S. Flügge – författare
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60 produkter
Electrical Conductivity I / Elektrische Leitungsphänomene I
Av S. Flügge
Inbunden, 1956
1098 kr
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191 Apart from numerous difficulties arising from the high pressure technique as such, there is a natural limitation to the possibility of applying a hydrostatic pressure, since liquids under pressure will solidify above a certain pressure limit. 8 2 Up to pressures of 3 X 10 kg.jm. at room …
Principles of Classical Mechanics and Field Theory / Prinzipien der Klassischen Mechanik und Feldtheorie
Av S. Flügge
Häftad, 1960
1024 kr
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Springer Tracts in Modern Physics
Av W. Kundt, Klaus Stierstadt m. fl.
E-bok, 2006
587 kr
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Encyclopedia of Physics / Handbuch der Physik
Mathematical Methods II / Mathematische Methoden II
Av S. Flugge
E-bok, 2013
587 kr
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Encyclopedia of Physics / Handbuch der Physik
Mathematical Methods II / Mathematische Methoden II
Av S. Flügge
Häftad, 2012
568 kr
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Kristallphysik I / Crystal Physics I
Av S. Flügge
Häftad, 2012
770 kr
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Ziff. 13. 41 Wir wollen das Problem folgendermaBen formulieren: Gegeben sei eine be- liebige physikalische Eigenschaft eines Kristalls beliebiger Symmetrie. Welche Bedingungen zwingt die Symmetrie des Korpers der betreffenden physikalischen Eigenschaft auf? Man braucht sich dabei keineswegs auf die …
Low Temperature Physics II / Kaltephysik II
Av S. Flugge
E-bok, 2012
718 kr
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71 For a given value of I the field is independent of the geometrical composition of the coil inside the winding space. The actual number of turns and the cross section of the conductors is entirely determined by the impedance of the power supply to which the magnet should be adapted. In the case …
Low Temperature Physics II / Kältephysik II
Av S. Flügge
Häftad, 2012
551 kr
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71 For a given value of I the field is independent of the geometrical composition of the coil inside the winding space. The actual number of turns and the cross section of the conductors is entirely determined by the impedance of the power supply to which the magnet should be adapted. In the case …
Electron-Emission Gas Discharges I / Elektronen-Emission Gasentladungen I
Av S. Flugge
E-bok, 2012
1427 kr
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v. Formation of negative ions by processes other than attachment in the gaseous phase at low X/po 17. Introduction. As early as 1912, J. J. THOMSON [32J in his first mass spectro graph observed negative ions of 0-, Cl-, H- and what he believed to be N-. He at first ascribed these to possible …
Electron-Emission Gas Discharges I / Elektronen-Emission Gasentladungen I
Av S. Flügge
Häftad, 2012
1098 kr
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v. Formation of negative ions by processes other than attachment in the gaseous phase at low X/po 17. Introduction. As early as 1912, J. J. THOMSON [32J in his first mass spectro graph observed negative ions of 0-, Cl-, H- and what he believed to be N-. He at first ascribed these to possible …
Spektroskopie II / Spectroscopy II
Av S. Flügge
Häftad, 2014
568 kr
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Sect. 23. 325 transitions have been drawn for which L1~=0 (n-components). Moreover it is assumed that the hfs splitting of the 3 s 2 Pal, level is negligibly small compared with that of the 3 s 25,/, level. BACK and GOUDSMIT succeeded in resolving the structure of the components of the Bi I line A …
Structure of Atomic Nuclei / Bau der Atomkerne
Av S. Flugge
E-bok, 2012
1459 kr
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243 number n and orbital angular momentum 1, but also a total angular momentum 1 f = 1 ± !. This modification lead to striking successes for the model. Almost without exception, the ground state spins of odd nuclei were found to be cor rectly predicted. Furthermore several other features of nuclei …
Structure of Atomic Nuclei / Bau der Atomkerne
Av S. Flügge
Häftad, 2014
1098 kr
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243 number n and orbital angular momentum 1, but also a total angular momentum 1 f = 1 ± !. This modification lead to striking successes for the model. Almost without exception, the ground state spins of odd nuclei were found to be cor rectly predicted. Furthermore several other features of nuclei …
Elasticity and Plasticity / Elastizitat und Plastizitat
Av S. Flugge
E-bok, 2012
1459 kr
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Elasticity and Plasticity / Elastizität und Plastizität
Av S. Flügge
Häftad, 2012
1098 kr
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External Properties of Atomic Nuclei / Äussere Eigenschaften der Atomkerne
Av S. Flugge
E-bok, 2013
570 kr
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External Properties of Atomic Nuclei / Äussere Eigenschaften der Atomkerne
Av S. Flügge
Häftad, 2012
568 kr
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39 2 2 Here B = hJ8:!t Ib and A = hJ8:!t Ia where Ia and Ib are the moments of inertia parallel and perpendicular respectively to the symmetry axis. ~ V I(J + 1) is 2n the total angular momentum of the molecule and K ~ its projection on the 2n symmetry axis. If the molecule possesses a permanent …
Astrophysik I: Sternoberflächen-Doppelsterne / Astrophysics I: Stellar-Surfaces-Binaries
Av S. Flugge
E-bok, 2013
717 kr
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Astrophysik I: Sternoberflächen-Doppelsterne / Astrophysics I: Stellar-Surfaces-Binaries
Av S. Flügge
Häftad, 2012
770 kr
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Sect. 13. 203 and the geometric elements for the large orbit are re-computed. From the analysis it cannot be decided whether the third body is close to the visual primary or secondary component; this can only be decided by measuring the orbital motion on an astrometric background of other stars …
Prinzipien der Thermodynamik und Statistik / Principles of Thermodynamics and Statistics
Av S. Flugge
E-bok, 2013
893 kr
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Prinzipien der Thermodynamik und Statistik / Principles of Thermodynamics and Statistics
Av S. Flügge
Häftad, 2013
871 kr
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177 Die statistische Mechanik ist ursprunglich von BOLTZMANN und GIBBS auf der Grundlage der Hamiltonschen Mechanik entwickelt worden. Da wir jedoch den Ausgangspunkt als ein Problem der Atom-Mechanik formullert haben, muB eine streng logische Darstellung des Gebietes notwendig an die …
Atoms III - Molecules I / Atome III - Molekule I
Av S. Flugge
E-bok, 2012
1427 kr
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dissociation, E, of a dimer into two monomers and that, E'', of a trimer into a dimer and a monomer. The observed velocity distribution for a beam of sodium iodide is shown in Fig. 23. The monomer and dimer distributions, which are each of the form of Eq. (9. 2), are separately shown. The sum of …
Atoms III — Molecules I / Atome III — Moleküle I
Av S. Flügge
Häftad, 2013
1098 kr
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dissociation, E, of a dimer into two monomers and that, E', of a trimer into a dimer and a monomer. The observed velocity distribution for a beam of sodium iodide is shown in Fig. 23. The monomer and dimer distributions, which are each of the form of Eq. (9. 2), are separately shown. The sum of the …
