Secular and tidal evolution of circumbinary systems

We investigate the secular dynamics of three-body circumbinary systems under the effect of tides. We use the octupolar non-restricted approximation for the orbital interactions, general relativity corrections, the quadrupolar approximation for the spins, and the viscous linear model for tides. We derive the averaged equations of motion in a simplified vectorial formalism, which is suitable to model the long-term evolution of a wide variety of circumbinary systems in very eccentric and inclined orbits. In particular, this vectorial approach can be used to derive constraints for tidal migration, capture in Cassini states, and stellar spin–orbit misalignment. We show that circumbinary planets with initial arbitrary orbital inclination can become coplanar through a secular resonance between the precession of the orbit and the precession of the spin of one of the stars. We also show that circumbinary systems for which the pericenter of the inner orbit is initially in libration present chaotic motion for the spins and for the eccentricity of the outer orbit. Because our model is valid for the non-restricted problem, it can also be applied to any three-body hierarchical system such as star–planet–satellite systems and triple stellar systems.

A doorway to Borromean halo nuclei: the Samba configuration

We exploit the possibility of new configurations in three-body halo nuclei, Samba type (the neutron-core form a bound system) as a doorway to Borromean systems. The nuclei Be-12, B-15, N-23 and F-27 are of such nature, in particular N-23 with a half-life of 37.7 s and a halo radius of 6.07 fm is an excellent example of Samba-halo configuration. The fusion below the barrier of the Samba halo nuclei with heavy targets could reveal the so far elusive enhancement and a dominance of one-neutron over two-neutron transfers, in contrast to what was found recently for the Borromean halo nucleus He-6 + U-238.

Efecto del ejercicio de tiro y arrastre sobre el eje renina-angiotensina-aldosterona y cociente testosterona/cortisol en caballos euhidratados y deshidratados

Introducción. El estado hídrico previo al inicio de un ejercicio (hiperhidratación-deshidratación o hipohidratación y euhidratación) modifica la respuesta neurohumoral. En personas, la deshidratación origina una liberación incrementada de las hormonas implicadas en el mantenimiento de la volemia y del estado hidroelectrolítico, tales como la renina (REN), angiotensina (ANG) y aldosterona (ALD). La testosterona (T) es una hormona anabólica, mientras que el cortisol (C) es una hormona de estrés, con funciones catabólicas. El cociente T/C es un reflejo de la intensidad anabólica/catabólica de un ejercicio y en atletas humanos, se ve afectada por el estado hídrico. Objetivos. 1) Describir las variaciones en las concentraciones de REN, ANG, ALD, T, C y ratio T/C en caballos durante un ejercicio de tiro y arrastre, en relación con otros marcadores de equilibrio hidroelectrolítico y en función de la carga arrastrada; 2) Analizar si la respuesta de estas hormonas al ejercicio difiere entre animales con deshidratación hipertónica y euhidratados; Hipótesis: 1) Que las concentraciones de REN, ANG, ALD, T, C serán más elevadas en los caballos deshidratados que en los euhidratados; 2) Que el ejercicio de tiro y arrastre, particularmente en los animales de mayor peso corporal, inducirá una mayor activación del eje REN, ANG, ALD y una liberación superior de T; 3) Que los animales deshidratados experimentarán un incremento más intenso de estas hormonas en respuesta al ejercicio. Material y métodos. Se han llevado a cabo dos estudios simultáneos. En el estudio I, se han analizado los siguientes parámetros: valor hematócrito (HTO), albúmina (ALB), sodio (Na), potasio (K), cloro (Cl), lactato (LA) y concentraciones séricas de REN, ANG y ALD y en el estudio II, se han determinado las concentraciones de ALB, T, C y ratio T/C. En el estudio I, se han incluido 64 caballos machos, enteros y castrados, divididos en dos grupos según su estado hídrico: grupo control o euhidratado (CTR, n=11) y grupo deshidratado (DH; n=53), con deshidratación hipertónica inducida por restricción de agua y comida. Además, según su peso corporal, los animales se han dividido en 3 categorías de peso: I (<350 kg; n=3 para grupo CTR; n=23 para DH), II (351-450 kg; n=3 para CTR; n=18 para DH) y III (>451 kg; n=5 para CTR; n=12 para DH). En el estudio II, se han incluido los mismos animales, con excepción de la categoría de peso III para el grupo CTR, que solo está constituida por 3 animales, en lugar de 5, al descartar a los machos castrados, debido a la medición de T. Todos los animales, realizaron un ejercicio consistente en recorrer una pista de arena de playa de 60 m de longitud, tirando de un carruaje, con 2, 2,25 y 2,5 veces su peso corporal para las tres categorías de peso. La pista de arena se dividió en cuatro áreas de 15 m, en cada una de las cuales, el animal hizo una parada obligatoria, de duración decidida por el acompañante, y que se incluyó como tiempo de carrera. Los animales eran eliminados si se superan los 5 min de duración. En los dos estudios, se tomaron muestras de sangre en los siguientes tiempos: en reposo, antes del ejercicio (R), dentro del primer minuto tras finalizar el ejercicio (E) y a los 5, 10, 15 y 30 minutos de una recuperación pasiva (5REC, 10REC, 15REC y 30REC). Resultados. Estudio I. La diferencia de peso de los caballos tuvo una influencia mínima en los valores basales y en la respuesta al ejercicio. En reposo, los caballos DH tuvieron valores superiores de HTO, ALB, LA, Na, K y ANG en comparación con los CTR. El ejercicio condicionó una elevación de HTO, ALB, LA y Na, tanto en los caballos CTR como en los DH. Se encontró un incremento de ANG en los caballos DH y de ALD en los caballos CTR. La elevación con el ejercicio experimentada por los parámetros analizados fue de magnitud similar en los grupos CTR y DH, con excepción del LA (incrementó más en DH) y ALD (aumentó más en CTR). Estudio II. El ejercicio dio lugar a un aumento de T en las categorías I y III de los grupos CTR y DH, así como un descenso en la categoría II del grupo CTR. El C mostró un aumento progresivo en las tres categorías y en los dos grupos de estado hídrico, con los valores máximos en el tiempo 30REC. El ratio T/C aumentó en la categoría III del grupo DH, descendió en la categoría II del grupo CTR y no varió en los otros casos. Los animales DH, independientemente de la categoría de peso, tuvieron valores superiores de T y C, en la mayoría de los tiempos de extracción de muestras. Sin embargo, si se consideran los cambios experimentados por estas hormonas durante el ejercicio o en la recuperación, en relación a los valores basales, el aumento del C fue más marcado en el grupo CTR que en el DH, para las tres categorías de peso. Las variaciones de la concentración de T fueron superiores en las categorías de peso I y III del grupo CTR que en el grupo DH. El ratio T/C fue estadísticamente igual entre caballos CTR y DH en las categorías I y III, mientras que en la categoría II, los caballos DH presentaron cocientes T/C mayores. Conclusiones. La deshidratación hipertónica altera la concentración de las hormonas implicadas en la regulación del equilibrio hidro-electrolítico, de la presión sanguínea y del metabolismo. Sin embargo, el estado hídrico previo al ejercicio tiene una acción mínima sobre la magnitud de estos cambios en respuesta a un ejercicio de tiro y arrastre de corta duración (inferior a 5 min). Relevancia. Se ha demostrado que la respuesta neurohumoral, determinada en base a las concentraciones circulantes de las hormonas REN, ANG, ALD, T y C, se ve afectada por el ejercicio cuando el animal empieza el mismo en estado de euhidratación o de deshidratación.

Accurate Treatment of Large Supramolecular Complexes by Double-Hybrid Density Functionals Coupled with Nonlocal van der Waals Corrections

In this work, we present a thorough assessment of the performance of some representative double-hybrid density functionals (revPBE0-DH-NL and B2PLYP-NL) as well as their parent hybrid and GGA counterparts, in combination with the most modern version of the nonlocal (NL) van der Waals correction to describe very large weakly interacting molecular systems dominated by noncovalent interactions. Prior to the assessment, an accurate and homogeneous set of reference interaction energies was computed for the supramolecular complexes constituting the L7 and S12L data sets by using the novel, precise, and efficient DLPNO-CCSD(T) method at the complete basis set limit (CBS). The correction of the basis set superposition error and the inclusion of the deformation energies (for the S12L set) have been crucial for obtaining precise DLPNO-CCSD(T)/CBS interaction energies. Among the density functionals evaluated, the double-hybrid revPBE0-DH-NL and B2PLYP-NL with the three-body dispersion correction provide remarkably accurate association energies very close to the chemical accuracy. Overall, the NL van der Waals approach combined with proper density functionals can be seen as an accurate and affordable computational tool for the modeling of large weakly bonded supramolecular systems.

A transient three-dimensional heat transfer model of the human body

The objective of this work is to develop an improved model of the human thermal system. The features included are important to solve real problems: 3D heat conduction, the use of elliptical cylinders to adequately approximate body geometry, the careful representation of tissues and important organs, and the flexibility of the computational implementation. Focus is on the passive system, which is composed by 15 cylindrical elements and it includes heat transfer between large arteries and veins. The results of thermal neutrality and transient simulations are in excellent agreement with experimental data, indicating that the model represents adequately the behavior of the human thermal system. (C) 2009 Elsevier Ltd. All rights reserved.

Estimation of total body water from bioelectrical impedance analysis in patients with pancreatic cancer - agreement between three methods of prediction

Introduction Bioelectrical impedance analysis (BIA) is a useful field measure to estimate total body water (TBW). No prediction formulae have been developed or validated against a reference method in patients with pancreatic cancer. The aim of this study was to assess the agreement between three prediction equations for the estimation of TBW in cachectic patients with pancreatic cancer. Methods Resistance was measured at frequencies of 50 and 200 kHz in 18 outpatients (10 males and eight females, age 70.2 +/- 11.8 years) with pancreatic cancer from two tertiary Australian hospitals. Three published prediction formulae were used to calculate TBW - TBWs developed in surgical patients, TBWca-uw and TBWca-nw developed in underweight and normal weight patients with end-stage cancer. Results There was no significant difference in the TBW estimated by the three prediction equations - TBWs 32.9 +/- 8.3 L, TBWca-nw 36.3 +/- 7.4 L, TBWca-uw 34.6 +/- 7.6 L. At a population level, there is agreement between prediction of TBW in patients with pancreatic cancer estimated from the three equations. The best combination of low bias and narrow limits of agreement was observed when TBW was estimated from the equation developed in the underweight cancer patients relative to the normal weight cancer patients. When no established BIA prediction equation exists, practitioners should utilize an equation developed in a population with similar critical characteristics such as diagnosis, weight loss, body mass index and/or age. Conclusions Further research is required to determine the accuracy of the BIA prediction technique against a reference method in patients with pancreatic cancer.

Body proportions in three Nigerian tribes

Prediction equations of body composition based on measurements of whole-body bioelectrical impedance analysis (BIA) have been found to be population-specific. It was hypothesised that this may be, in part, due to differences in proportional limb lengths between ethnic or racial groups. As a preliminary to a survey of body composition in urban Nigerians using BIA, the relative limb lengths of the three major tribal groups (Hausa, Yoruba and Ibo) were determined. We found small (5-9%) but significantly longer limb lengths in Nigerians compared to a Caucasian population, but no significant differences between tribes. This implies that BIA prediction equations generated in a Caucasian population are inappropriate for use in a Nigerian population.

Comparative winter thermoregulation and body temperature in three sympatric Apodemus species (A-alpicola, A-flavicollis, and A-sylvaticus)

When living in sympatry with Apodemus sylvaticus and A. flavicollis, A. alpicola dominates numerically at higher altitudes. A more efficient winter thermal isolation or a higher winter thermogenic capacity procuring a physiological advantage could explain at least part of this domination. We therefore measured body temperature (Tb), oxygen consumption (VO2), wet minimal thermal conductance (C) and non shivering thermogenesis (NST) at different ambient temperatures (Ta) on winter acclimated mice of the three species, and this for the first time in A. alpicola. NST was high and C low in the three species. No significant difference could be noticed either in Tb between 5 and -10 degrees C, in VO2 measurements at a Ta of -10 degrees C or in C. The NST measurements represent, respectively, 135.2% for A. sylvaticus, 142.8% for A. flavicollis and 140.5% for A. alpicola of the expected values, the values for A. sylvaticus being significantly lower than for the other two species. The basal metabolic rates (BMR) represent 169.4% for A. sylvaticus, 161.6% for A. flavicollis and 138.3% for A. alpicola of the expected values. Having removed the effect of body weight, the BMR value was significantly lower in A. alpicola than in A. flavicollis, but no difference could be noticed between A. sylvaticus and the other two species. In conclusion, the three species of mice have very similar acclimated thermoregulatory characteristics, well adapted to cold ambient conditions. One discriminating and advantageous factor could be the lower basal metabolic rate measured in A. alpicola compared to the other two species.

Modelling body mass index and endometrial cancer risk in a pooled-analysis of three case-control studies.

OBJECTIVE: To quantify the relation between body mass index (BMI) and endometrial cancer risk, and to describe the shape of such a relation. DESIGN: Pooled analysis of three hospital-based case-control studies. SETTING: Italy and Switzerland. POPULATION: A total of 1449 women with endometrial cancer and 3811 controls. METHODS: Multivariate odds ratios (OR) and 95% confidence intervals (95% CI) were obtained from logistic regression models. The shape of the relation was determined using a class of flexible regression models. MAIN OUTCOME MEASURE: The relation of BMI with endometrial cancer. RESULTS: Compared with women with BMI 18.5 to <25 kg/m(2) , the odds ratio was 5.73 (95% CI 4.28-7.68) for women with a BMI ≥35 kg/m(2) . The odds ratios were 1.10 (95% CI 1.09-1.12) and 1.63 (95% CI 1.52-1.75) respectively for an increment of BMI of 1 and 5 units. The relation was stronger in never-users of oral contraceptives (OR 3.35, 95% CI 2.78-4.03, for BMI ≥30 versus <25 kg/m(2) ) than in users (OR 1.22, 95% CI 0.56-2.67), and in women with diabetes (OR 8.10, 95% CI 4.10-16.01, for BMI ≥30 versus <25 kg/m(2) ) than in those without diabetes (OR 2.95, 95% CI 2.44-3.56). The relation was best fitted by a cubic model, although after the exclusion of the 5% upper and lower tails, it was best fitted by a linear model. CONCLUSIONS: The results of this study confirm a role of elevated BMI in the aetiology of endometrial cancer and suggest that the risk in obese women increases in a cubic nonlinear fashion. The relation was stronger in never-users of oral contraceptives and in women with diabetes. TWEETABLE ABSTRACT: Risk of endometrial cancer increases with elevated body weight in a cubic nonlinear fashion.

Three-dimensional supersonic flow over a spike-nosed body of revolution

The unsteady, viscous, supersonic flow over a spike-nosed body of revolution is numerically investigated by solving the Navier-Stokes equations. The time-accurate computations are performed employing an implicit algorithm based on the second-order time-accurate LU-SGS scheme with the incorporation of a subiteration procedure to maintain time accuracy. The characteristics of the flow field for a Mach number of 3.0, Reynolds number of 7.87 x 10(6)/m, and angles of attack of 5 and 10 degrees are described. Self-sustained asymmetric shock wave oscillations were observed in the numerical computations for these angles of attack. The main characteristic of the flow field, as well as its influence on drag coefficient is discussed.

An O(N) Algorithm for Three-Dimensional N-Body Simulations

We develop an algorithm that computes the gravitational potentials and forces on N point-masses interacting in three-dimensional space. The algorithm, based on analytical techniques developed by Rokhlin and Greengard, runs in order N time. In contrast to other fast N-body methods such as tree codes, which only approximate the interaction potentials and forces, this method is exact ?? computes the potentials and forces to within any prespecified tolerance up to machine precision. We present an implementation of the algorithm for a sequential machine. We numerically verify the algorithm, and compare its speed with that of an O(N2) direct force computation. We also describe a parallel version of the algorithm that runs on the Connection Machine in order 0(logN) time. We compare experimental results with those of the sequential implementation and discuss how to minimize communication overhead on the parallel machine.

Toward the Application of Three-Dimensional Approach to Few-body Atomic Bound States

The first step toward the application of an effective non partial wave (PW) numerical approach to few-body atomic bound states has been taken. The two-body transition amplitude which appears in the kernel of three-dimensional Faddeev-Yakubovsky integral equations is calculated as function of two-body Jacobi momentum vectors, i.e. as a function of the magnitude of initial and final momentum vectors and the angle between them. For numerical calculation the realistic interatomic interactions HFDHE2, HFD-B, LM2M2 and TTY are used. The angular and momentum dependence of the fully off-shell transition amplitude is studied at negative energies. It has been numerically shown that, similar to the nuclear case, the transition amplitude exhibits a characteristic angular behavior in the vicinity of He-4 dimer pole.

Three-Dimensional Low-Momentum Interaction in Two-Body Bound State Calculations

The deuteron binding energy and wave function are calculated by using the recently developed three-dimensional form of low-momentum nucleon-nucleon (NN) interaction. The homogeneous Lippmann-Schwinger equation is solved in momentum space by using the low-momentum two-body interaction, which is constructed from Malfliet-Tjon potential. The results for both, deuteron binding energy and wave function, obtained with low-momentum interaction, are compared with the corresponding results obtained with bare potential. © 2012 Springer-Verlag.

Three-dimensional joint kinematics of swimming using body-worn inertial and magnetic sensors

Wearable inertial and magnetic measurements units (IMMU) are an important tool for underwater motion analysis because they are swimmer-centric, they require only simple measurement set-up and they provide the performance results very quickly. In order to estimate 3D joint kinematics during motion, protocols were developed to transpose the IMMU orientation estimation to a biomechanical model. The aim of the thesis was to validate a protocol originally propositioned to estimate the joint angles of the upper limbs during one-degree-of-freedom movements in dry settings and herein modified to perform 3D kinematics analysis of shoulders, elbows and wrists during swimming. Eight high-level swimmers were assessed in the laboratory by means of an IMMU while simulating the front crawl and breaststroke movements. A stereo-photogrammetric system (SPS) was used as reference. The joint angles (in degrees) of the shoulders (flexion-extension, abduction-adduction and internal-external rotation), the elbows (flexion-extension and pronation-supination), and the wrists (flexion-extension and radial-ulnar deviation) were estimated with the two systems and compared by means of root mean square errors (RMSE), relative RMSE, Pearson’s product-moment coefficient correlation (R) and coefficient of multiple correlation (CMC). Subsequently, the athletes were assessed during pool swimming trials through the IMMU. Considering both swim styles and all joint degrees of freedom modeled, the comparison between the IMMU and the SPS showed median values of RMSE lower than 8°, representing 10% of overall joint range of motion, high median values of CMC (0.97) and R (0.96). These findings suggest that the protocol accurately estimated the 3D orientation of the shoulders, elbows and wrists joint during swimming with accuracy adequate for the purposes of research. In conclusion, the proposed method to evaluate the 3D joint kinematics through IMMU was revealed to be a useful tool for both sport and clinical contexts.