Informatizamos el cole : memoria final curso 97-98.

Ayudas concedidas a proyectos de innovación educativa del CIDE en el curso 1997-1998. Anexo memoria en C-Innov.51

Mejoramos la convivencia participando en el cole.

En el CD se anexan los vídeos sobre todas las actividades y talleres organizados.

La violencia en el ??mbito escolar = La violence dans l'??cole = Violence in School

Percepciones y preocupaciones del profesorado con respecto a la violencia en la Educaci??n Secundaria y a las posibilidades de la educaci??n para elaborar estrategias y alternativas v??lidas para educar en favor de la paz, la justicia y el desarrollo. 42 profesores de Educaci??n Secundaria, seleccionados en funci??n de: cobertura geogr??fica, disponibilidad y criterios de tipo pr??ctico. La investigaci??n se distribuy?? en cuatro fases, la primera de car??cter exploratorio y de inmersi??n en la comunidad, en la segunda se realiz?? una din??mica con un grupo de discusi??n formado por educadores con circunstancias personales, profesionales y acad??micas distintas, en la tercera la realizaci??n de entrevistas pretest y selecci??n de la muestra y en la cuarta la interpretaci??n y categorizaci??n de la informaci??n obtenida de las entrevistas. Investigaci??n cualitativa de car??cter cuasi-etnogr??fico. No se puede afirmar que se disponga de un paradigma conceptual capaz de interpretar la naturaleza del problema de la violencia escolar en todas sus dimensiones. Su estudio requiere de una reflexi??n profunda sobre el alcance del problema que ponga las bases para comprender su naturaleza y gu??e el camino de la intervenci??n educativa para prevenirla; para ello es necesario multiplicar los procesos de investigaci??n y de intervenci??n que permitan acceder, de forma democr??tica y no traum??tica a su comprensi??n y erradicaci??n.

Teatro en el cole : El Mago de Oz

Proyecto realizado por alumnos del CEIP Santiago Ramón y Cajal de Plasencia (Cáceres), con los objetivos de fomentar el hábito lector-escritor, dinamizar el uso de la biblioteca, reforzar la implicación de los padres en la tarea educativa y desarrollar aspectos de inteligencia emocional (motivación, autoestima y empatía)

Un barrio de cine, un cole de pel??cula

Experiencia realizada en el CEIP Santa Teresa, de Valencia, ubicado en un antiguo cine. Participan todos los alumnos del centro y tambi??n los otros colectivos de la comunidad educativa. El objetivo del proyecto ha sido el hacer una pel??cula que rindiera homenaje a las pel??culas de todos los tiempos y recobrar de esta manera el pasado del edificio. Se explican el proceso de aprendizaje y la programaci??n de las actividades que finalizan con el estreno de la pel??cula en el patio del colegio convertido en el patio de butacas del antiguo cine.

"Enseigner les sciences": un espace numérique d'échange et de formation concernant l'enseignement des sciences à l'école primaire

Cela fait maintenant plus de 10 ans que les premiers dispositifs de e-learning ont vu le jour, que ce soit pour la formation continue ou pour la formation initiale. Dans un premier temps, le recours aux technologies n’a consisté qu’à publier sur Internet l’ensemble des ressources ainsi que le cours, sous forme de texte, dispensé par l’enseignant. Puis, grâce à l’évolution des technologies, de nouvelles possibilités ont vu le jour : la mise en ligne de documents audios, de vidéos, et plus récemment, la mise en place d’espaces numériques de travail permettant à l’enseignant, comme à tous les participants, d’y placer des documents et des commentaires. L’apparition des wikis a permis de voir apparaître de nouvelles formes de e-learning, basés sur la collaboration. Depuis quelques mois, l’explosion des réseaux sociaux, facebook pour le plus célèbre, permet d’envisager de nouveaux dispositifs d’apprentissage interconnectant cours en présentiel et travail à distance

Les Affiches engagées à l'école primaire: out un décodage!

La publicité est depuis bien longtemps un sujet de débat social sur lequel différents auteurs se sont penchés, l’ont étudiée et ont donné leur avis, ainsi que des pistes d’analyse pour mieux comprendre ce phénomène qui est partout et qui touche toutes les couches de la population. Parmi toutes les formes que la publicité peut revêtir, il y en a une que l’on retrouve partout où l’on va et qui s’impose à notre regard. Il s’agit des affiches publicitaires. Ces dernières peuvent parfois être confondues avec une autre sorte d’affiches: il s’agit des affiches dites engagées. En effet, les élèves retrouvent ce type d’affiches partout ; sur le chemin de l’école, lorsqu’ils marchent dans la rue, que cela soit à la ville comme à la campagne, dans les journaux ou encore sur Internet. Dans ce projet de mémoire, je me suis intéressée à la création d’une séquence d’enseignement aux messages visuels, qu’ils soient scripturaux et/ou iconiques, véhiculés par les affiches engagées pour une classe de 6P de l’école primaire genevoise. Cette séquence se compose de six leçons et a comme finalité la production, par les élèves eux-mêmes, d’une affiche engagée

The counter-propagating Rossby-wave perspective on baroclinic instability. Part III: Primitive-equation disturbances on the sphere

Baroclinic instability of perturbations described by the linearized primitive quations, growing on steady zonal jets on the sphere, can be understood in terms of the interaction of pairs of counter-propagating Rossby waves (CRWs). The CRWs can be viewed as the basic components of the dynamical system where the Hamiltonian is the pseudoenergy and each CRW has a zonal coordinate and pseudomomentum. The theory holds for adiabatic frictionless flow to the extent that truncated forms of pseudomomentum and pseudoenergy are globally conserved. These forms focus attention on Rossby wave activity. Normal mode (NM) dispersion relations for realistic jets are explained in terms of the two CRWs associated with each unstable NM pair. Although derived from the NMs, CRWs have the conceptual advantage that their structure is zonally untilted, and can be anticipated given only the basic state. Moreover, their zonal propagation, phase-locking and mutual interaction can all be understood by ‘PV-thinking’ applied at only two ‘home-bases’—potential vorticity (PV) anomalies at one home-base induce circulation anomalies, both locally and at the other home-base, which in turn can advect the PV gradient and modify PV anomalies there. At short wavelengths the upper CRW is focused in the mid-troposphere just above the steering level of the NM, but at longer wavelengths the upper CRW has a second wave-activity maximum at the tropopause. In the absence of meridional shear, CRW behaviour is very similar to that of Charney modes, while shear results in a meridional slant with height of the air-parcel displacement-structures of CRWs in sympathy with basic-state zonal angular-velocity surfaces. A consequence of this slant is that baroclinically growing eddies (on jets broader than the Rossby radius) must tilt downshear in the horizontal, giving rise to up-gradient momentum fluxes that tend to accelerate the barotropic component of the jet.

Small- and waiting-time behaviour of the thin-film-equation

We consider the small-time behavior of interfaces of zero contact angle solutions to the thin-film equation. For a certain class of initial data, through asymptotic analyses, we deduce a wide variety of behavior for the free boundary point. These are supported by extensive numerical simulations. © 2007 Society for Industrial and Applied Mathematics

An integral equation method for a boundary value problem arising in unsteady water wave problems

In this paper we consider the 2D Dirichlet boundary value problem for Laplace’s equation in a non-locally perturbed half-plane, with data in the space of bounded and continuous functions. We show uniqueness of solution, using standard Phragmen-Lindelof arguments. The main result is to propose a boundary integral equation formulation, to prove equivalence with the boundary value problem, and to show that the integral equation is well posed by applying a recent partial generalisation of the Fredholm alternative in Arens et al [J. Int. Equ. Appl. 15 (2003) pp. 1-35]. This then leads to an existence proof for the boundary value problem. Keywords. Boundary integral equation method, Water waves, Laplace’s

Understanding mixing efficiency in the oceans. Do the nonlinearities of the equation of state matter?

There exist two central measures of turbulent mixing in turbulent stratified fluids that are both caused by molecular diffusion: 1) the dissipation rate D(APE) of available potential energy APE; 2) the turbulent rate of change Wr, turbulent of background gravitational potential energy GPEr. So far, these two quantities have often been regarded as the same energy conversion, namely the irreversible conversion of APE into GPEr, owing to the well known exact equality D(APE)=Wr, turbulent for a Boussinesq fluid with a linear equation of state. Recently, however, Tailleux (2009) pointed out that the above equality no longer holds for a thermally-stratified compressible, with the ratio ξ=Wr, turbulent/D(APE) being generally lower than unity and sometimes even negative for water or seawater, and argued that D(APE) and Wr, turbulent actually represent two distinct types of energy conversion, respectively the dissipation of APE into one particular subcomponent of internal energy called the "dead" internal energy IE0, and the conversion between GPEr and a different subcomponent of internal energy called "exergy" IEexergy. In this paper, the behaviour of the ratio ξ is examined for different stratifications having all the same buoyancy frequency N vertical profile, but different vertical profiles of the parameter Υ=α P/(ρCp), where α is the thermal expansion coefficient, P the hydrostatic pressure, ρ the density, and Cp the specific heat capacity at constant pressure, the equation of state being that for seawater for different particular constant values of salinity. It is found that ξ and Wr, turbulent depend critically on the sign and magnitude of dΥ/dz, in contrast with D(APE), which appears largely unaffected by the latter. These results have important consequences for how the mixing efficiency should be defined and measured in practice, which are discussed.

A well-posed integral equation formulation for three-dimensional rough surface scattering

We consider the problem of scattering of time-harmonic acoustic waves by an unbounded sound-soft rough surface. Recently, a Brakhage Werner type integral equation formulation of this problem has been proposed, based on an ansatz as a combined single- and double-layer potential, but replacing the usual fundamental solution of the Helmholtz equation with an appropriate half-space Green's function. Moreover, it has been shown in the three-dimensional case that this integral equation is uniquely solvable in the space L-2 (Gamma) when the scattering surface G does not differ too much from a plane. In this paper, we show that this integral equation is uniquely solvable with no restriction on the surface elevation or slope. Moreover, we construct explicit bounds on the inverse of the associated boundary integral operator, as a function of the wave number, the parameter coupling the single- and double-layer potentials, and the maximum surface slope. These bounds show that the norm of the inverse operator is bounded uniformly in the wave number, kappa, for kappa > 0, if the coupling parameter h is chosen proportional to the wave number. In the case when G is a plane, we show that the choice eta = kappa/2 is nearly optimal in terms of minimizing the condition number.

On integral equation and least squares methods for scattering by diffraction gratings

In this paper we consider the scattering of a plane acoustic or electromagnetic wave by a one-dimensional, periodic rough surface. We restrict the discussion to the case when the boundary is sound soft in the acoustic case, perfectly reflecting with TE polarization in the EM case, so that the total field vanishes on the boundary. We propose a uniquely solvable first kind integral equation formulation of the problem, which amounts to a requirement that the normal derivative of the Green's representation formula for the total field vanish on a horizontal line below the scattering surface. We then discuss the numerical solution by Galerkin's method of this (ill-posed) integral equation. We point out that, with two particular choices of the trial and test spaces, we recover the so-called SC (spectral-coordinate) and SS (spectral-spectral) numerical schemes of DeSanto et al., Waves Random Media, 8, 315-414 1998. We next propose a new Galerkin scheme, a modification of the SS method that we term the SS* method, which is an instance of the well-known dual least squares Galerkin method. We show that the SS* method is always well-defined and is optimally convergent as the size of the approximation space increases. Moreover, we make a connection with the classical least squares method, in which the coefficients in the Rayleigh expansion of the solution are determined by enforcing the boundary condition in a least squares sense, pointing out that the linear system to be solved in the SS* method is identical to that in the least squares method. Using this connection we show that (reflecting the ill-posed nature of the integral equation solved) the condition number of the linear system in the SS* and least squares methods approaches infinity as the approximation space increases in size. We also provide theoretical error bounds on the condition number and on the errors induced in the numerical solution computed as a result of ill-conditioning. Numerical results confirm the convergence of the SS* method and illustrate the ill-conditioning that arises.