Short QT Syndrome Presenting As Syncope: How Short Is Too Short?

We report the case of a 52-year-old man who presented to our emergency department (ED) after three episodes of syncope in the seven hours before admission. During his stay in the ED he had recurrent ventricular tachycardia (VT) requiring external electrical cardioversion. A 12-lead electrocardiogram (ECG) showed a short QT (SQT) interval (270 ms, QTc 327 ms), with frequent R-on-T extrasystoles triggering sustained polymorphic VT. After exclusion of other precipitating causes, the patient was diagnosed as having SQT syndrome (SQTS) according to the Gollob criteria. To our knowledge, this is the first known documentation of an SQT-caused arrhythmic episode on a 12-lead ECG, as well as the first reported case of SQTS in Portugal. The patient received an implantable cardioverter-defibrillator and was discharged. At a follow-up assessment 14 months later he was symptom-free, interrogation of the device showed no arrhythmic events, and the ECG showed a QT interval of 320 ms (QTc 347 ms).

Numerical methods and tangible interfaces for pollutant dispersion simulation

Dissertação apresentada para obtenção do Grau de Doutor em Engenharia do Ambiente, pela Universidade Nova de Lisboa, Faculdade de Ciências e Tecnologia

The role of dispersion into assets allocation

Dispersion of returns has gained a lot of attention as a measure to distinguish good and bad investment opportunities time. In the following dissertation, the cross-sectional returns volatility is analyzed over a fifteen year period across the S&P100 Index composition. The main inference drawn from the data sample is that the canonical measure of dispersion is highly macro-risk driven and therefore more biased towards returns volatility rather than its correlation component.

Probing dispersion and re-agglomeration phenomena upon melt-mixing of polymer-functionalized graphite nanoplates

A one-step melt-mixing method is proposed to study dispersion and re-agglomeration phenomena of the as-received and functionalized graphite nanoplates in polypropylene melts. Graphite nanoplates were chemically modified via 1,3-dipolar cycloaddition of an azomethine ylide and then grafted with polypropylene-graft-maleic anhydride. The effect of surface functionalization on the dispersion kinetics, nanoparticle re-agglomeration and interface bonding with the polymer is investigated. Nanocomposites with 2 or 10 wt% of as-received and functionalized graphite nanoplates were prepared in a small-scale prototype mixer coupled to a capillary rheometer. Samples were collected along the flow axis and characterized by optical microscopy, scanning electron microscopy and electrical conductivity measurements. The as-received graphite nanoplates tend to re-agglomerate upon stress relaxation of the polymer melt. The covalent attachment of a polymer to the nanoparticle surface enhances the stability of dispersion, delaying the re-agglomeration. Surface modification also improves interfacial interactions and the resulting composites presented improved electrical conductivity.

Dispersion and re-agglomeration of graphite nanoplates in polypropylene melts under controlled flow conditions

The kinetics of GnP dispersion in polypropylene melt was studied using a prototype small scale modular extensional mixer. Its modular nature enabled the sequential application of a mixing step, melt relaxation, and a second mixing step. The latter could reproduce the flow conditions on the first mixing step, or generate milder flow conditions. The effect of these sequences of flow constraints upon GnP dispersion along the mixer length was studied for composites with 2 and 10 wt.% GnP. The samples collected along the first mixing zone showed a gradual decrease of number and size of GnP agglomerates, at a rate that was independent of the flow conditions imposed to the melt, but dependent on composition. The relaxation zone induced GnP re-agglomeration, and the application of a second mixing step caused variable dispersion results that were largely dependent on the hydrodynamic stresses generated.

Dispersion of graphite nanoplates during melt mixing

Artigo publicado a convite da Society for Polymer Engineers

Dispersion of fillers in viscoelastic polymer matrices using Eulerian-Lagrangian approaches

Understanding the behavior of c omplex composite materials using mixing procedures is fundamental in several industrial processes. For instance, polymer composites are usually manufactured using dispersion of fillers in polymer melt matrices. The success of the filler dispersion depends both on the complex flow patterns generated and on the polymer melt rheological behavior. Consequently, the availability of a numerical tool that allow to model both fluid and particle would be very useful to increase the process insight. Nowadays there ar e computational tools that allow modeling the behavior of filled systems, taking into account both the behavior of the fluid (Computational Rheology) and the particles (Discrete Element Method). One example is the DPMFoam solver of the OpenFOAM ® framework where the averaged volume fraction momentum and mass conservation equations are used to describe the fluid (continuous phase) rheology, and the Newton’s second law of motion is used to compute the particles (discrete phase) movement. In this work the refer red solver is extended to take into account the elasticity of the polymer melts for the continuous phase. The solver capabilities will be illustrated by studying the effect of the fluid rheology on the filler dispersion, taking into account different fluid types (generalized Newtonian or viscoelastic) and particles volume fraction and size. The results obtained are used to evaluate the relevance of considering the fluid complex rheology for the prediction of the composites morphology

Understanding the dispersion of fillers in polymer matrices

Understanding the mixing process of complex composite materials is fundamental in several industrial processes. For instance, the dispersion of fillers in polymer melt matrices is commonly employed to manufacture polymer composites, using a twin-screw extruder. The effectiveness of the filler dispersion depends not only on the complex flow patterns generated, but also on the polymer melt rheological behavior. Therefore, the availability of a numerical tool able to predict mixing, taking into account both fluid and particles phases would be very useful to increase the process insight, and thus provide useful guidelines for its optimization. In this work, a new Eulerian-Lagrangian numerical solver is developed OpenFOAM® computational library, and used to better understand the mechanisms determining the dispersion of fillers in polymer matrices. Particular attention will be given to the effect of the rheological model used to represent the fluid behavior, on the level of dispersion obtained. For the Eulerian phase the averaged volume fraction governing equations (conservation of mass and linear momentum) are used to describe the fluid behavior. In the case of the Lagrangian phase, Newton’s second law of motion is used to compute the particles trajectories and velocity. To study the effect of fluid behavior on the filler dispersion, several systems are modeled considering different fluid types (generalized Newtonian or viscoelastic) and particles volume fraction and size. The results obtained are used to correlate the fluid and particle characteristics on the effectiveness of mixing and morphology obtained.

Microstructure and mechanical properties of carbon nanotube reinforced cementitious composites developed using a novel dispersion technique

The authors also acknowledge Centre for Textile Science and Technology (University of Minho) and FIBRENAMICS PLATFORMfor providing required conditions for this research. Sincere thanks are also due to Mr. Pedro Samuel Leite and Mr. Carlos Jesus for their kind help in sample preparation and testing.

Nanocomposites: the contribution of multiscale modelling to improve the dispersion levels

Tese de Doutoramento em Ciência e Engenharia de Polímeros e Compósitos

Contribuição de eletrocardiografia dinâmica pelo sistema Holter na avaliação de pacientes com a síndrome congênita do QT longo

OBJETIVO: Avaliar pelo Holter-24h a dinâmica da repolarização ventricular de pacientes com a síndrome congênita do QT longo. MÉTODOS: Foram incluídos seis pacientes, sendo os resultados confrontados com os observados em um grupo controle semelhante em número, idade e sexo. Analisaram-se nas gravações a morfologia da onda T e sua dinâmica, o intervalo QTc médio para as 24h, as relações entre QT e ciclo cardíaco, a variabilidade do QTc das 24h, bem como a sua dispersão (diferença entre o maior e menor QTc observado). Todas as variáveis foram definidas a partir da medida do intervalo QT obtida no 1º minuto de cada hora da gravação. RESULTADOS: Alterações morfológicas da onda T estiveram presentes em todos os pacientes, observando-se em cinco deles freqüentes episódios de alternância da onda T, achados ausentes no controle. QTc médio para as 24h - controle: 436,1±8,9ms; pacientes: 598,2±73,8ms (p=0,000). Correlação linear entre QT e ciclo cardíaco - controle: r= 0,967; pacientes: r= 0,812 (p=0,000). Variabilidade do QTc para as 24h - controle: 14,7±2,1ms; pacientes: 36,9±17,2ms (p=0,01). Dispersão do QTc - controle: 53,3±8,1ms; pacientes: 168,3±70,2ms (p=0,000). CONCLUSÃO: Os resultados apresentaram ampla variabilidade dos intervalos QTc nas 24h, menor adaptabilidade do intervalo QT às flutuações dos ciclos cardíacos e significativa dispersão da repolarização ventricular nas 24h, confirmando mais uma vez a existência de importante alteração da vulnerabilidade ventricular nesses pacientes.

Análise da dispersão do intervalo QT em pacientes com infarto agudo do miocárdio: efeito da reperfusão coronariana

OBJETIVO: Estudar o efeito da reperfusão precoce da artéria relacionada ao infarto sobre a dispersão do intervalo QT(deltaQT), e seu valor como marcador de reperfusão coronária e de arritmias ventriculares. MÉTODOS: Foram avaliados 106 pacientes com reperfusão (CR) e 48 pacientes sem reperfusão (SR) que receberam terapia trombolítica na fase aguda do infarto. Foram analisados os eletrocardiogramas realizados na admissão e no 4º dia de evolução. A deltaQT, definido como a diferença entre o maior e o menor intervalo QT, foram medidos no ECG de 12 derivações. RESULTADOS: Na evolução do grupo com reperfusão, houve redução significativa da deltaQT de 89,66±20,47ms para 70,95±21,65ms (p<0,001). Por outro lado, no grupo sem reperfusão, houve aumento significativo da deltaQT de 81,27±20,52ms para 91,85±24,66ms (p<0,001). Análise de regressão logística demonstrou que a magnitude de redução entre a deltaQT pré e pós-trombólise foi o fator independente que identificou mais efetivamente a reperfusão coronária (OR 1,045, p<0,0001; IC 95%). Não houve diferença significativa das medidas de dispersão quando comparados os pacientes que apresentaram arritmias ventriculares nas primeiras 48 h com aqueles sem arritmias. CONCLUSÃO: Esse estudo mostra que a deltaQT reduz significativamente em pacientes com infarto agudo do miocárdio submetidos à trombólise com sucesso, aumentando nos pacientes que evoluem com a artéria fechada. A redução deltaQT entre a situação pré e pós-trombólise foi fator preditor de reperfusão coronária nesses pacientes, não apresentando correlação com arritmias ventriculares.