Published by Cambridge University Press (edition 1), 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
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Published by Cambridge University Press (edition 1), 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
Language: English
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Published by Cambridge University Press, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
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Published by Cambridge University Press, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
Language: English
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Published by Cambridge University Press, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
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Published by Cambridge University Press CUP, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
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Published by Cambridge University Press, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
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Published by Cambridge University Press, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
Language: English
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Published by Cambridge University Press, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
Language: English
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Published by Cambridge University Press, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
Language: English
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Published by Cambridge University Press, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
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Published by Cambridge University Press, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
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Published by Cambridge University Press, 2007
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Published by Cambridge University Press, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
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Published by Cambridge University Press, Cambridge, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
Language: English
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First Edition
Hardcover. Condition: new. Hardcover. This book illustrates how potential flows enter into the general theory of motions of viscous and viscoelastic fluids. Traditionally, the theory of potential flow is presented as a subject called 'potential flow of an inviscid fluid'; when the fluid is incompressible these fluids are, curiously, said to be 'perfect' or 'ideal'. This type of presentation is widespread; it can be found in every book on fluid mechanics, but it is flawed. It is never necessary and typically not useful to put the viscosity of fluids in potential (irrotational) flow to zero. The dimensionless description of potential flows of fluids with a nonzero viscosity depends on the Reynolds number, and the theory of potential flow of an inviscid fluid can be said to rise as the Reynolds number tends to infinity. The theory given here can be described as the theory of potential flows at finite and even small Reynolds numbers. The goal of this book is to show how potential flows enter into the general theory of motions of viscous and viscoelastic fluids. Traditionally, the theory of potential flows is thought to apply to idealized fluids without viscosity. Here we show how to apply this theory to real fluids that are viscous. The theory is applied to problems of the motion of bubbles; to the decay of waves on interfaces between fluids; to capillary, Rayleigh-Taylor, and Kelvin-Hemholtz instabilities; to viscous effects in acoustics; to boundary layers on solids at finite Reynolds numbers; to problems of stress-induced cavitation; and to the creation of microstructures in the flow of viscous and viscoelastic liquids. Shipping may be from multiple locations in the US or from the UK, depending on stock availability.
Published by Cambridge University Press, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
Language: English
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Published by Cambridge University Press, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
Language: English
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Published by Cambridge University Press, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
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Published by Cambridge University Press, Cambridge, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
Language: English
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First Edition
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Add to basketHardcover. Condition: new. Hardcover. This book illustrates how potential flows enter into the general theory of motions of viscous and viscoelastic fluids. Traditionally, the theory of potential flow is presented as a subject called 'potential flow of an inviscid fluid'; when the fluid is incompressible these fluids are, curiously, said to be 'perfect' or 'ideal'. This type of presentation is widespread; it can be found in every book on fluid mechanics, but it is flawed. It is never necessary and typically not useful to put the viscosity of fluids in potential (irrotational) flow to zero. The dimensionless description of potential flows of fluids with a nonzero viscosity depends on the Reynolds number, and the theory of potential flow of an inviscid fluid can be said to rise as the Reynolds number tends to infinity. The theory given here can be described as the theory of potential flows at finite and even small Reynolds numbers. The goal of this book is to show how potential flows enter into the general theory of motions of viscous and viscoelastic fluids. Traditionally, the theory of potential flows is thought to apply to idealized fluids without viscosity. Here we show how to apply this theory to real fluids that are viscous. The theory is applied to problems of the motion of bubbles; to the decay of waves on interfaces between fluids; to capillary, Rayleigh-Taylor, and Kelvin-Hemholtz instabilities; to viscous effects in acoustics; to boundary layers on solids at finite Reynolds numbers; to problems of stress-induced cavitation; and to the creation of microstructures in the flow of viscous and viscoelastic liquids. Shipping may be from our UK warehouse or from our Australian or US warehouses, depending on stock availability.
Published by Cambridge University Press, Cambridge, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
Language: English
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First Edition
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Add to basketHardcover. Condition: new. Hardcover. This book illustrates how potential flows enter into the general theory of motions of viscous and viscoelastic fluids. Traditionally, the theory of potential flow is presented as a subject called 'potential flow of an inviscid fluid'; when the fluid is incompressible these fluids are, curiously, said to be 'perfect' or 'ideal'. This type of presentation is widespread; it can be found in every book on fluid mechanics, but it is flawed. It is never necessary and typically not useful to put the viscosity of fluids in potential (irrotational) flow to zero. The dimensionless description of potential flows of fluids with a nonzero viscosity depends on the Reynolds number, and the theory of potential flow of an inviscid fluid can be said to rise as the Reynolds number tends to infinity. The theory given here can be described as the theory of potential flows at finite and even small Reynolds numbers. The goal of this book is to show how potential flows enter into the general theory of motions of viscous and viscoelastic fluids. Traditionally, the theory of potential flows is thought to apply to idealized fluids without viscosity. Here we show how to apply this theory to real fluids that are viscous. The theory is applied to problems of the motion of bubbles; to the decay of waves on interfaces between fluids; to capillary, Rayleigh-Taylor, and Kelvin-Hemholtz instabilities; to viscous effects in acoustics; to boundary layers on solids at finite Reynolds numbers; to problems of stress-induced cavitation; and to the creation of microstructures in the flow of viscous and viscoelastic liquids. Shipping may be from our Sydney, NSW warehouse or from our UK or US warehouse, depending on stock availability.
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Add to basketHardcover. Condition: Brand New. 1st edition. 497 pages. 10.00x7.25x1.00 inches. In Stock.
Published by Cambridge University Press, 2007
ISBN 10: 0521873371 ISBN 13: 9780521873376
Language: English
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Add to basketBuch. Condition: Neu. Druck auf Anfrage Neuware - Printed after ordering - This book illustrates how potential flows enter into the general theory of motions of viscous and viscoelastic fluids. Traditionally, the theory of potential flow is presented as a subject called 'potential flow of an inviscid fluid'; when the fluid is incompressible these fluids are, curiously, said to be 'perfect' or 'ideal'. This type of presentation is widespread; it can be found in every book on fluid mechanics, but it is flawed. It is never necessary and typically not useful to put the viscosity of fluids in potential (irrotational) flow to zero. The dimensionless description of potential flows of fluids with a nonzero viscosity depends on the Reynolds number, and the theory of potential flow of an inviscid fluid can be said to rise as the Reynolds number tends to infinity. The theory given here can be described as the theory of potential flows at finite and even small Reynolds numbers.
Published by Cambridge University Press (2008), Cambridge, 2008
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Add to basketorig.boards Minor rubbing. An ink mark to bottom page-edge. VG. 24x15cm, xvii,497 pp., Series: Cambridge Aerospace Series, 21. "This book illustrates how potential flows enter into the general theory of motions of viscous and viscoelastic fluids. Traditionally, the theory of potential flow is presented as a subject called 'potential flow of an inviscid fluid'; when the fluid is incompressible these fluids are, curiously, said to be 'perfect' or 'ideal'. This type of presentation is widespread; it can be found in every book on fluid mechanics, but it is flawed. It is never necessary and typically not useful to put the viscosity of fluids in potential (irrotational) flow to zero. The dimensionless description of potential flows of fluids with a nonzero viscosity depends on the Reynolds number, and the theory of potential flow of an inviscid fluid can be said to rise as the Reynolds number tends to infinity. The theory given here can be described as the theory of potential flows at finite and even small Reynolds numbers" - publisher's description. Minor rubbing. An ink mark to bottom page-edge. VG.
Published by Cambridge University Press, New York, 2007
Language: French
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First Edition
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Add to basketOriginalpappband. 24 cm. Condition: Wie neu. First published. XVI, 497 Seiten. FRISCHES, SEHR schönes Exemplar der ERSTAUSGABE. VERY fresh copy. (We offer a lot of books on PHYSICS and MATHEMATICS on stock in EXCELLENT shape). Sprache: Französisch Gewicht in Gramm: 1005.
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Add to basketHardcover. Condition: Brand New. 1st edition. 497 pages. 10.00x7.25x1.00 inches. In Stock. This item is printed on demand.
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Add to basketCondition: New. Dieser Artikel ist ein Print on Demand Artikel und wird nach Ihrer Bestellung fuer Sie gedruckt. Traditionally, the theory of potential flows is thought to apply to fluids without viscosity. This book illustrates how to apply this theory to real fluids that are viscous.Über den AutorDaniel Joseph is a professor of Aerospace.