper tantrums), and an autism spectrum disorder (ASD)-like cluster (delayed language, poor eye contact, repetitive behaviors, unusual use of language, inflexibility, difficulties associated with eating). The natural clusters mapped reasonably well onto the six-factor solution generated. Comparison between cluster and factor solutions from this study and the earlier feasibility study showed significant similarity, particularly in cluster solutions. CONCLUSIONS: Results from this TOSCA research project in an independent international data set showed that the combination of cluster analysis and factor analysis may be able to identify clinically meaningful natural TAND clusters. Findings were remarkably similar to those identified in the earlier feasibility study, supporting the potential robustness of these natural TAND clusters. Further steps should include examination of larger samples, investigation of internal consistency, and evaluation of the robustness of the proposed natural clusters

    Search for the Zγ decay mode of new high-mass resonances in pp collisions at √s = 13 TeV with the ATLAS detector

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    This letter presents a search for narrow, high-mass resonances in the Zγ final state with the Z boson decaying into a pair of electrons or muons. The √s = 13 TeV pp collision data were recorded by the ATLAS detector at the CERN Large Hadron Collider and have an integrated luminosity of 140 fb−1. The data are found to be in agreement with the Standard Model background expectation. Upper limits are set on the resonance production cross section times the decay branching ratio into Zγ. For spin-0 resonances produced via gluon–gluon fusion, the observed limits at 95% confidence level vary between 65.5 fb and 0.6 fb, while for spin-2 resonances produced via gluon–gluon fusion (or quark–antiquark initial states) limits vary between 77.4 (76.1) fb and 0.6 (0.5) fb, for the mass range from 220 GeV to 3400 GeV

    Search for single production of vector-like T quarks decaying into Ht or Zt in pp collisions at s√ = 13 TeV with the ATLAS detector

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    This paper describes a search for the single production of an up-type vector-like quark (T) decaying as T → Ht or T → Zt. The search utilises a dataset of pp collisions at s√ = 13 TeV collected with the ATLAS detector during the 2015–2018 data-taking period of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb−1. Data are analysed in final states containing a single lepton with multiple jets and b-jets. The presence of boosted heavy resonances in the event is exploited to discriminate the signal from the Standard Model background. No significant excess above the Standard Model expectation is observed, and 95% CL upper limits are set on the production cross section of T quarks in different decay channels. The results are interpreted in several benchmark scenarios to set limits on the mass and universal coupling strength (Îș) of the vector-like quark. For singlet T quarks, Îș values above 0.53 are excluded for all masses below 2.3 TeV. At a mass of 1.6 TeV, Îș values as low as 0.35 are excluded. For T quarks in the doublet scenario, where the production cross section is much lower, Îș values above 0.72 are excluded for all masses below 1.7 TeV, and this exclusion is extended to Îș above 0.55 for low masses around 1.0 TeV

    Search for excited τ-leptons and leptoquarks in the final state with τ-leptons and jets in pp collisions at s√ = 13 TeV with the ATLAS detector

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    A search is reported for excited τ-leptons and leptoquarks in events with two hadronically decaying τ-leptons and two or more jets. The search uses proton-proton (pp) collision data at s√ = 13 TeV recorded by the ATLAS experiment during the Run 2 of the Large Hadron Collider in 2015–2018. The total integrated luminosity is 139 fb−1. The excited τ-lepton is assumed to be produced and to decay via a four-fermion contact interaction into an ordinary τ-lepton and a quark-antiquark pair. The leptoquarks are assumed to be produced in pairs via the strong interaction, and each leptoquark is assumed to couple to a charm or lighter quark and a τ-lepton. No excess over the background prediction is observed. Excited τ-leptons with masses below 2.8 TeV are excluded at 95% CL in scenarios with the contact interaction scale Λ set to 10 TeV. At the extreme limit of model validity where Λ is set equal to the excited τ-lepton mass, excited τ-leptons with masses below 4.6 TeV are excluded. Leptoquarks with masses below 1.3 TeV are excluded at 95% CL if their branching ratio to a charm quark and a τ-lepton equals 1. The analysis does not exploit flavour-tagging in the signal region

    Measurement of the cross-sections of the electroweak and total production of a Zγ pair in association with two jets in pp collisions at √s = 13 TeV with the ATLAS detector

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    This Letter presents the measurement of the fiducial and differential cross-sections of the electroweak production of a ZÎł pair in association with two jets. The analysis uses 140 fb−1 of LHC proton–proton collision data taken at √s = 13 TeV recorded by the ATLAS detector during the years 2015–2018. Events with a Z boson candidate decaying into either an e+e− or ÎŒ+Ό− pair, a photon and two jets are selected. The electroweak component is extracted by requiring a large dijet invariant mass and by using the information about the centrality of the system and is measured with an observed and expected significance well above five standard deviations. The fiducial pp → ZÎł jj cross-section for the electroweak production is measured to be 3.6 ± 0.5 fb. The total fiducial cross-section that also includes contributions where the jets arise from strong interactions is measured to be 16.8+2.0 −1.8 fb. The results are consistent with the Standard Model predictions. Differential cross-sections are also measured using the same events and are compared with parton-shower Monte Carlo simulations. Good agreement is observed between data and predictions

    Search for heavy Higgs bosons with flavour-violating couplings in multi-lepton plus b-jets final states in pp collisions at 13 TeV with the ATLAS detector

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    A search for new heavy scalars with flavour-violating decays in final states with multiple leptons and b-tagged jets is presented. The results are interpreted in terms of a general two-Higgs-doublet model involving an additional scalar with couplings to the top-quark and the three up-type quarks (ρtt, ρtc, and ρtu). The targeted signals lead to final states with either a same-sign top-quark pair, three top-quarks, or four top-quarks. The search is based on a data sample of proton-proton collisions at √s = 13 TeV recorded with the ATLAS detector during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb−1. Events are categorised depending on the multiplicity of light charged leptons (electrons or muons), total lepton charge, and a deep-neural-network output to enhance the purity of each of the signals. Masses of an additional scalar boson mH between 200 − 630 GeV with couplings ρtt = 0.4, ρtc = 0.2, and ρtu = 0.2 are excluded at 95% confidence level. Additional interpretations are provided in models of R-parity violating supersymmetry, motivated by the recent flavour and (g − 2)ÎŒ anomalies

    Search for a new heavy scalar particle decaying into a Higgs boson and a new scalar singlet in final states with one or two light leptons and a pair of τ-leptons with the ATLAS detector

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    A search for a new heavy scalar particle X decaying into a Standard Model (SM) Higgs boson and a new singlet scalar particle S is presented. The search uses a proton-proton (pp) collision data sample with an integrated luminosity of 140 fb−1 recorded at a centre-of-mass energy of s√ = 13 TeV with the ATLAS detector at the Large Hadron Collider. The most sensitive mass parameter space is explored in X mass ranging from 500 to 1500 GeV, with the corresponding S mass in the range 200–500 GeV. The search selects events with two hadronically decaying τ-lepton candidates from H → τ+τ− decays and one or two light leptons (ℓ = e, ÎŒ) from S → VV (V = W, Z) decays while the remaining V boson decays hadronically or to neutrinos. A multivariate discriminant based on event kinematics is used to separate the signal from the background. No excess is observed beyond the expected SM background and 95% confidence level upper limits between 72 fb and 542 fb are derived on the cross-section σ(pp → X → SH) assuming the same SM-Higgs boson-like decay branching ratios for the S → VV decay. Upper limits on the visible cross-sections σ(pp → X → SH → WWττ) and σ(pp → X → SH → ZZττ) are also set in the ranges 3–26 fb and 6–33 fb, respectively
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