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  1. #1
    The Thinker
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    Particles for Momentum

    This is another part of my TOE. Although I'm still not sure of adding it, because it seems to be more abstract and less verifyable than the processes.

    The basic idea is that there is a fifth type of force. This force is generally accepted as not being a force, but being "momentum". I think I should call it inertia, so that people don't get confused. Well this inertia is made of force particles: force carriers: bosons. This type of bosons I have deliberatelly called "inertions".

    I will later post the properties of these particles: charge, mass, spin.....Also the experiments that could be done to verify this and the predictions this allow us to do.

  2. #2
    Raider of the lost time
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    Quote Originally Posted by GUILLE
    I think I should call it inertia
    Are you giving a new definition? Or, are you giving an extension of the physics definition?

    The physics definition of inertia is given at the following link.

    http://scienceworld.wolfram.com/physics/Inertia.html

  3. #3
    The Thinker
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    Yes: my definition is the same as the one given in the link. But I have realised that the best word to define what I mean is momentum. so, the particles I know call "Momentumons" or "momentoms".

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    Raider of the lost time
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    Quote Originally Posted by GUILLE
    But I have realised that the best word to define what I mean is momentum.
    In physics, momentum is already defined by the following link
    http://scienceworld.wolfram.com/physics/Momentum.html

  5. #5
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    Quote Originally Posted by AntonioLao
    In physics, momentum is already defined by the following link
    http://scienceworld.wolfram.com/physics/Momentum.html
    I think this definition is correct. Only that it should be considered a force.

  6. #6
    Raider of the lost time
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    Quote Originally Posted by GUILLE
    Only that it should be considered a force.
    As noted by Newton, force is defined as the time rate of change of momentum

    Newton's second law gives



    which, when m is constant, reduces to the familiar
    see some more about physics' definition of force at

 

 

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