Skip to main content
  • Book
  • © 1999

Differentiable and Complex Dynamics of Several Variables

Part of the book series: Mathematics and Its Applications (MAIA, volume 483)

Buy it now

Buying options

eBook USD 39.99
Price excludes VAT (USA)
  • Available as PDF
  • Read on any device
  • Instant download
  • Own it forever
Softcover Book USD 54.99
Price excludes VAT (USA)
  • Compact, lightweight edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info
Hardcover Book USD 54.99
Price excludes VAT (USA)
  • Durable hardcover edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info

Tax calculation will be finalised at checkout

Other ways to access

This is a preview of subscription content, log in via an institution to check for access.

Table of contents (9 chapters)

  1. Front Matter

    Pages i-ix
  2. Fatou-Julia type theory

    • Pei-Chu Hu, Chung-Chun Yang
    Pages 1-37
  3. Ergodic theorems and invariant sets

    • Pei-Chu Hu, Chung-Chun Yang
    Pages 39-62
  4. Hyperbolicity in differentiable dynamics

    • Pei-Chu Hu, Chung-Chun Yang
    Pages 63-97
  5. Some topics in dynamics

    • Pei-Chu Hu, Chung-Chun Yang
    Pages 99-136
  6. Hyperbolicity in complex dynamics

    • Pei-Chu Hu, Chung-Chun Yang
    Pages 137-177
  7. Iteration theory on â„™m

    • Pei-Chu Hu, Chung-Chun Yang
    Pages 179-202
  8. Complex dynamics in â„‚m

    • Pei-Chu Hu, Chung-Chun Yang
    Pages 203-232
  9. Foundations of differentiable dynamics

    • Pei-Chu Hu, Chung-Chun Yang
    Pages 233-274
  10. Foundations of complex dynamics

    • Pei-Chu Hu, Chung-Chun Yang
    Pages 275-318
  11. Back Matter

    Pages 319-341

About this book

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.

Authors and Affiliations

  • Shandong University, Jinan, China

    Pei-Chu Hu

  • The Hong Kong University of Science and Technology, Kowloon, Hong Kong

    Chung-Chun Yang

Bibliographic Information

Buy it now

Buying options

eBook USD 39.99
Price excludes VAT (USA)
  • Available as PDF
  • Read on any device
  • Instant download
  • Own it forever
Softcover Book USD 54.99
Price excludes VAT (USA)
  • Compact, lightweight edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info
Hardcover Book USD 54.99
Price excludes VAT (USA)
  • Durable hardcover edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info

Tax calculation will be finalised at checkout

Other ways to access