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Planck constant quantum theory

In the optical case the transition amounts to taking wavelength into account - in the mechanical case Planck s constant becomes a factor, also in the short-wavelength region. There is no implication that the classical equations describe fundamentally different situations. They are simply less detailed than their non-classical analogues and more convenient to use in the macroscopic world. The two sets of equations deal with the same concepts at different levels of refinement. Apart from Planck s constant quantum theory does not introduce any additional concepts, unknown to classical theory, but it has the ability to explain some experimental results that baffled classical science. [Pg.104]

To explain the photoelectric effect, Einstein assumed that the radiant energy striking the metal surface behaves like a stream of tiny energy packets. Each packet, which is like a particle of energy, is called a photon. Extending Planck s quantum theory, Einstein deduced that each photon must have an energy equal to Planck constant times the frequency of the light ... [Pg.217]

Briefly explain Planck s quantum theory and explain what a quantum is. What are the units for Planck s constant ... [Pg.312]

Differences in the physicochemical properties of isotopes arise as a result of quantum mechanical effects. Figure 1.3 shows schematically the energy of a diatomic molecule, as a function of the distance between the two atoms. According to the quantum theory, the energy of a molecule is restricted to certain discrete energy levels. The lowest level is not at the minimum of the energy curve, but above it by an amount 1/2/tv where h is Planck s constant and v is the frequency with... [Pg.5]

The finitencss of Planck s constant ft and its resulting implications laid the foundations of quantum theory. Quantum theory, like Hie special theory of relativity, was discovered through experiments on electromagnetic phenomena and their theoretical interpretations. [Pg.1393]

The development of quantum theory, particularly of quantum mechanics, forced certain changes in statistical mechanics. In the development of the resulting quantum statistics, the phase space is divided into cells of volume hf. where h is the Planck constant and / is the number of degrees of freedom. In considering the permutations of the molecules, it is recognized that the interchange of two identical particles does not lead to a new state. With these two new ideas, one arrives at the Bose-Einstein statistics. These statistics must be further modified for particles, such as electrons, to which the Pauli exclusion principle applies, and the Fermi-Dirac statistics follow. [Pg.1539]

A full explanation of the properties of light requires both the wave theory of electromagnetic radiation and the quantum theory. Most photochemical processes are best understood in terms of the quantum theory, which says that light is made up of discrete particles called quanta or photons. Each quantum carries an amount of energy, S, determined by the wavelength of the light, A. Equation 13.1, in which h is Planck s constant and c is the speed of light in a vacuum,... [Pg.681]

In order to explain the diffraction of radiation on the quantum theory, the writer proposed1 an hypothesis according to which the momenta of the radiation quanta are transferred to the diffracting material in multiples of Ifija where h is Planck s action constant and a is a grating space." The momenta of a quantum transferred in the directions of three axes may be written... [Pg.1]

Bohm s failure to give an adequate explanation to support the pilot-wave proposal does not diminish the importance of the quantum-potential concept. In all forms of quantum theory it is the appearance of Planck s constant that signals non-classical behaviour, hence the common, but physically meaningless, proposition that the classical/quantum limit appears as h —> 0. The actual limiting condition is Vq —> 0, which turns the quantum-mechanical... [Pg.110]

The 1998 adjustment of the values of the fundamental physical constants has been carried out by the authors under the auspices of the CODATA Task Group on Fundamental Constants [1,2]. The purpose of the adjustment is to determine best values of various fundamental constants such as the fine-structure constant, Rydberg constant, Avogadro constant, Planck constant, electron mass, muon mass, as well as many others, that provide the greatest consistency among the most critical experiments based on relationships derived from condensed matter theory and quantum electrodynamics (QED) theory. The 1998 CODATA recommended values of the constants also may be found on the Web at physics.nist.gov/constants. [Pg.145]

According to the third postulate the energy of activation may be set equal to hv (Planck s constant X frequency of light absorbed) in agreement with the quantum theory which has been so successful in many different fields. There is no support for this hypothesis, except the general success of the quantum theory (whenever applied to radiation phenomena, and chemical activation was assumed to be a radiation phenomenon. [Pg.32]

In parallel there exist some attempts trying to introduce a field theory (FT) starting from the standard description in terms of phase space [4—6], Of course, the best way to derive a FT for classical systems should consist in taking the classical limit of a QFT in the same way as the so called classical statistical mechanics is in fact the classical limit of a quantum approach. This limit is not so trivial and the Planck constant as well as the symmetry of wave functions survive in the classical domain (see for instance [7]). Here, we adopt a more pragmatic approach, assuming the existence of a FT we work in the spirit of QFT. [Pg.3]

Here, h = (6.626 068 76 0.000 000 52)-10 34 Js is the Planck constant, also known as Planck s action quantum v is the frequency of the photons. Quantum theory is required to calculate the spectral distribution of the energy emitted by a body. Other aspects of heat transfer can, in contrast, be covered by classical theory, according to which the radiation is described as the emission and propagation of electromagnetic waves. [Pg.504]

Planck s constant (b) A physical constant used to describe the sizes of quanta (any quantity that can only take on integer multiples of some base value). Named after Max Planck, it plays a central role in the theory of quantum mechanics, in which Planck is one of the founders of quantum theory. Its value is expressed as ... [Pg.214]


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See also in sourсe #XX -- [ Pg.99 ]




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