Loading [MathJax]/jax/output/HTML-CSS/jax.js
Skip to main content
Library homepage
 

Text Color

Text Size

 

Margin Size

 

Font Type

Enable Dyslexic Font
Physics LibreTexts

Search

  • Filter Results
  • Location
  • Classification
    • Article type
    • Author
    • Embed Hypothes.is?
    • Embebbed CalcPlot3D?
    • Cover Page
    • License
    • Show TOC
    • Transcluded
    • OER program or Publisher
    • Student Analytics
    • Autonumber Section Headings
    • License Version
    • Print CSS
      • Screen CSS
      • PrintOptions
    • Include attachments
    Searching in
    About 1 results
    • https://phys.libretexts.org/Bookshelves/Classical_Mechanics/Graduate_Classical_Mechanics_(Fowler)/07%3A_Time_Evolution_in_Phase_Space-__Poisson_Brackets_and_Constants_of_the_Motion/7.04%3A_Poissons_Theorem
      If f and g are two constants of the motion (i.e., they both have zero Poisson brackets with the Hamiltonian), then the Poisson bracket is also a constant of...If f and g are two constants of the motion (i.e., they both have zero Poisson brackets with the Hamiltonian), then the Poisson bracket is also a constant of the motion. \end{equation}\) or it could be a function of the original variables. But sometimes it’s a new constant of motion. If f,g are time-independent, the proof follows immediately from Jacobi’s identity. A proof for time dependent functions is given in Landau—it’s not difficult.

    Support Center

    How can we help?