175 research outputs found
Integrability of a linear center perturbed by a fourth degree homogeneous polynomial
In this work we study the integrability of a two-dimensional autonomous system in the plane with linear part of center type and non-linear part given by homogeneous polynomials of fourth degree. We give sufficient conditions for integrability in polar coordinates. Finally we establish a conjecture about the independence of the two classes of parameters which appear in the system; if this conjecture is true the integrable cases found will be the only possible ones
Integrability of a linear center perturbed by a fifth degree homogeneous polynomial
In this work we study the integrability of two-dimensional autonomous system in the plane with linear part of center type and non-linear part given by homogeneous polynomials of fifth degree. We give a simple characterisation for the integrable cases in polar coordinates. Finally we formulate a conjecture about the independence of the two classes of parameters which appear on the system; if this conjecture is true the integrable cases found will be the only possible ones
Integrability of a linear center perturbed by a fifth degree homogeneous polynomial
In this work we study the integrability of two-dimensional autonomous system in the plane with linear part of center type and non-linear part given by homogeneous polynomials of fifth degree. We give a simple characterisation for the integrable cases in polar coordinates. Finally we formulate a conjecture about the independence of the two classes of parameters which appear on the system; if this conjecture is true the integrable cases found will be the only possible ones
Integrability of a linear center perturbed by a fourth degree homogeneous polynomial
In this work we study the integrability of a two-dimensional autonomous system in the plane with linear part of center type and non-linear part given by homogeneous polynomials of fourth degree. We give sufficient conditions for integrability in polar coordinates. Finally we establish a conjecture about the independence of the two classes of parameters which appear in the system; if this conjecture is true the integrable cases found will be the only possible ones
The null divergence factor
Let be a vector field defined in a open subset . We call a null divergence factor a solution of the equation . In previous works it has been shown that this function plays a fundamental role in the problem of the center and in the determination of the limit cycles. In this paper we show how to construct systems with a given null divergence factor. The method presented in this paper is a generalization of the classical Darboux method to generate integrable systems
Isochronicity conditions for some planar polynomial systems II
We study the isochronicity of centers at for systems
where , which
can be reduced to the Li\'enard type equation. When and , using the so-called C-algorithm we found new families of
isochronous centers. When the Urabe function we provide an explicit
general formula for linearization. This paper is a direct continuation of
\cite{BoussaadaChouikhaStrelcyn2010} but can be read independantly
The null divergence factor
Let (P,Q) be a C1 vectorfield defined in a open subset U ⊂ R2. We call a null divergence factor a C1 solution V (x, y) of the equation P ∂V ∂x + Q∂V ∂y = ∂P ∂x + ∂Q ∂y V . In previous works it has been shown that this function plays a fundamental role in the problem of the center and in the determination of the limit cycles. In this paperw e show how to construct systems with a given null divergence factor. The method presented in this paper is a generalization of the classical Darboux method to generate integrable systems
Microfiltracion apical de pasta preparadas en base a hidroxido de calcio con diferentes vehiculos, para apexificacion. Estudio in vitro.
61 p.El objetivo de este estudio In Vitro fue determinar la microfiltración apical que sufre
el Hidróxido de calcio aplicado con diferentes vehÃculos.
Para esto se recolectaron 70 dientes uniradiculares (comprobado radiográficamente), luego se les cortaron las coronas y 1mm del 1/3 apical, luego fueron instrumentados con fresas Peeso nº II, irrigando con suero. Luego de esto
se pincelaron todas las muestras con esmalte de uñas desde 2mm del ápice hacia coronal.
Las muestras fueron divididas en 7 grupos de 10 ejemplares cada uno, conformando 7 grupos con los siguientes rellenos: 10 muestra rellenas con vidrio ionómero( control-),10 muestra no rellenas (control +),10 muestras rellenas con
hidróxido de calcio sólo,10 muestras rellenas con pasta de hidróxido de calcio más suero,10 muestra rellenas con pasta de hidróxido de calcio más propilenglicol,10 muestra rellenas con pasta de hidróxido de calcio más agua destilada y 10 muestra rellenas con pasta de hidróxido de calcio más anestesia. Luego se
sellaron en coronal con Chemfil, para posteriormente ser suspendidas en laminas
de plumavit rotuladas por grupo, en placas petri que contenÃan azul de metileno y estaban dentro de un baño termoregulado a 37ºC , 100% de humedad por 24 hrs. Luego se hicieron 2 cortes longitudinales a cada raÃz, se separaron las
mitades y se cuantificó la microfiltración con una lupa del articulador Panadent calibrada en décimas de mm. Los datos fueron analizados estadÃsticamente usando el test ANOVA , test de
Tukey y Duncan con un nivel de significancia de p≤0.05, encontrándose diferencias significativas en la micofiltración apical de las pastas en base a hidróxido de calcio con vehÃculos acuosos y viscosos. Se encontró una diferencia
altamente significativa entre las pasta en que se uso como vehÃculo agua destilada, anestesia y suero, que presentaron filtraciones promedio 11,73;11,99; 10,25 mm. respectivamente, y el grupo que utilizó un vehÃculo viscoso que fue el
propilenglicol cuyo promedio fue 6,67mm
Number and Amplitude of Limit Cycles emerging from {\it Topologically Equivalent} Perturbed Centers
We consider three examples of weekly perturbed centers which do not have {\it
geometrical equivalence}: a linear center, a degenerate center and a
non-hamiltonian center. In each case the number and amplitude of the limit
cycles emerging from the period annulus are calculated following the same
strategy: we reduce of all of them to locally equivalent perturbed integrable
systems of the form: , with
. This reduction allows us to find the Melnikov
function, , associated to each particular problem. We
obtain the information on the bifurcation curves of the limit cycles by solving
explicitly the equation in each case.Comment: 17 pages, 0 figure
- …