Journal of Research of the National Bureau of Standards, Volume 86U.S. Department of Commerce, National Bureau of Standards, 1981 |
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Page 33
... Energy levels and Lande g - factors for the configurations 3d4p + 3d - 14s4p + 3d - 24s24p in the first spectra of the iron group were calculated and compared with experimental values , in both general and individual treat- ments . The ...
... Energy levels and Lande g - factors for the configurations 3d4p + 3d - 14s4p + 3d - 24s24p in the first spectra of the iron group were calculated and compared with experimental values , in both general and individual treat- ments . The ...
Page 84
... energy expression is then Į U dx'dx'dx3 = Σ . Ex w1 U. ( mk ) ( 19 ) ( 20 ) c . Modifications for penalty methods The numerical integration scheme of ( 20 ) is adequate for a compressible energy density . For incompressi- ble or nearly ...
... energy expression is then Į U dx'dx'dx3 = Σ . Ex w1 U. ( mk ) ( 19 ) ( 20 ) c . Modifications for penalty methods The numerical integration scheme of ( 20 ) is adequate for a compressible energy density . For incompressi- ble or nearly ...
Page 86
... energy expression . Boundary conditions are also imposed on in the same manner as in linear analysis [ 22,23 ] . a . Separation of tensorial factors In what follows , let U , represent generically either a compressible element energy ...
... energy expression . Boundary conditions are also imposed on in the same manner as in linear analysis [ 22,23 ] . a . Separation of tensorial factors In what follows , let U , represent generically either a compressible element energy ...
Page 92
... energy expressions of section 2.2 . Any explicit occurrence of x3 is replaced by x3 = 0 , since we assume negligible variation of all quantities through the thickness . The x3 - integral in the multiple integrals of the energy ...
... energy expressions of section 2.2 . Any explicit occurrence of x3 is replaced by x3 = 0 , since we assume negligible variation of all quantities through the thickness . The x3 - integral in the multiple integrals of the energy ...
Page 96
... energy expressions and the finite element model are very similar to 3 - D linear elasticity , but e33 = 0 , and ... energy expressions . The point is that this can be done because the energy principle ( 6 ) which charac- terizes ...
... energy expressions and the finite element model are very similar to 3 - D linear elasticity , but e33 = 0 , and ... energy expressions . The point is that this can be done because the energy principle ( 6 ) which charac- terizes ...
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