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Additional info for BS EN 1015-2:1999: Methods of test for mortar for masonry. Bulk sampling of mortars and preparation of test mortars

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84. Fe3–xCoxSi. Dependence of magnetocrystalline anisotropy constant K, extrapolated to 0 K on Co concentration [86K1]. 4 Fig. 83. Fe3–xCoxSi. Dependence of the halfwidth Γ of the outermost lines of the Mössbauer spectra, at room temperature, on Co concentration [86K1]. 50 [Ref. p. 4 20 T [K] 40 120 180 240 300 360 60 120 180 240 300 360 0 b Temperature T [K] Temperature T [K] Fig. 86. Fe1–xMnxSi (a) and Fe1–xCoxSi (b). Temperature dependence of the linear thermal expansion coefficient α [89P1].

Fig. 54. Mn1–xCoxGe4 high-temperature synthesized. 0 Susceptibility cg [10 cm g ] Magnetization σ [G cm g ] Mn1-x Cox Ge4 Fig. 55. Mn3Sn. Temperature dependence of the spontaneous mass magnetization σs and the magnetic mass susceptibility χg [87O2]. (a) For magnetic field parallel to the a axis. (b) For magnetic field parallel to the c axis. 6Sn and was annealed at 850 °C for 50 h and cooled down to room temperature at 10 K/h. Landolt-Börnstein New Series III/32C Ref. p. 4 3d elements and C, Si, Ge, Sn or Pb Mn3 Sn A 33 A C B C B B C B C A y A A A C B B C C B A B C A x Mn a Fig.

The Fe magnetic moments at z = 1/4 and 3/4 are parallel to each other and stay in the c plane. (a) Collinear structure between TN = 378 K and Ttr = 93 K. The Fe moments, which are oriented along <100> (± [010] are chosen in the figure) at TN (β = 45°), rotate continuously by 19° (β =26°) with decreasing temperature. (b) Noncollinear structure below Ttr. Hyperfine-field directions at Sn (at z = 0 and at z = 1/2) are also shown. Magnetic unit cell becomes twice as large as chemical cell: amag = 2 a .

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BS EN 1015-2:1999: Methods of test for mortar for masonry. Bulk sampling of mortars and preparation of test mortars


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