A Collection of Problems in Illustration of the Principles of Theoretical Hydrostatics and Hydrodynamics |
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Page v
... homogeneous fluids II . - Bodies floating in incompressible heterogeneous fluids . III . - Bodies floating under the action of elastic fluids • 24 35 39 39 49 59 62 CHAPTER V. Equilibrium of Solid Bodies floating under constraint .
... homogeneous fluids II . - Bodies floating in incompressible heterogeneous fluids . III . - Bodies floating under the action of elastic fluids • 24 35 39 39 49 59 62 CHAPTER V. Equilibrium of Solid Bodies floating under constraint .
Page vii
... in incompressible fluids II . - Motion of bodies subject to the action of aeriform fluids III . - Small oscillations of floating bodies 186 194 215 218 221 } HYDROSTATICS . CHAPTER I. NORMAL PRESSURE OF FLUIDS . CONTENTS . vii.
... in incompressible fluids II . - Motion of bodies subject to the action of aeriform fluids III . - Small oscillations of floating bodies 186 194 215 218 221 } HYDROSTATICS . CHAPTER I. NORMAL PRESSURE OF FLUIDS . CONTENTS . vii.
Page 3
... action by the discussion of the following question , which , as having relation to the fundamental principles of the transmission of hydrostatical pressure , and as serving to exemplify the accuracy of his mechanical ideas of fluids ...
... action by the discussion of the following question , which , as having relation to the fundamental principles of the transmission of hydrostatical pressure , and as serving to exemplify the accuracy of his mechanical ideas of fluids ...
Page 39
... instead of the positive direction , we must replace A by - A : analogous remarks are applicable to the actions of Y and Z. Multiplying L , M , N , by X , CHAPTER III Resultant pressures of fluids on curved surfaces of immersed solids 39.
... instead of the positive direction , we must replace A by - A : analogous remarks are applicable to the actions of Y and Z. Multiplying L , M , N , by X , CHAPTER III Resultant pressures of fluids on curved surfaces of immersed solids 39.
Page 61
... depth equal to the diameter of the sphere , will rest just totally immersed in the fluid . - The required power is 3 or 8 . SECTION III . Bodies floating under the action of Elastic EQUILIBRIUM OF SOLID BODIES FLOATING FREELY . 61.
... depth equal to the diameter of the sphere , will rest just totally immersed in the fluid . - The required power is 3 or 8 . SECTION III . Bodies floating under the action of Elastic EQUILIBRIUM OF SOLID BODIES FLOATING FREELY . 61.
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Common terms and phrases
Albert Girard altitude angular velocity aperture axem axes axis vertical base Bernoulli body Bossut Bossut Traité Cambridge centre of gravity centre of pressure coinciding cone cos² cube Daniel Bernoulli denote the density denote the length depth determine distance dx dy Edition efflux elastic equal equation filled with fluid floating fluid displaced force free surface given hemisphere Hence humidum Hydrodynamique immersed vertically inclination incompressible fluid James Bernoulli lamina late Fellow latus rectum motion parabola parallel particles portion position of equilibrium position of rest problem quæ ratio required pressure resultant pressure right angles sesquialterum sin² small orifice solid cylinder specific gravity sphere supposed tangent Treatise triangle Trinity College unit of pressure University of Cambridge vertex vertical line vessel volume weight whole pressure
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