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Equipartitioning of energy

Each hamionic temi in the Hamiltonian contributes k T to the average energy of the system, which is the theorem of the equipartition of energy. Since this is also tire internal energy U of the system, one can compute the heat capacity... [Pg.392]

A well known example of this is obtained by settmg % = p a, a=x, y, z, any component of momentum, giving the equipartition-of-energy relation... [Pg.2248]

This rule conforms with the principle of equipartition of energy, first enunciated by Maxwell, that the heat capacity of an elemental solid, which reflected the vibrational energy of a tliree-dimensional solid, should be equal to 3f JK moH The anomaly that the free electron dreory of metals described a metal as having a tliree-dimensional sUmcture of ion-cores with a three-dimensional gas of free electrons required that the electron gas should add anodier (3/2)7 to the heat capacity if the electrons behaved like a normal gas as described in Maxwell s kinetic theory, whereas die quanmtii theory of free electrons shows that diese quantum particles do not contribute to the heat capacity to the classical extent, and only add a very small component to the heat capacity. [Pg.164]

Now let the silver be supposed to be surrounded by a monatomic gas, such as helium. The atoms of the gas, when they collide with those of the solid, will impart kinetic energy to them. According to Maxwell s Law of Equipartition of Energy, two bodies are in temperature equilibrium when the mean kinetic energy for each degree of freedom of motion of each atom is the same in both. The atoms of the solid and those of the gas have three degrees of freedom each to each degree corresponds the kinetic... [Pg.519]

There is, however, a fatal objection to the theory of Boltzmann. At very low temperatures the oscillations will be small, and should conform to the theory. But the atomic heats, instead of approaching the limit 5 955 at low temperatures, diminish very rapidly, and in the case of diamond the specific heat is already inappreciable at the temperature of liquid air. A new point of view is therefore called for, and it is a priori very probable that this will consist of a replacement of the hypothesis of Equipartition of Energy adopted by Boltzmann. This supposition has been verified, and the new law of partition of energy derived... [Pg.519]

The atoms are of a complex structure made up of positive nuclei and electrons, of which the latter, at least, are in very rapid motion. If we assume that the electrons are 1/1800 the mass of hydrogen atoms and that they obey the same laws of motion as other atoms, their average velocity would be about sixty times the velocity of molecules of hydrogen (H2). I will not attempt to discuss here the question whether the law of equipartition of energy actually holds for electrons. [Pg.3]

Since equipartition of energy requires that the kinetic energy corresponding to each transnational degree of freedom is kTI2, where k is Boltzmann s constant and T is the thermodynamic absolute temperature, three degrees of freedom corre-... [Pg.636]

Given equipartition of energy (i.e., mwfrX2 = muj2Y2), the relative amplitudes of the displacements, momenta, and forces are... [Pg.294]

The Boltzmann distribution for quantum systems is totally different in concept from the principle of classical equipartition of energy. The main difference comes from the way in which the energies of the various modes vary with quantum number ... [Pg.276]

J.C. Maxwell saw these atoms as capable of internal vibrations 9). Atoms had some form of internal stracture and were not static If there were internal modes of motion in the atoms, Boltzmarm predicted that equipartition of energy would lead to an increased heat capacity. Maxwell worried about the missing heat capacity due to these motions as well. Maxwell died before an explanation of the... [Pg.92]

Boltzmann s Law. The law of the equipartition of energy to a molecular system. Stef an-Boltzmann Law states that the total energy radiated from a black body is proportional to its absolute temp raised to the fourth power. It is expressed by E= a (T4 - T ) where E - total energy in ergs,... [Pg.222]


See other pages where Equipartitioning of energy is mentioned: [Pg.1070]    [Pg.324]    [Pg.5]    [Pg.180]    [Pg.59]    [Pg.59]    [Pg.60]    [Pg.1034]    [Pg.491]    [Pg.524]    [Pg.540]    [Pg.498]    [Pg.657]    [Pg.644]    [Pg.61]    [Pg.5]    [Pg.263]    [Pg.451]    [Pg.5]    [Pg.53]    [Pg.3]    [Pg.22]    [Pg.216]    [Pg.208]    [Pg.96]    [Pg.14]    [Pg.420]    [Pg.165]    [Pg.59]    [Pg.59]    [Pg.60]   


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