124 research outputs found

    DISEÑO DE UNA INCUBADORA AVÍCOLA SUSTENTABLE, AUTOMATIZADA CON MICROPROCESADORES Y MONITOREADA CON APLICACIÓN MÓVIL (DESIGN OF A SUSTAINABLE POULTRY INCUBATOR, AUTOMATED WITH MICROPROCESSORS AND MONITORED WITH MOBILE APPLICATION)

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    Resumen El presente proyecto se desarrolló en las instalaciones del Instituto Tecnológico de Pinotepa. En la población de Santiago Pinotepa Nacional, Oax con la finalidad de realizar un primer acercamiento, a la solución de la problemática que se presenta en la comunidad avícola de esta población, con respecto a la producción de la avicultura. Se pretende eliminar la dependencia que tiene el avicultor, al comprar los pollos recién nacidos, lo que causa un porcentaje de alta mortalidad. El artículo presenta el resultado del proyecto denominado “Diseño de una Incubadora Avícola Sustentable Automatizada con Microprocesadores y Monitoreada Con Aplicación Móvil” que tiene como objetivo aumentar producción avícola en la población reduciendo los costos de incubación, diseñando un Sistema de Incubación sostenible, automatizada con un Microprocesador ATmega2560 y Monitoreada con Aplicación Móvil. El cual se Implementó tecnologías actuales para el control y monitoreo del sistema, en donde los parámetros eficientes de operación como la humedad, la temperatura y el movimiento fueron controlados de manera autónoma por sensores DHT11 este es un sensor digital de temperatura y humedad relativa, mediante la lógica difusa. El monitoreo fue diseñando en un lenguaje de programación app inventor con Arduino en una computadora portátil. El diseño de los sistemas de control difuso de temperatura y rotación se desarrollaron mediante la metodología del experto, se implementaron en una plataforma hardware DsPIC y finalmente, se validaron mediante tres enfoques: computacional, control y aplicación. Se obtuvo un 95% de eclosión, por lo que se concluye que es viable realizar la incubación artificial con este prototipo de incubadora para huevos. Palabras clave: Automatización, control, incubación, sensor, temperatura. Abstract This project was developed at the facilities of the Technological Institute of Pinotepa. In the town of Santiago Pinotepa Nacional, Oax with the aim of making a first approach, to the solution of the problem that occurs in the poultry community of this population, with respect to the incomplete production of poultry. It is intended to eliminate the dependence that the poultry farmer has, when buying newborn chickens, which causes a high mortality rate. The article presents the implementation of a This project aims to increase poultry production in the population by reducing incubation costs, designing a sustainable Automated Incubation System with ATmega2560 Microprocessor and Monitored with Mobile Application. Implementing current technologies for the control and monitoring of the system, where efficient operating parameters such as humidity, temperature and movement are controlled autonomously by sensors DHT11 is a digital temperature and relative humidity sensor, using fuzzy logic. The monitoring was designing in an inventor app programming language with an Arduino laptop. The design of the diffuse temperature and rotation control systems were developed using the expert's methodology, they were implemented in a DsPIC hardware platform and finally, they were validated using three approaches: computational, control and application. 95% hatching was obtained, so it is concluded that it is feasible to carry out artificial incubation with this prototype incubator for bird eggs. Keywords: Automation, control, incubation, sensor, temperature

    El huerto escolar : recurso educativo del geocentro

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    El trabajo obtuvo un premio de la Modalidad A de los Premios Tomás García Verdejo a las buenas practicas educativas en la Comunidad Autónoma de Extremadura para el curso 2011-2012Se describe un proyecto que consistió en crear un huerto escolar con el que se quería enfatizar la importancia de la protección del medio ambiente y fomentar el respeto y el amor por la naturaleza, valorando su importancia e interdependencia con la vida de los seres humanos. Se detallan las actividades llevadas a cabo dirigidas tanto a alumnos de infantil como de primariaExtremaduraES

    Multiplicity dependence of light (anti-)nuclei production in p–Pb collisions at sNN=5.02 TeV

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    The measurement of the deuteron and anti-deuteron production in the rapidity range −1 < y < 0 as a function of transverse momentum and event multiplicity in p–Pb collisions at √sNN = 5.02 TeV is presented. (Anti-)deuterons are identified via their specific energy loss dE/dx and via their time-of- flight. Their production in p–Pb collisions is compared to pp and Pb–Pb collisions and is discussed within the context of thermal and coalescence models. The ratio of integrated yields of deuterons to protons (d/p) shows a significant increase as a function of the charged-particle multiplicity of the event starting from values similar to those observed in pp collisions at low multiplicities and approaching those observed in Pb–Pb collisions at high multiplicities. The mean transverse particle momenta are extracted from the deuteron spectra and the values are similar to those obtained for p and particles. Thus, deuteron spectra do not follow mass ordering. This behaviour is in contrast to the trend observed for non-composite particles in p–Pb collisions. In addition, the production of the rare 3He and 3He nuclei has been studied. The spectrum corresponding to all non-single diffractive p-Pb collisions is obtained in the rapidity window −1 < y < 0 and the pT-integrated yield dN/dy is extracted. It is found that the yields of protons, deuterons, and 3He, normalised by the spin degeneracy factor, follow an exponential decrease with mass number

    Measurement of electrons from semileptonic heavy-flavour hadron decays at midrapidity in pp and Pb–Pb collisions at √sNN = 5.02 TeV

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    The differential invariant yield as a function of transverse momentum (pT) of electrons from semileptonic heavy-flavour hadron decays was measured at midrapidity in central (0–10%), semi-central (30–50%) and peripheral (60–80%) lead–lead (Pb–Pb) collisions at √sNN = 5.02 TeV in the pT intervals 0.5–26 GeV/c (0–10% and 30–50%) and 0.5–10 GeV/c (60–80%). The production cross section in proton–proton (pp) collisions at √s = 5.02 TeV was measured as well in 0.5 < pT < 10 GeV/c and it lies close to the upper band of perturbative QCD calculation uncertainties up to pT = 5 GeV/c and close to the mean value for larger pT. The modification of the electron yield with respect to what is expected for an incoherent superposition of nucleon–nucleon collisions is evaluated by measuring the nuclear modification factor RAA. The measurement of the RAA in different centrality classes allows in-medium energy loss of charm and beauty quarks to be investigated. The RAA shows a suppression with respect to unity at intermediate pT, which increases while moving towards more central collisions. Moreover, the measured RAA is sensitive to the modification of the parton distribution functions (PDF) in nuclei, like nuclear shadowing, which causes a suppression of the heavy-quark production at low pT in heavy-ion collisions at LHC

    Measurement of prompt D0^{0}, D+^{+}, D+^{*+}, and DS+ {\mathrm{D}}_{\mathrm{S}}^{+} production in p–Pb collisions at sNN \sqrt{{\mathrm{s}}_{\mathrm{NN}}} = 5.02 TeV

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    International audienceThe measurement of the production of prompt D0^{0}, D+^{+}, D+^{*+}, and DS+ {\mathrm{D}}_{\mathrm{S}}^{+} mesons in proton–lead (p–Pb) collisions at the centre-of-mass energy per nucleon pair of sNN \sqrt{s_{\mathrm{NN}}} = 5.02 TeV, with an integrated luminosity of 292 ± 11 μb1^{−1}, are reported. Differential production cross sections are measured at mid-rapidity (−0.96 < ycms_{cms}< 0.04) as a function of transverse momentum (pT_{T}) in the intervals 0 < pT_{T}< 36 GeV/c for D0^{0}, 1 < pT_{T}< 36 GeV/c for D+^{+} and D+^{*+}, and 2 < pT_{T}< 24 GeV/c for D+^{+} mesons. For each species, the nuclear modification factor RpPb_{pPb} is calculated as a function of pT_{T} using a proton-proton (pp) ref- erence measured at the same collision energy. The results are compatible with unity in the whole pT_{T} range. The average of the non-strange D mesons RpPb_{pPb} is compared with theoretical model predictions that include initial-state effects and parton transport model predictions. The pT_{T} dependence of the D0^{0}, D+^{+}, and D+^{*+} nuclear modification factors is also reported in the interval 1 < pT_{T}< 36 GeV/c as a function of the collision centrality, and the central-to-peripheral ratios are computed from the D-meson yields measured in different centrality classes. The results are further compared with charged-particle measurements and a similar trend is observed in all the centrality classes. The ratios of the pT_{T}-differential cross sections of D0^{0}, D+^{+}, D+^{*+}, and DS+ {\mathrm{D}}_{\mathrm{S}}^{+} mesons are also reported. The DS+ {\mathrm{D}}_{\mathrm{S}}^{+} and D+^{+} yields are compared as a function of the charged-particle multiplicity for several pT_{T} intervals. No modification in the relative abundances of the four species is observed with respect to pp collisions within the statistical and systematic uncertainties

    Azimuthal correlations of prompt D mesons with charged particles in pp and p–Pb collisions at sNN\sqrt{s_{NN}} = 5.02 TeV

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    International audienceThe measurement of the azimuthal-correlation function of prompt D mesons with charged particles in pp collisions at s=5.02 TeV\sqrt{s} =5.02\ \hbox {TeV} and p–Pb collisions at sNN=5.02 TeV\sqrt{s_{\mathrm{NN}}} = 5.02\ \hbox {TeV} with the ALICE detector at the LHC is reported. The D0\mathrm{D}^{0}, D+\mathrm{D}^{+} , and D+\mathrm{D}^{*+} mesons, together with their charge conjugates, were reconstructed at midrapidity in the transverse momentum interval 30.3 GeV/c3 0.3\ \hbox {GeV}/c and pseudorapidity η<0.8|\eta | < 0.8. The properties of the correlation peaks appearing in the near- and away-side regions (for Δφ0\Delta \varphi \approx 0 and Δφπ\Delta \varphi \approx \pi , respectively) were extracted via a fit to the azimuthal correlation functions. The shape of the correlation functions and the near- and away-side peak features are found to be consistent in pp and p–Pb collisions, showing no modifications due to nuclear effects within uncertainties. The results are compared with predictions from Monte Carlo simulations performed with the PYTHIA, POWHEG+PYTHIA, HERWIG, and EPOS 3 event generators

    Λc+\Lambda_\mathrm{c}^+ production in Pb-Pb collisions at sNN=5.02\sqrt{s_{\rm NN}} = 5.02 TeVUC

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    A measurement of the production of prompt Λc+\Lambda_\mathrm{c}^+ baryons in Pb–Pb collisions at sNN\sqrt{s_{\rm NN}} = 5.02 TeV with the ALICE detector at the LHC is reported. The Λc+\Lambda_\mathrm{c}^+ and Λcˉ\bar{\Lambda_\mathrm{c}}^- were reconstructed at midrapidity (|y|<0.5) via the hadronic decay channel Λc+\Lambda_\mathrm{c}^+→pKS0_{\rm S}^0 (and charge conjugate) in the transverse momentum and centrality intervals 6 < pTp_{\rm T} < 12 GeV/ c and 0–80%. The Λc+\Lambda_\mathrm{c}^+/D0^0 ratio, which is sensitive to the charm quark hadronisation mechanisms in the medium, is measured and found to be larger than the ratio measured in minimum-bias pp collisions at s\sqrt{s} = 7 TeV and in p–Pb collisions at sNN\sqrt{s_{\rm NN}} = 5.02 TeV. In particular, the values in p–Pb and Pb–Pb collisions differ by about two standard deviations of the combined statistical and systematic uncertainties in the common pTp_{\rm T} interval covered by the measurements in the two collision systems. The Λc+\Lambda_\mathrm{c}^+/D0^0 ratio is also compared with model calculations including different implementations of charm quark hadronisation. The measured ratio is reproduced by models implementing a pure coalescence scenario, while adding a fragmentation contribution leads to an underestimation. The Λc+\Lambda_\mathrm{c}^+ nuclear modification factor, RAAR_{\rm AA}, is also presented. The measured values of the RAAR_{\rm AA} of Λc+\Lambda_\mathrm{c}^+, Ds+_{\rm s}^+ and non-strange D mesons are compatible within the combined statistical and systematic uncertainties. They show, however, a hint of a hierarchy (RAAD0R_{\rm AA}^{D^0} < RAADs+R_{\rm AA}^{D_\mathrm{s}^+} < RAAΛc+R_{\rm AA}^{\Lambda_\mathrm{c}^+}) , conceivable with a contribution from coalescence mechanisms to charm hadron formation in the medium

    Longitudinal and azimuthal evolution of two-particle transverse momentum correlations in Pb-Pb collisions at sNN=2.76TeV\sqrt{s_{\rm{NN}}} = 2.76 TeV

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    This paper presents the first measurements of the charge independent (CI) and charge dependent (CD) two-particle transverse momentum correlators G2CI and G2CD in Pb–Pb collisions at sNN=2.76TeV by the ALICE collaboration. The two-particle transverse momentum correlator G2 was introduced as a measure of the momentum current transfer between neighboring system cells. The correlators are measured as a function of pair separation in pseudorapidity (Δ η ) and azimuth (Δ φ ) and as a function of collision centrality. From peripheral to central collisions, the correlator G2CI exhibits a longitudinal broadening while undergoing a monotonic azimuthal narrowing. By contrast, G2CD exhibits a narrowing along both dimensions. These features are not reproduced by models such as HIJING and AMPT. However, the observed narrowing of the correlators from peripheral to central collisions is expected to result from the stronger transverse flow profiles produced in more central collisions and the longitudinal broadening is predicted to be sensitive to momentum currents and the shear viscosity per unit of entropy density η/s of the matter produced in the collisions. The observed broadening is found to be consistent with the hypothesized lower bound of η/s and is in qualitative agreement with values obtained from anisotropic flow measurements.This paper presents the first measurements of the charge independent (CI) and charge dependent (CD) two-particle transverse momentum correlators G2CIG_{2}^{\rm CI} and G2CDG_{2}^{\rm CD} in Pb--Pb collisions at \sqrt{s_{\text{NN}}} = 2.76\;\text{\TeVe} by the ALICE collaboration. The two-particle transverse momentum correlator G2G_{2} was introduced as a measure of the momentum current transfer between neighbouring system cells. The correlators are measured as a function of pair separation in pseudorapidity (Δη\Delta \eta) and azimuth (Δφ\Delta \varphi) and as a function of collision centrality. From peripheral to central collisions, the correlator G2CIG_{2}^{\rm CI} exhibits a longitudinal broadening while undergoing a monotonic azimuthal narrowing. By contrast, G2CDG_{2}^{\rm CD} exhibits a narrowing along both dimensions. These features are not reproduced by models such as HIJING and AMPT. However, the observed narrowing of the correlators from peripheral to central collisions is expected to result from the stronger transverse flow profiles produced in more central collisions and the longitudinal broadening is predicted to be sensitive to momentum currents and the shear viscosity per unit of entropy density η/s\eta/s of the matter produced in the collisions. The observed broadening is found to be consistent with the hypothesized lower bound of η/s\eta/s and is in qualitative agreement with values obtained from anisotropic flow measurements

    Inclusive J/ψ\psi production in Xe–Xe collisions at sNN\sqrt{s_{\rm NN}} = 5.44 TeV

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    Inclusive J/ψ\psi production is studied in Xe-Xe interactions at a centre-of-mass energy per nucleon pair of sNN=5.44\sqrt{s_{\rm NN}}= 5.44 TeV, using the ALICE detector at the CERN LHC. The J/ψ\psi meson is reconstructed via its decay into a muon pair, in the centre-of-mass rapidity interval 2.5<y<42.5<y<4 and down to zero transverse momentum. In this Letter, the nuclear modification factors RAAR_{\rm AA} for inclusive J/ψ\psi, measured in the centrality range 0-90% as well as in the centrality intervals 0-20% and 20-90% are presented. The RAAR_{\rm AA} values are compared to previously published results for Pb-Pb collisions at sNN=5.02\sqrt{s_{\rm NN}}= 5.02 TeV and to the calculation of a transport model. A good agreement is found between Xe-Xe and Pb-Pb results as well as between data and the model
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