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
    • 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 2 results
    • https://phys.libretexts.org/Bookshelves/Classical_Mechanics/Classical_Mechanics_(Dourmashkin)/01%3A_Introduction_to_Classical_Mechanics/1.01%3A_Introduction
      Alongside this development and refinement of the concept of force and its application to the description of motion, the concept of energy slowly emerged, culminating in the middle of the nineteenth ce...Alongside this development and refinement of the concept of force and its application to the description of motion, the concept of energy slowly emerged, culminating in the middle of the nineteenth century in the discovery of the principle of conservation of energy and its immediate applications to the laws of thermodynamics.
    • https://phys.libretexts.org/Bookshelves/University_Physics/Mechanics_and_Relativity_(Idema)/07%3A_General_Rotational_Motion/7.03%3A_Rotations_About_an_Arbitrary_Axis
      In Chapter 5, we studied the rotation of rigid bodies about an axis of symmetry. For these cases, we have L=Iω, where I is the moment of inertia with respect to t...In Chapter 5, we studied the rotation of rigid bodies about an axis of symmetry. For these cases, we have L=Iω, where I is the moment of inertia with respect to the rotation axis. In this section, we’ll derive the more general form, in which the number I is replaced by a 2-tensor, i.e., a map from a vector space (here R3) into itself, represented by a 3×3 matrix.

    Support Center

    How can we help?