Isbn: 9783540102236 - solitons: mathematical methods for physicists: 19 (14 risultati)

gebundene Ausgabe. Condizione: Gut. 192 Seiten Der Erhaltungszustand des hier angebotenen Werks ist trotz seiner Bibliotheksnutzung sehr sauber und kann entsprechende Merkmale aufweisen (Rückenschild, Instituts-Stempel.). In ENGLISCHER Sprache. Sprache: Englisch Gewicht in Gramm: 420.

Paperback. Condizione: Gut. VIII, 192 S.; Ill. Ex.-Libr., Good condition. Sprache: Englisch Gewicht in Gramm: 415.

Hardcover. Condizione: Sehr gut. Berlin, Springer 1981. gr.8°. 31 figs. VIII, 192 p. Hardbound. (corners slihtly bumped).- Springer Series in Solid-State Science 19.

Hardcover. Condizione: Gut. 2., corr. print. Ex-library with stamp and library-signature. GOOD condition, some traces of use. C-02900 354010223X Sprache: Englisch Gewicht in Gramm: 1050.

24 cm, VIII, 192 pages, with 31 Figures, brauner Pappband. Kapitale und Ecken leicht berieben, viele Markeranstreichungen auf den ersten ca. 30 Seiten, leichter Kellergeruch, insgesamt gut erhalten. Springer Series in Solid-State Sciences 19. Sprache: Deutsch.

Broschiert. Condizione: Sehr gut. Auflage: Second Corrected Printing. 192 Seiten Sehr gutes frisches Exemplar. Ungelesen. Sprache: Englisch Gewicht in Gramm: 320.

Condizione: New. In English.

Paperback. Condizione: Brand New. second printing edition. 204 pages. 9.25x6.10x0.46 inches. In Stock.

Taschenbuch. Condizione: Neu. Druck auf Anfrage Neuware - Printed after ordering - 1.1 Why Study Solitons The last century of physics, which was initiated by Maxwell's completion of the theory of electromagnetism, can, with some justification, be called the era of linear physi cs. ~Jith few excepti ons, the methods of theoreti ca 1 phys ics have been dominated by linear equations (Maxwell, Schrodinger), linear mathematical objects (vector spaces, in particular Hilbert spaces), and linear methods (Fourier transforms, perturbation theory, linear response theory) . Naturally the importance of nonlinearity, beginning with the Navier-Stokes equations and continuing to gravitation theory and the interactions of par ticles in solids, nuclei, and quantized fields, was recognized. However, it was hardly possible to treat the effects of nonlinearity, except as a per turbation to the basis solutions of the linearized theory. During the last decade, it has become more widely recognized in many areas of 'field physics' that nonlinearity can result in qualitatively new phenom ena which cannot be constructed via perturbation theory starting from linear ized equations. By 'field physics' we mean all those areas of theoretical physics for which the description of physical phenomena leads one to consider field equations, or partial differential equations of the form (1.1.1) ~t or ~tt = F(~, ~x . ) for one- or many-component 'fields' Ht,x,y, . ) (or their quantum analogs).…

Paperback. Condizione: Very Good. Dust Jacket may NOT BE INCLUDED.CDs may be missing. SHIPS FROM MULTIPLE LOCATIONS. book.

Condizione: gut. 1981. Solitons. Mathematical Methods for Physicists. (= Springer Series in Solid-State Sciences - Volume 19). In deutscher Sprache. pages.

Taschenbuch. Condizione: Neu. This item is printed on demand - it takes 3-4 days longer - Neuware -1.1 Why Study Solitons The last century of physics, which was initiated by Maxwell's completion of the theory of electromagnetism, can, with some justification, be called the era of linear physi cs. ~Jith few excepti ons, the methods of theoreti ca 1 phys ics have been dominated by linear equations (Maxwell, Schrodinger), linear mathematical objects (vector spaces, in particular Hilbert spaces), and linear methods (Fourier transforms, perturbation theory, linear response theory) . Naturally the importance of nonlinearity, beginning with the Navier-Stokes equations and continuing to gravitation theory and the interactions of par ticles in solids, nuclei, and quantized fields, was recognized. However, it was hardly possible to treat the effects of nonlinearity, except as a per turbation to the basis solutions of the linearized theory. During the last decade, it has become more widely recognized in many areas of 'field physics' that nonlinearity can result in qualitatively new phenom ena which cannot be constructed via perturbation theory starting from linear ized equations. By 'field physics' we mean all those areas of theoretical physics for which the description of physical phenomena leads one to consider field equations, or partial differential equations of the form (1.1.1) ~t or ~tt = F(~, ~x . ) for one- or many-component 'fields' Ht,x,y, . ) (or their quantum analogs). 204 pp. Englisch. …

Condizione: New. Dieser Artikel ist ein Print on Demand Artikel und wird nach Ihrer Bestellung fuer Sie gedruckt. 1. Introduction.- 1.1 Why Study Solitons.- 1.2 Basic Concepts Illustrated by Simple Examples.- 2. The Korteweg-de Vries Equation (KdV-Equation).- 2.1 The Physical Meaning of the KdV Equation.- 2.2 The KdV Equation as a Lagrangian Field Theory: Symmetries.-.…

Taschenbuch. Condizione: Neu. This item is printed on demand - Print on Demand Titel. Neuware -1.1 Why Study Solitons The last century of physics, which was initiated by Maxwell's completion of the theory of electromagnetism, can, with some justification, be called the era of linear physi cs. ~Jith few excepti ons, the methods of theoreti ca 1 phys ics have been dominated by linear equations (Maxwell, Schrodinger), linear mathematical objects (vector spaces, in particular Hilbert spaces), and linear methods (Fourier transforms, perturbation theory, linear response theory) . Naturally the importance of nonlinearity, beginning with the Navier-Stokes equations and continuing to gravitation theory and the interactions of par ticles in solids, nuclei, and quantized fields, was recognized. However, it was hardly possible to treat the effects of nonlinearity, except as a per turbation to the basis solutions of the linearized theory. During the last decade, it has become more widely recognized in many areas of 'field physics' that nonlinearity can result in qualitatively new phenom ena which cannot be constructed via perturbation theory starting from linear ized equations. By 'field physics' we mean all those areas of theoretical physics for which the description of physical phenomena leads one to consider field equations, or partial differential equations of the form (1.1.1) ~t or ~tt = F(~, ~x . ) for one- or many-component 'fields' Ht,x,y, . ) (or their quantum analogs).Springer-Verlag KG, Sachsenplatz 4-6, 1201 Wien 204 pp. Englisch.…