Editing Frenkel line
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of transverse excitations is <math> 1 k_B </math>. Therefore at the Frenkel | of transverse excitations is <math> 1 k_B </math>. Therefore at the Frenkel | ||
line, where transverse excitations vanish, the isochoric heat | line, where transverse excitations vanish, the isochoric heat | ||
capacity per particle should be <math> c_V=2 k_B </math>, a direct prediction from the phonon theory of liquid thermodynamics | capacity per particle should be <math> c_V=2 k_B </math>, a direct prediction from the phonon theory of liquid thermodynamics <ref> [http://www.nature.com/srep/2012/120524/srep00421/full/srep00421.html D. Bolmatov, V. V. Brazhkin, and K. Trachenko "The phonon theory of liquid thermodynamics", Scientific Reports '''2''' 421 (2012)]</ref>, <ref> [http://www.nature.com/ncomms/2013/130816/ncomms3331/full/ncomms3331.html Dima Bolmatov, V. V. Brazhkin, and K. Trachenko "Thermodynamic behaviour of supercritical matter", Scientific Reports '''4''' 2331 (2013)]</ref>, <ref> [http://physicsworld.com/cws/article/news/2012/jun/13/phonon-theory-sheds-light-on-liquid-thermodynamics "Phonon theory sheds light on liquid thermodynamics", PhysicsWorld, 2012]</ref>. | ||
<ref> [http:// | |||
<ref> [http://physicsworld.com/cws/article/news/2012/jun/13/phonon-theory-sheds-light-on-liquid-thermodynamics | |||
Crossing the Frenkel line leads also to some structural crossovers in fluids | Crossing the Frenkel line leads also to some structural crossovers in fluids |