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Atomic birimler (Atomic units) (au veya a.u.) form a system of natural units which is especially convenient for atomic physics calculations. There are two different kinds of atomic units, Hartree atomic units and Rydberg atomic units, which differ in the choice of the unit of mass and charge. This article deals with Hartree atomic units. In atomic units, the numerical values of the following four fundamental physical constants are all unity by definition:
- 1 Kullanım ve notasyon
- 2 Temel atomik birimler
- 3 İlgili fiziki sabitler
- 4 Derived atomic units
- 5 SI and Gaussian-CGS variants, and magnetism-related units
- 6 Atomik birimde Bohr modeli
- 7 Non-relativistic quantum mechanics in atomic units
- 8 Comparison with Planck units
- 9 See also
- 10 References
- 11 External links
Kullanım ve notasyon[değiştir | kaynağı değiştir]
Atomic units, like SI units, have a unit of mass, a unit of length, and so on. However, the use and notation is somewhat different from SI.
Suppose a particle with a mass of m has 3.4 times the mass of electron. The value of m can be written in three ways:
- "". This is the clearest notation (but least common), where the atomic unit is included explicitly as a symbol.
- "" ("a.u." means "expressed in atomic units"). This notation is ambiguous: Here, it means that the mass m is 3.4 times the atomic unit of mass. But if a length L were 3.4 times the atomic unit of length, the equation would look the same, "" The dimension needs to be inferred from context.
- "". This notation is similar to the previous one, and has the same dimensional ambiguity. It comes from formally setting the atomic units to 1, in this case , so .
Temel atomik birimler[değiştir | kaynağı değiştir]
These four fundamental constants form the basis of the atomic units (see above). Therefore, their numerical values in the atomic units are unity by definition.
|Dimension||Name||Symbol/Definition||Value in SI units|
|mass||electron rest mass||9.10938291(40)×10−31 kg|
|charge||elementary charge||1.602176565(35)×10−19 C|
|angular momentum||reduced Planck's constant||1.054571726(47)×10−34 J·s|
|electric constant||Coulomb force constant||8.9875517873681×109 kg·m3·s-2·C-2|
İlgili fiziki sabitler[değiştir | kaynağı değiştir]
Dimensionless physical constants retain their values in any system of units. Of particular importance is the fine-structure constant . This immediately gives the value of the speed of light, expressed in atomic units.
|Name||Symbol/Definition||Value in atomic units|
|speed of light|
|classical electron radius|
Derived atomic units[değiştir | kaynağı değiştir]
Below are given a few derived units. Some of them have proper names and symbols assigned, as indicated in the table. kB is Boltzmann constant.
|Dimension||Name||Symbol||Expression||Value in SI units||Value in more common units|
|length||Bohr radius||5.2917720859(36)×10−11 m||0.052918 nm=0.52918 Å|
|energy||Hartree energy||4.35974417(75)×10−18 J||27.211 eV=627.509 kcal·mol−1|
|force||8.2387225(14)×10−8 N||82.387 nN=51.421 eV·Å−1|
|electric field||5.14220652(11)×1011 V·m−1||5.14220652(11) GV·cm−1=51.4220652(11) V·Å−1|
|electric dipole moment||8.47835326(19)×10−30 C·m||2.541746 D|
There are two common variants of atomic units, one where they are used in conjunction with SI units for electromagnetism, and one where they are used with Gaussian-CGS units. Although the units written above are the same either way (including the unit for electric field), the units related to magnetism are not. In the SI system, the atomic unit for magnetic field is
and in the Gaussian-cgs unit system, the atomic unit for magnetic field is
(These differ by a factor of α.)
and in Gaussian-based atomic units,
Atomik birimde Bohr modeli[değiştir | kaynağı değiştir]
Atomic units are chosen to reflect the properties of electrons in atoms. This is particularly clear from the classical Bohr model of the hydrogen atom in its ground state. The ground state electron orbiting the hydrogen nucleus has (in the classical Bohr model):
- Orbital velocity = 1
- Orbital radius = 1
- Angular momentum = 1
- Orbital period = 2π
- Ionization energy = 1⁄2
- Electric field (due to nucleus) = 1
- Electrical attractive force (due to nucleus) = 1
Non-relativistic quantum mechanics in atomic units[değiştir | kaynağı değiştir]
The Schrödinger equation for an electron in SI units is
The same equation in au is
For the special case of the electron around a hydrogen atom, the Hamiltonian in SI units is:
while atomic units transform the preceding equation into
Comparison with Planck units[değiştir | kaynağı değiştir]
Both Planck units and au are derived from certain fundamental properties of the physical world, and are free of anthropocentric considerations. It should be kept in mind that au were designed for atomic-scale calculations in the present-day universe, while Planck units are more suitable for quantum gravity and early-universe cosmology. Both au and Planck units normalize the reduced Planck constant. Beyond this, Planck units normalize to 1 the two fundamental constants of general relativity and cosmology: the gravitational constant G and the speed of light in a vacuum, c. Atomic units, by contrast, normalize to 1 the mass and charge of the electron, and, as a result, the speed of light in atomic units is a large value, . The orbital velocity of an electron around a small atom is of the order of 1 in atomic units, so the discrepancy between the velocity units in the two systems reflects the fact that electrons orbit small atoms much slower than the speed of light (around 2 orders of magnitude slower).
There are much larger discrepancies in some other units. For example, the unit of mass in atomic units is the mass of an electron, while the unit of mass in Planck units is the Planck mass, a mass so large that if a single particle had that much mass it might collapse into a black hole. Indeed, the Planck unit of mass is 22 orders of magnitude larger than the au unit of mass. Similarly, there are many orders of magnitude separating the Planck units of energy and length from the corresponding atomic units.
See also[değiştir | kaynağı değiştir]
References[değiştir | kaynağı değiştir]
- ^ Hartree, D. R. (1928). "The Wave Mechanics of an Atom with a Non-Coulomb Central Field. Part I. Theory and Methods". Mathematical Proceedings of the Cambridge Philosophical Society (Cambridge University Press) 24 (1): ss. 89–110. doi:10.1017/S0305004100011919. http://journals.cambridge.org/action/displayAbstract?aid=1733252.
- ^ a b Pilar, Frank L. (2001). Elementary Quantum Chemistry. Dover Publications. ss. 155. ISBN 978-0-486-41464-5. http://books.google.com/books?id=XpGM7r69LdkC&pg=PA155.
- ^ Bishop, David M. (1993). Group Theory and Chemistry. Dover Publications. ss. 217. ISBN 978-0-486-67355-4. http://books.google.com/books?id=l4zv4dukBT0C&pg=PA217.
- ^ Drake, Gordon W. F. (2006). Springer Handbook of Atomic, Molecular, and Optical Physics (2nd bas.). Springer. ss. 5. ISBN 978-0-387-20802-2. http://books.google.com/books?id=Jj-ad_2aNOAC&pg=PA5.
- ^ Şablon:Cite article
- ^ "A note on Units". Physics 7550 — Atomic and Molecular Spectra. University of Colorado lecture notes. http://www.colorado.edu/physics/phys7550/phys7550_sp07/extras/Appendix_1.pdf.
- ^ Chis, Vasile. "Atomic Units; Molecular Hamiltonian; Born-Oppenheimer Approximation". Molecular Structure and Properties Calculations. Babes-Bolyai University lecture notes. http://phys.ubbcluj.ro/~vchis/cursuri/cspm/course2.pdf. )
- ^ Budker, Dmitry; Kimball, Derek F.; DeMille, David P. (2004). Atomic Physics: An Exploration through Problems and Solutions. Oxford University Press. ss. 380. ISBN 978-0-19-850950-9. http://books.google.com/books?id=GW6pclAk-JcC&pg=PA380.
- Shull, H.; Hall, G. G. (1959). "Atomic Units". Nature 184 (4698): 1559. Bibcode 1959Natur.184.1559S. doi:10.1038/1841559a0.