3,968 research outputs found

    Three-dimensional coating and rimming flow : a ring of fluid on a rotating horizontal cylinder

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    The steady three-dimensional flow of a thin, slowly varying ring of Newtonian fluid on either the outside or the inside of a uniformly rotating large horizontal cylinder is investigated. Specifically, we study “full-ring” solutions, corresponding to a ring of continuous, finite and non-zero thickness that extends all the way around the cylinder. In particular, it is found that there is a critical solution corresponding to either a critical load above which no full-ring solution exists (if the rotation speed is prescribed) or a critical rotation speed below which no full-ring solution exists (if the load is prescribed). We describe the behaviour of the critical solution and, in particular, show that the critical flux, the critical load, the critical semi-width and the critical ring profile are all increasing functions of the rotation speed. In the limit of small rotation speed, the critical flux is small and the critical ring is narrow and thin, leading to a small critical load. In the limit of large rotation speed, the critical flux is large and the critical ring is wide on the upper half of the cylinder and thick on the lower half of the cylinder, leading to a large critical load. We also describe the behaviour of the non-critical full-ring solution, and, in particular, show that the semi-width and the ring profile are increasing functions of the load but, in general, non-monotonic functions of the rotation speed. In the limit of large rotation speed, the ring approaches a limiting non-uniform shape, whereas in the limit of small load, the ring is narrow and thin with a uniform parabolic profile. Finally, we show that, while for most values of the rotation speed and the load the azimuthal velocity is in the same direction as the rotation of the cylinder, there is a region of parameter space close to the critical solution for sufficiently small rotation speed in which backflow occurs in a small region on the upward-moving side of the cylinder

    Is a "Feminine" Ethic Enough?

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    One aspect of the feminine which has received much attention in recent nontraditional ethical theory (most notably in Nel Noddings' Caring) is the feminine practice of caring for others. The ability of the caring person to "receive" or "pay attention to" the reality of another in order to "feel with" that other is commonly presented as the most crucial ingredient to the caring relation. I argue that however imporant this caring attitude is to ethical relations, an ethics which focuses almost entirely on it is not enough to set us on the path to a moral society if applied within the oppressive social system of patriarchy. A feminist re-vision of this notion of caring is needed to ensure that the care women give to others does not contribute to sustaining patriarchal relations, and that women, too, receive care (from themselves, other women, and men). I offer a vision of such a feminist ethics of caring.Un des aspects du féminin sur lequel les théories éthiques non-traditionnelles se sont beaucoup penchées récemment (notamment dans Caring, de Nel Noddings) est celui de la pratique féminine de "bienveillance" envers son prochain. L'élément principal des rapports entre la personne qui montre cette "bienveillance" et la personne qui la reçoit est le fait que la première soit capable de "capter" la réali té de l'autre, d'y "prêter attention," afin de pouvoir "ressentir" les émotions de cette autre personne. Je soutiens cependant que, bien que cette attitude de "bienveillance" soit très importante dans les relations éthiques, une éthique qui en dépendrait presque exclusivement ne suffirait pas à nous meure sur la voie d’une société morale si elle était pratiquée dans le cadre du système social oppressif du patriarcat. Il est indispensable de procéder à une ré-vision féministre de cette notion de "bienveillance," afin d’assurer que cette bienveillance que les femmes portent à leur prochain ne contribue pas à entretenir des relations patriarcales. Les femmes, elles aussi, sont des êtres qui se concilient la bienveillance d'autrui (d'elles-mêmes, d'autres femmes, et des hommes). Je propose une vision d’une telle "éthique de bienveillance féministe.

    Commentary on Women's Choices: Philosophical Problems Facing Feminism.

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    The rise of the golden city: Los Angeles in the twentieth century

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    At the turn of the twentieth century, Los Angeles was poised to become the premier city on the West Coast.Within thirty years, the boosters, businessmen, and politicians made it a reality. These people believed that the twentieth century belonged to the city of Los Angeles, and they propelled the city into the forefront. They did so by constructing a massive aqueduct system; annexing lands to the east, west, and south of its original borders; developing a harbor; building a massive infrastructure including roads and rail lines; instituting the nation’s first zoning laws; and fostering financial investment. By 1930, the city became the largest in the West, boasting a population of 1,238,084

    Three-dimensional coating and rimming flow: a ring of fluid on a rotating horizontal cylinder

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    The steady three-dimensional flow of a thin, slowly varying ring of Newtonian fluid on either the outside or the inside of a uniformly rotating large horizontal cylinder is investigated. Specifically, we study “full-ring” solutions, corresponding to a ring of continuous, finite and non-zero thickness that extends all the way around the cylinder. In particular, it is found that there is a critical solution corresponding to either a critical load above which no full-ring solution exists (if the rotation speed is prescribed) or a critical rotation speed below which no full-ring solution exists (if the load is prescribed). We describe the behaviour of the critical solution and, in particular, show that the critical flux, the critical load, the critical semi-width and the critical ring profile are all increasing functions of the rotation speed. In the limit of small rotation speed, the critical flux is small and the critical ring is narrow and thin, leading to a small critical load. In the limit of large rotation speed, the critical flux is large and the critical ring is wide on the upper half of the cylinder and thick on the lower half of the cylinder, leading to a large critical load.\ud \ud We also describe the behaviour of the non-critical full-ring solution, and, in particular, show that the semi-width and the ring profile are increasing functions of the load but, in general, non-monotonic functions of the rotation speed. In the limit of large rotation speed, the ring approaches a limiting non-uniform shape, whereas in the limit of small load, the ring is narrow and thin with a uniform parabolic profile. Finally, we show that, while for most values of the rotation speed and the load the azimuthal velocity is in the same direction as the rotation of the cylinder, there is a region of parameter space close to the critical solution for sufficiently small rotation speed in which backflow occurs in a small region on the right-hand side of the cylinder

    Thermoviscous Coating and Rimming Flow

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    A comprehensive description is obtained of steady thermoviscous (i.e. with temperature-dependent viscosity) coating and rimming flow on a uniformly rotating horizontal cylinder that is uniformly hotter or colder than the surrounding atmosphere. It is found that, as in the corresponding isothermal problem, there is a critical solution with a corresponding critical load (which depends, in general, on both the Biot number and the thermoviscosity number) above which no ``full-film'' solutions corresponding to a continuous film of fluid covering the entire outside or inside of the cylinder exist. The effect of thermoviscosity on both the critical solution and the full-film solution with a prescribed load is described. In particular, there are no full-film solutions with a prescribed load M for any value of the Biot number when M is greater than or equal to M_{c0} divided by the square root of f for positive thermoviscosity number and when M is greater than M_{c0} for negative thermoviscosity number, where f is a monotonically decreasing function of the thermoviscosity number and M_{c0} = 4.44272 is the critical load in the constant-viscosity case. It is also found that when the prescribed load M is less than 1.50315 there is a narrow region of the Biot number - thermoviscosity number parameter plane in which backflow occurs
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