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3: Momentum and Angular Momentum

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    Chapter 2 introduced energy as a mathematical construct that has turned out to be very useful. There are two other conserved quantities that show up throughout all of our theories of physics. Both of those have to do with motion, but are different from kinetic energy. These other quantities are momentum and angular momentum.

    • 3.1: Vectors
      Both momentum and angular momentum are vector quantities. Later, we’ll be talking about a more abstract form of vector used to represent the state of quantum systems. Here, we’re talking about a special kind of vector, a vector in regular old 3d-space. Distinguish these from more general vectors, I shall call them 3-vectors, in reference to 3-dimensional space.
    • 3.2: Momentum
      Kinetic energy is a quantity that’s associated with motion. However, kinetic energy itself is not always conserved. If a cue pool ball runs into another ball, and the cue ball stops dead, the other ball goes off with the same speed that the cue ball came in at.
    • 3.3: Angular Momentum
      Imagine the following experiment. You’ve got, somehow, a frictionless plane. (These frictionless planes are common in physics, but much more difficult to manufacture in the real world! If you wish, you can imagine it as an air hockey table, or a particularly smooth and slippery sheet of ice or teflon.)


    This page titled 3: Momentum and Angular Momentum is shared under a CC BY-SA 3.0 license and was authored, remixed, and/or curated by Rob Knop via source content that was edited to the style and standards of the LibreTexts platform; a detailed edit history is available upon request.

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