tabel 50 elemente tfab

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  • 7/30/2019 Tabel 50 Elemente TFAB

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    1R. D. Rugescu, 2011 Materiale pentru sisteme de propulsie aerospaial

    NrElementul chimic

    To

    pire[C]

    Densitate [g/cmc] Masa molar [g-mol]

    raza atomic

    Emp,Calc[][4]

    Modul Young

    [GPa]

    Rupere, r[Pa] 107 lungire r%Cond.ter

    mic[W/m/K

    ]

    MyOx

    Hf0

    Entalpieformare[kJ/mol]

    de adaugatoxizii

    Anul

    descopeririii

    cercettorul

    1Galiu Ga 5.91 69.723 1.870 - - 29 276.9808(g)

    0 (s)

    1875

    2Sodiu Na 0.97 22.98976928

    1.100 10 - 140 107.738 (g)2.4058 (l)

    0 (s)

    1807

    3Litiu Li 0.534 6.941 1.820 4.9 - 85 160.6656(g)

    2.380696 (l)0 (s)

    1817

    4Staniu Sn 7.287 118.710 2.170 50 0.36 66.6 302.0848(g)

    -2.092 (sgri)

    0 (s alb)

    3500.Hr.

    5Bismut Bi 9.807 208.98040 2.070 32 0.33 7.87 207.108 (g)0 (s)

    1753

    6Taliu Tl 11.8 204.3833 1.960 8 0.45 46.1 182.2132(g)0 (s)

    1861

    7Cadmiu Cd 8.69 112.411 2.180 50 0.30 96.8 112.00568(g)

    -0.58576 (salpha)

    0 (s gamma)

    1817

    8Plumb Pb 11.342 207.2 2.020 16 1213*10e5 0.44 35.3 195.602 (g)4.2886 (l)

    0 (s)

    3000.Hr.

    9Zinc Zn 7.134 65.38 2.010 108 0.25 116 130.72908(g)

    0 (s)

    1746

    10Telur Te 6.232 127.60 2.060 43 - 2.35 196.73168(g)

    0 (s)

    1782

    11MagneziuMg 1.74 24.3050 1.730 45 0.29 156 147.61152(g)

    9.03744 (l)0 (s)

    1808

    12Aluminiu Al 2.70 26.9815386

    1.840 70 0.35 237 326.352 (g)8.66088 (l)

    0 (s)

    1808

    13Bariu Ba 3.62 137.327 2.680 13 - 18.4 179.0752

    (g)4.97896 (l)0 (s)

    1808

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    2R. D. Rugescu, 2011 Materiale pentru sisteme de propulsie aerospaial

    14Ytterbiu Yb 6.90 173.054 2.260 24 0.21 34.9 152.2976(g)

    0 (s)

    1878

    15GermaniuGe 5.323 72.64 2.110 - - 59.9 376.56 (g)0 (s)1871DmitriMendeleyev

    16Argint 47 Ag 10.501 107.8682 2.110 83 0.37 429 1192.0216(g)

    284.55384(g)

    0 (s)

    antichitate

    17Aur Au 19.282 196.966569

    2.140 78 0.44 317 366.1 (g)0 (s) antichitate

    18Cupru Cu 8.933 63.546 1.960 130 0.34 401 338.31824(g)

    0 (s)

    antichitate

    19Mangan Mn 7.3 54.938045 2.050 198 - 7.82 280.7464(g)

    1.54808 (sgamma)

    0 (s alpha)

    CarlWilhelmScheele

    177420Beriliu Be 1.85 9.012182 1.530 287 0.032 200 324.26 (g)

    12.04992 (l)0 (s)

    AbbHay,1798

    21GadoliniuGd 7.9 157.25 2.340 55 0.26 10.6 397.48 (g)0 (s)

    1880,Jean deMarignac

    22Terbiu Tb 8.23 158.92535 2.330 56 0.26 11.1 388.6936(g)

    0 (s)

    1843,CarlMosander

    23[Siliciu] Si 2.3296 28.0855 2.100 47 - 148 455.6376(g)

    0 (s)

    1824,

    JnsJacobBerzelius

    24Nichel Ni 8.912 58.6934 1.970 200 0.31 90.7 429.6968(g)

    0 (s)

    1751,

    AxelFredrikCrons

    tedt25Cobalt Co 8.86 58.933195 2.000 209 0.31 100 -110.54128

    (g)1739,

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    3R. D. Rugescu, 2011 Materiale pentru sisteme de propulsie aerospaial

    0.46024(structur

    cubicsolida)

    0 (structursolid

    hexagonal)

    GeorgBrandt

    26Ytriu Y 4.47 88.90585 2.320 64 0.24 17.2 421.3288(g)

    0 (s)

    1789,

    JohanGadolin

    27Erbiu Er

    28Fier Fe

    29Scandiu Sc

    30Paladiu Pd

    31Thuliu Tm

    32Lutetiu Lu

    33Titan Ti

    34Thoriu Th

    35Platin Pt36Zirconiu Zr

    37Crom Cr

    38Vanadiu V

    39Rhodiu Rh

    40[Bor] B

    41Hafniu Hf

    42Rhuteniu Ru

    43Iridiu Ir

    44Niobiu Nb

    45Molibden Mo

    46Tantal Ta

    47Osmiu Os

    48Rheniu Re

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    4R. D. Rugescu, 2011 Materiale pentru sisteme de propulsie aerospaial

    49Wolfram W

    50[Carbon] C

    Se vor completa pentru fiecare element casetele lipsa, prin documentare, cu mentionarea sursei bibliografice folosite. Exemplu maijos.

    Exemple de citare bibliografic:

    Litiul a fost descoperit n mineralul petalit (LiAl(Si2O5)2) de Johann August Arfvedson n1817 [5].

    Borul a fost descoperit de Joseph-Louis Gay-Lussac i Louis-Jaques Thnard, chimitifrancezi, i independent de Sir Humphry Davy, un chimist englez, n 1808 [7].

    1.Pagini http:[1]http://education.jlab.org/itselemental/ele005.html[2] *** Periodensystem pocketcard, ISBN 3-929785-28-5, Brm Bruckmeier Verlag, 82031Grnwald, Germany,www.media4u.com, 2002.[3] Visual elements,www.rsc.org/periodic-table/element/4/beryllium [4]http://www.webelements.com[-]

    2.Cri:[5] A.M. Howatson, P.G. Lund, and J.D. Todd,Engineering Tables and Data, p. 41.[6] *** CRC Handbook of Chemistry and Physics, CRC Press, 92nd Edition, 2011.

    [7] Alfred Buch (1999),Pure metals properties: a scientific-technical handbook, ISBN 08717063779780871706379, OCLC Number 441824091, Materials Park, ASM International, London-Tel Aviv,Freund Pub. House, 306 p, 25 cm.[8] Dean, John A. Lange's Handbook of Chemistry, 12th ed.; McGraw-Hill Book Company: NewYork, NY, 1979; p 9:4-9:94.[9] Lide, David R. CRC Handbook of Chemistry and Physics, 84th ed.; CRC Press: Boca Raton, FL,2002.[10] Ibidem, 83rd ed, 2002.3.Reviste:[11] Jiemin Z, Lamvik M, 1998, "Thermal conductivity of gallium at solid/liquid phasetransformation"High Temperatures - High Pressures30(3), 307314:[Thermal conductivity of gallium at solid/liquid phase transformation, received 29 April 1997]Abstract. The thermal conductivity of pure gallium during liquid/solid phase transformation has

    been measured. The measurements establish that there is a one-dimensional motion of a freezing ormelting front in the specimen. The technique employed allows the study of alternative conditions:the propagation of the phase transition interface, as opposed to the quasi-equilibrium state where theinterface is stationary. The position of the interface is determined from the measurement of theelectric resistance over the specimen including the interface. The resistance over time obtainedduring the melting/freezing processes enables the speed of the solid-liquid interface to bedetermined. The thermal conductivity of the specimen at the interface is evaluated as a real-time

    property from the speed of the moving interface, temperature gradients normal to the interface, andthermal properties. The mean values of the thermal conductivity of gallium at the transitiontemperature, 29.772 C, were found to be l s = 43.6 W m-1 K-1 and ll = 27.8 W m-1 K-1 for the solidand the liquid phase, respectively. These values are 16% and 10% lower than a set of definedreference data based on electric measurements that are referred to in the literature.

    http://education.jlab.org/itselemental/ele005.htmlhttp://education.jlab.org/itselemental/ele005.htmlhttp://education.jlab.org/itselemental/ele005.htmlhttp://www.media4u.com/http://www.media4u.com/http://www.media4u.com/http://www.rsc.org/periodic-table/element/4/berylliumhttp://www.rsc.org/periodic-table/element/4/berylliumhttp://www.rsc.org/periodic-table/element/4/berylliumhttp://www.webelements.com/beryllium/physics.htmlhttp://www.webelements.com/beryllium/physics.htmlhttp://www.webelements.com/beryllium/physics.htmlhttp://www.webelements.com/beryllium/physics.htmlhttp://www.rsc.org/periodic-table/element/4/berylliumhttp://www.media4u.com/http://education.jlab.org/itselemental/ele005.html
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    5R. D. Rugescu, 2011 Materiale pentru sisteme de propulsie aerospaial

    http://www.mrteverett.com/Chemistry/pdictable/q_elements.asp?language=en&Symbol=TeAdd to languages: 120110Rumanian: Telur

    http://www.mrteverett.com/Chemistry/pdictable/q_elements.asp?language=en&Symbol=Tehttp://www.mrteverett.com/Chemistry/pdictable/q_elements.asp?language=en&Symbol=Tehttp://www.mrteverett.com/Chemistry/pdictable/q_elements.asp?language=en&Symbol=Te
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    6R. D. Rugescu, 2011 Materiale pentru sisteme de propulsie aerospaial

    [Tellurium element was discovered in Romania, sylvanite (AgAuTe4)is its most spread ore, bearingthe name from Transylvania, and 23 million Romanians may read this text]

    Add to languages:Romanian: Zinc[An alloy containing 87% zinc has been found in prehistoric ruins in Transylvania (Romania); 23mill. Romanians may read Everett page]