Tracker : Applikationen som håller koll på din rörelse

Målet med det här arbetet har varit att ta fram en Androidapplikation som kan spåra användaren och ge information om hur användaren rört sig med tid, distans altitud och hastighet. Applikationen ska vara individuellt fungerande men det stora syftet är att den ska fungera som en av tre delar i en större applikation med fler funktioner för de som är ute i skogen och rör på sig. Då inte alla telefoner har en inbyggd stegräknare kommer en undersökning göras för att se vilken sensor som lämpar sig bäst för att räkna steg och sedan använda den i applikationen. Resultatet blev en fungerande applikation som spårar användaren med hjälp av GPS, räknar antalet steg med antingen den inbyggda stegräknaren eller med hjälp av gyroskopet som visade sig vara den mest lämpade sensorn att räkna steg med. Utöver det så presenteras information om tid, distans och vilken altitud användaren rört sig på. All information kan sparas och användaren kan scrolla i en lista med sparade rutter.

Student digital experience tracker 2016: results from the pilot project

Building on funded work on the experiences of today’s digital students http://bit.ly/jiscdigistudent (2014-2015) and feedback from stakeholders, Jisc piloted a tracker tool with 24 education providers in Higher education (HE) and Further Education (FE) and skills. The aim of the tracker is to provide a snapshot of learners’ digital experiences at a training provider, college or university so that education providers can better understand this aspect of the learning experience. This survey report highlights key findings from the tracker pilot.

Student Digital Experience Tracker Case Study: University of Westminster

Student Digital Experience Tracker Case Study: University of Westminster. A case study describing the pilot of the Jisc Student Digital Experience Tracker at the University of Westminster.

Student Digital Experience Tracker Case Study: North Lindsey College

Student Digital Experience Tracker Case Study: North Lindsey College describing their experiences of being involved in the Jisc Pilot.

Student Digital Experience Tracker Case Study: University of Northampton

Student Digital Experience Tracker Case Study: University of Northampton describing their experience of being in the Jisc pilot.

Student Digital Experience Tracker Case Study: University of Nottingham Ningbo China

Student Digital Experience Tracker Case Study: University of Nottingham Ningbo China describing their experience of being in the Jisc pilot.

Student Digital Experience Tracker Case Study: Case study: Barton Peverill Sixth Form College

Student Digital Experience Tracker Case Study: Case study: Barton Peverill Sixth Form College describing their experiences of the tracker pilot.

Student Digital Experience Tracker Case Study: Royal National College for the Blind

Student Digital Experience Tracker Case Study: Royal National College for the Blind describing their experience of the Tracker pilot.

Student Digital Experience Tracker Case Study: University of Westminster

Student Digital Experience Tracker Case Study: University of Westminster to describe their participation in the Tracker pilot.

Student Digital Experience Tracker Case Study: Key Training

Student Digital Experience Tracker Case Study: Key Training describing their experiences of the Tracker pilot.

Il sistema Trauma Tracker - individuazione e analisi di parametri vitali acquisiti da monitor multiparametrico.

Lo scopo della presente tesi è lo studio e la progettazione di un sistema Hands-Free applicato in ambito Healthcare, volto ad aiutare il personale sanitario nello svolgimento delle mansioni lavorative. Il progetto, denominato Trauma Tracker, ha avuto origine grazie alla collaborazione con medici ed infermieri dell'ospedale Maurizio Bufalini di Cesena. In particolare, il sistema in prodotto si prende carico della compilazione del report finale contenente tutte le operazioni svolte sui pazienti nell'ambito del Pronto Soccorso, riducendo così notevolmente le possibilità di errori dovuti a fattori umani. Durante le fasi di sviluppo e progettazione sono state aggiunte ulteriori funzionalità al sistema, fino a farlo diventare vero e proprio oggetto incantato, in grado di esibire proprietà finora inimmaginabili in questo campo di applicazione. Trauma Tracker, almeno in queste prime fasi, non si propone come uno strumento immediatamente utilizzabile sul campo e pronto ad affiancare i medici, poiché necessiterebbe subito di qualità come robustezza ed affidabilità a livelli estremamente elevati. Per questo motivo il progetto è stato trattato come un "Proof of Concept", ossia un prototipo che ha lo scopo di dimostrare la fattibilità di tale sistema nella realtà, e di verificarne l'utilità una volta applicato in uno scenario concreto. L'argomento trattato ha quindi una grande importanza, poiché getta le basi di una tecnologia che un giorno potrà aiutare medici ed infermieri a svolgere al meglio l'impegnativo compito di salvare vite. In questa tesi, è stato approfondito in particolare il sottosistema utilizzato per il riconoscimento dei parametri vitali dal monitor multi-parametrico posto nei diversi reparti ospedalieri. Esso ha richiesto lunghe fasi di implementazione e collaudo per ottenere dei risultati soddisfacenti, che alla fine sono stati raggiunti.

K*(0) production in Cu plus Cu and Au plus Au collisions at root s(NN)=62.4 GeV and 200 GeV

We report on K*(0) production at midrapidity in Au + Au and Cu + Cu collisions at root s(NN) = 62.4 and 200 GeV collected by the Solenoid Tracker at the Relativistic Heavy Ion Collider detector. The K*(0) is reconstructed via the hadronic decays K*(0) -> K(+)pi(-) and (K*(0)) over bar -> K(+)pi(-). Transverse momentum, p(T), spectra are measured over a range of p(T) extending from 0.2 GeV/c up to 5 GeV/c. The center-of-mass energy and system size dependence of the rapidity density, dN/dy, and the average transverse momentum, < p(T)>, are presented. The measured N(K*(0))/N(K) and N(phi)/N(K*(0)) ratios favor the dominance of rescattering of decay daughters of K*(0) over the hadronic regeneration for the K*(0) production. In the intermediate p(T) region (2.0 < p(T) < 4.0 GeV/c), the elliptic flow parameter, v(2), and the nuclear modification factor, R(CP), agree with the expectations from the quark coalescence model of particle production.

Charged and strange hadron elliptic flow in Cu plus Cu collisions at root s(NN)=62.4 and 200 GeV

We present the results of an elliptic flow, v(2), analysis of Cu + Cu collisions recorded with the solenoidal tracker detector (STAR) at the BNL Relativistic Heavy Ion Collider at root s(NN) = 62.4 and 200 GeV. Elliptic flow as a function of transverse momentum, v(2)(p(T)), is reported for different collision centralities for charged hadrons h(+/-) and strangeness-ontaining hadrons K(S)(0), Lambda, Xi, and phi in the midrapidity region vertical bar eta vertical bar < 1.0. Significant reduction in systematic uncertainty of the measurement due to nonflow effects has been achieved by correlating particles at midrapidity, vertical bar eta vertical bar < 1.0, with those at forward rapidity, 2.5 < vertical bar eta vertical bar < 4.0. We also present azimuthal correlations in p + p collisions at root s = 200 GeV to help in estimating nonflow effects. To study the system-size dependence of elliptic flow, we present a detailed comparison with previously published results from Au + Au collisions at root s(NN) = 200 GeV. We observe that v(2)(p(T)) of strange hadrons has similar scaling properties as were first observed in Au + Au collisions, that is, (i) at low transverse momenta, p(T) < 2 GeV/c, v(2) scales with transverse kinetic energy, m(T) - m, and (ii) at intermediate p(T), 2 < p(T) < 4 GeV/c, it scales with the number of constituent quarks, n(q.) We have found that ideal hydrodynamic calculations fail to reproduce the centrality dependence of v(2)(p(T)) for K(S)(0) and Lambda. Eccentricity scaled v(2) values, v(2)/epsilon, are larger in more central collisions, suggesting stronger collective flow develops in more central collisions. The comparison with Au + Au collisions, which go further in density, shows that v(2)/epsilon depends on the system size, that is, the number of participants N(part). This indicates that the ideal hydrodynamic limit is not reached in Cu + Cu collisions, presumably because the assumption of thermalization is not attained.