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4: Dynamics

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    • 4.1: Ultrarelativistic particles
      Ultrarelativistic objects are objects moving at nearly c . A good way of thinking about an ultrarelativistic particle is that it’s a particle with a very small mass. For example, the subatomic particle called the neutrino has a very small mass, thousands of times smaller than that of the electron.
    • 4.2: E=mc²
      We now know the relativistic expression for kinetic energy in the limiting case of an ultrarelativistic particle: its energy is proportional to the “stretch factor” D of the Lorentz transformation. What about intermediate cases?
    • 4.3: Relativistic Momentum
      Since mass and energy are equivalent, we must stop talking about a material object’s kinetic energy and consider instead its total energy E, which includes a contribution from its mass. Massless particles always move at v=c , while massive ones always move at v<c .
    • 4.4: Systems with internal structure
      E=mc2 and the four-vector nature of p are both valid for systems with finite spatial extent, provided that the systems are isolated.
    • 4.5: Force
      Force is a concept that is seldom needed in relativity, and that’s why this section is optional.
    • 4.6: Two Applications
    • 4.7: Tachyons and Faster-than-Light (FTL)
      A tachyons are hypothetical particle that always moves faster than light. Most physicists believe that faster-than-light (FTL) particles cannot exist because superluminal transmission of information would violate causality, since it would allow a causal relationship between events that were spacelike in relation to one another, and the timeordering of such events is different according to different observers.
    • 4.E: Dynamics (Exercises)

    This page titled 4: Dynamics is shared under a CC BY-SA 4.0 license and was authored, remixed, and/or curated by Benjamin Crowell 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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