From: ram@zedat.fu-berlin.de   
      
   Mikko wrote or quoted:   
   >On 2024-06-18 18:25:10 +0000, Stefan Ram said:   
   >>. Here's a quotation from "Quora":   
   . . .   
   >>|It turns out that it is a general law of nature that physical   
   >>|systems always "want" to be in the state of lowest possible   
   >>|energy.   
   . . .   
   >Not exactly. The law is that entropy always increases, which means   
   >that energy becomes more evenly distributed.   
      
    The heat death (the conversion of all forms of energy into   
    heat energy) is rather something long-term, but one can also   
    be interested in the dynamics within shorter periods of time.   
      
    At the system boundaries, the flow of extensive quantities   
    is determined by the difference of the intensive quantities   
    (potentials).   
      
    Thus, (positive) electric charge (extensive quantity)   
    flows, for example, from the system with the higher   
    electric potential (intensive quantity) to the system   
    with the smaller electric potential.   
      
    Yes, and in doing so, the total energy in the two systems would   
    become smaller. But since energy must not be destroyed, it must   
    be converted into another form. If the systems cannot exchange any   
    other forms of energy, then only the generation of entropy remains.   
    And it then flows rather to the colder of the two systems.   
      
    So you were right insofar as one must take entropy into account.   
      
    Here is the formulation with potential differences, once without   
    and once with "want":   
      
    Without "want": When two systems come into contact, an extensive   
    quantity flows to the system with the smaller associated potential.   
      
    With "want": Every system wants to give off its extensive   
    quantities (which reduces its energy), but this is only   
    possible if the system finds another system in which the   
    potential associated with the extensive quantity is smaller.   
      
    If we regard a system with a small potential as "weak"   
    and a system with a large potential as "strong", we can say   
    that every system wants to impose its energy in the form of   
    extensive quantities on other systems, but it only succeeds   
    in doing so if it finds a weaker system.   
      
    The concept of the thermodynamic potential, which determines   
    the direction of the flow of extensive quantities, was still   
    missing from your explanations.   
      
    (I'm not particularly interested in the Higgs field itself, as   
    I wrote, but if I imagine the Higgs field and another field, and   
    each wants to give away its energy, then I can't find suitable   
    forms of energy with their associated extensive and intensive   
    quantities that would help me predict the temporal evolution.)   
      
   --- SoupGate-Win32 v1.05   
    * Origin: you cannot sedate... all the things you hate (1:229/2)   
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