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Differentiable and Complex Dynamics of Several Variables by Pei-Chu Hu (English)

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Item specifics

Condition
Brand New: A new, unread, unused book in perfect condition with no missing or damaged pages. See all condition definitionsopens in a new window or tab
ISBN-13
9780792357711
Book Title
Differentiable and Complex Dynamics of Several Variables
ISBN
9780792357711
Subject Area
Mathematics
Publication Name
Differentiable and Complex Dynamics of Several Variables
Publisher
Springer Netherlands
Item Length
9.3 in
Subject
Differential Equations / General, Geometry / Differential, Mathematical Analysis, Complex Analysis
Publication Year
1999
Series
Mathematics and Its Applications Ser.
Type
Textbook
Format
Hardcover
Language
English
Author
Chung-Chun Yang, Pei-Chu Hu
Item Weight
52.9 Oz
Item Width
6.1 in
Number of Pages
X, 342 Pages

About this product

Product Identifiers

Publisher
Springer Netherlands
ISBN-10
079235771X
ISBN-13
9780792357711
eBay Product ID (ePID)
10038752985

Product Key Features

Number of Pages
X, 342 Pages
Publication Name
Differentiable and Complex Dynamics of Several Variables
Language
English
Subject
Differential Equations / General, Geometry / Differential, Mathematical Analysis, Complex Analysis
Publication Year
1999
Type
Textbook
Author
Chung-Chun Yang, Pei-Chu Hu
Subject Area
Mathematics
Series
Mathematics and Its Applications Ser.
Format
Hardcover

Dimensions

Item Weight
52.9 Oz
Item Length
9.3 in
Item Width
6.1 in

Additional Product Features

Intended Audience
Scholarly & Professional
LCCN
99-027065
Dewey Edition
21
Series Volume Number
483
Number of Volumes
1 vol.
Illustrated
Yes
Dewey Decimal
515/.94
Table Of Content
1 Fatou-Julia type theory.- 2 Ergodic theorems and invariant sets.- 3 Hyperbolicity in differentiable dynamics.- 4 Some topics in dynamics.- 5 Hyperbolicity in complex dynamics.- 6 Iteration theory on ?m.- 7 Complex dynamics in ?m.- A Foundations of differentiable dynamics.- B Foundations of complex dynamics.
Synopsis
The development of dynamics theory began with the work of Isaac Newton. In his theory the most basic law of classical mechanics is f = ma, which describes the motion n in IR. of a point of mass m under the action of a force f by giving the acceleration a. If n the position of the point is taken to be a point x E IR., and if the force f is supposed to be a function of x only, Newton's Law is a description in terms of a second-order ordinary differential equation: J2x m dt = f(x). 2 It makes sense to reduce the equations to first order by defining the velo city as an extra n independent variable by v =: i; = E IR. . Then x = v, mv = f(x). L. Euler, J. L. Lagrange and others studied mechanics by means of an analytical method called analytical dynamics. Whenever the force f is represented by a gradient vector field f = - \lU of the potential energy U, and denotes the difference of the kinetic energy and the potential energy by 1 L(x, v) = 2'm(v, v) - U(x), the Newton equation of motion is reduced to the Euler-Lagrange equation are used as the variables, the Euler-Lagrange equation can be If the momenta y written as . 8L y= 8x' Further, W. R., The development of dynamics theory began with the work of Isaac Newton. In his theory the most basic law of classical mechanics is f = ma, which describes the motion n in IR. of a point of mass m under the action of a force f by giving the acceleration a. If n the position of the point is taken to be a point x E IR. , and if the force f is supposed to be a function of x only, Newton's Law is a description in terms of a second-order ordinary differential equation: J2x m dt = f(x). 2 It makes sense to reduce the equations to first order by defining the velo city as an extra n independent variable by v = :i; = ~~ E IR. . Then x = v, mv = f(x). L. Euler, J. L. Lagrange and others studied mechanics by means of an analytical method called analytical dynamics. Whenever the force f is represented by a gradient vector field f = - \lU of the potential energy U, and denotes the difference of the kinetic energy and the potential energy by 1 L(x,v) = 2'm(v,v) - U(x), the Newton equation of motion is reduced to the Euler-Lagrange equation ~~ are used as the variables, the Euler-Lagrange equation can be If the momenta y written as . 8L y= 8x' Further, W. R.
LC Classification Number
QA614-614.97

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