Template:Metals-metalloids-nonmetals: compare, details/sandbox
Appearance
Metals[1] | Metalloids | Nonmetals[1] | |
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Presentation and structure | |||
Colour |
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Reflectivity | |||
Form |
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Density |
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Deformability (as a solid) | |||
Poisson's ratio[n 5] |
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Crystalline structure at freezing point[40] | |||
Packing & coordination number |
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Atomic radius (calculated)[45] |
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Allotropes[46][n 9] |
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Electron-related | |||
Periodic table block |
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Outer s and p electrons |
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Electron bands: (valence, conduction) |
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Electron behaviour |
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Electrical conductivity |
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... as a liquid[63] |
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Thermodynamics | |||
Thermal conductivity |
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Temperature coefficient of resistance[n 15] | |||
Melting point |
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Melting behaviour |
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Enthalpy of fusion |
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Elemental chemistry | |||
Overall behaviour |
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Ion formation |
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Bonds |
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Oxidation number |
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Ionization energy |
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Electronegativity |
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Combined form chemistry | |||
With metals |
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With carbon |
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Hydrides |
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Oxides | |||
Sulfates |
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Halides, esp. chlorides (see also[118]) |
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Environmental chemistry | |||
Molar composition of Earth's ecosphere[n 23] |
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Primary form on Earth |
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Required by mammals | |||
Composition of the human body, by weight |
This is the template sandbox page for Template:Metals-metalloids-nonmetals: compare, details (diff). |
Footnotes
[edit]- ^ At standard pressure and temperature, for the elements in their most thermodynamically stable forms, unless otherwise noted
- ^ Copernicium is reported to be the only metal known to be a gas at room temperature.[13]
- ^ Whether polonium is ductile or brittle is unclear. It is predicted to be ductile based on its calculated elastic constants.[18] It has a simple cubic crystalline structure. Such a structure has few slip systems and "leads to very low ductility and hence low fracture resistance".[19]
- ^ Carbon as exfoliated (expanded) graphite,[21] and as metre-long carbon nanotube wire;[22] phosphorus as white phosphorus (soft as wax, pliable and can be cut with a knife, at room temperature);[23] sulfur as plastic sulfur;[24] and selenium as selenium wires.[25]
- ^ For polycrystalline forms of the elements unless otherwise noted. Determining Poisson's ratio accurately is a difficult proposition and there could be considerable uncertainty in some reported values.[26]
- ^ Beryllium has the lowest known value (0.0476) amongst elemental metals; indium and thallium each have the highest known value (0.46). Around one third show a value ≥ 0.33.[27]
- ^ Boron 0.13;[28] silicon 0.22;[29] germanium 0.278;[30] amorphous arsenic 0.27;[31] antimony 0.25;[32] tellurium ~0.2.[33]
- ^ Graphitic carbon 0.25;[34] [diamond 0.0718];[35] black phosphorus 0.30;[36] sulfur 0.287;[37] amorphous selenium 0.32;[38] amorphous iodine ~0.[39]
- ^ At atmospheric pressure, for elements with known structures
- ^ The Goldhammer-Herzfeld criterion is a ratio that compares the force holding an individual atom's valence electrons in place with the forces, acting on the same electrons, arising from interactions between the atoms in the solid or liquid element. When the interatomic forces are greater than or equal to the atomic force, valence electron itinerancy is indicated. Metallic behaviour is then predicted.[51] Otherwise nonmetallic behaviour is anticipated. The Goldhammer-Herzfeld criterion is based on classical arguments.[52] It nevertheless offers a relatively simple first order rationalization for the occurrence of metallic character amongst the elements.[53]
- ^ Metals have electrical conductivity values of from 6.9 × 103 S•cm−1 for manganese to 6.3 × 105 for silver.[56]
- ^ Metalloids have electrical conductivity values of from 1.5 × 10−6 S•cm−1 for boron to 3.9 × 104 for arsenic.[58] If selenium is included as a metalloid the applicable conductivity range would start from ~10−9 to 10−12 S•cm−1.[59][60][61]
- ^ Nonmetals have electrical conductivity values of from ~10−18 S•cm−1 for the elemental gases to 3 × 104 in graphite.[62]
- ^ Mott and Davis[64] note however that 'liquid europium has a negative temperature coefficient of resistance' i.e. that conductivity increases with rising temperature
- ^ At or near room temperature
- ^ Chedd[88] defines metalloids as having electronegativity values of 1.8 to 2.2 (Allred-Rochow scale). He included boron, silicon, germanium, arsenic, antimony, tellurium, polonium and astatine in this category. In reviewing Chedd's work, Adler[89] described this choice as arbitrary, given other elements have electronegativities in this range, including copper, silver, phosphorus, mercury and bismuth. He went on to suggest defining a metalloid simply as, 'a semiconductor or semimetal' and 'to have included the interesting materials bismuth and selenium in the book'.
- ^ Phosphorus is known to form a carbide in thin films.
- ^ See, for example, the sulfates of the transition metals,[98] the lanthanides[99] and the actinides.[100]
- ^ Sulfates of osmium have not been characterized with any great degree of certainty.[101]
- ^ Common metalloids: Boron is reported to be capable of forming an oxysulfate (BO)2SO4,[102] a bisulfate B(HSO4)3[103] and a sulfate B2(SO4)3.[104] The existence of a sulfate has been disputed.[105] In light of the existence of silicon phosphate, a silicon sulfate might also exist.[106] Germanium forms an unstable sulfate Ge(SO4)2 (d 200 °C).[107] Arsenic forms oxide sulfates As2O(SO4)2 (= As2O3.2SO3)[108] and As2(SO4)3 (= As2O3.3SO3).[109] Antimony forms a sulfate Sb2(SO4)3 and an oxysulfate (SbO)2SO4.[110] Tellurium forms an oxide sulfate Te2O3(SO)4.[111] Less common: Polonium forms a sulfate Po(SO4)2.[112] It has been suggested that the astatine cation forms a weak complex with sulfate ions in acidic solutions.[113]
- ^ Hydrogen forms hydrogen sulfate H2SO4. Carbon forms (a blue) graphite hydrogen sulfate C+
24HSO–
4 • 2.4H2SO4.[114] Nitrogen forms nitrosyl hydrogen sulfate (NO)HSO4 and nitronium (or nitryl) hydrogen sulfate (NO2)HSO4.[115] There are indications of a basic sulfate of selenium SeO2.SO3 or SeO(SO4).[116] Iodine forms a polymeric yellow sulfate (IO)2SO4.[117] - ^ layer-lattice types often reversibly so
- ^ Based on a table of the elemental composition of the biosphere, and lithosphere (crust, atmosphere, and seawater) in Georgievskii,[125] and the masses of the crust and hydrosphere give in Lide and Frederikse.[126] The mass of the biosphere is negligible, having a mass of about one billionth that of the lithosphere.[citation needed] "The oceans constitute about 98 percent of the hydrosphere, and thus the average composition of the hydrosphere is, for all practical purposes, that of seawater."[127]
- ^ Hydrogen gas is produced by some bacteria and algae and is a natural component of flatus. It can be found in the Earth's atmosphere at a concentration of 1 part per million by volume.
- ^ Fluorine can be found in its elemental form, as an occlusion in the mineral antozonite[129]
References
- ^ a b Kneen, Rogers & Simpson, 1972, p. 263. Columns 2 (metals) and 4 (nonmetals) are sourced from this reference unless otherwise indicated.
- ^ Russell & Lee 2005, p. 147
- ^ a b c Rochow 1966, p. 4
- ^ Pottenger & Bowes 1976, p. 138
- ^ Askeland, Fulay & Wright 2011, p. 806
- ^ Born & Wolf 1999, p. 746
- ^ Lagrenaudie 1953
- ^ Rochow 1966, pp. 23, 25
- ^ Burakowski & Wierzchoń 1999, p. 336
- ^ Olechna & Knox 1965, pp. A991‒92
- ^ Stoker 2010, p. 62
- ^ Chang 2002, p. 304. Chang speculates that the melting point of francium would be about 23 °C.
- ^ New Scientist 1975; Soverna 2004; Eichler, Aksenov & Belozeroz et al. 2007; Austen 2012
- ^ Hunt 2000, p. 256
- ^ Sisler 1973, p. 89
- ^ Hérold 2006, pp. 149–150
- ^ Russell & Lee 2005
- ^ Legit, Friák & Šob 2010, p. 214118-18
- ^ Manson & Halford 2006, pp. 378, 410
- ^ a b McQuarrie & Rock 1987, p. 85
- ^ Chung 1987; Godfrin & Lauter 1995
- ^ Cambridge Enterprise 2013
- ^ Faraday 1853, p. 42; Holderness & Berry 1979, p. 255
- ^ Partington 1944, p. 405
- ^ Regnault 1853, p. 208
- ^ Christensen 2012, p. 14
- ^ Gschneidner 1964, pp. 292‒93.
- ^ Qin et al. 2012, p. 258
- ^ Hopcroft, Nix & Kenny 2010, p. 236
- ^ Greaves et al. 2011, p. 826
- ^ Brassington et al. 1980
- ^ Martienssen & Warlimont 2005, p. 100
- ^ Witczak 2000, p. 823
- ^ Marlowe 1970, p. 6;Slyh 1955, p. 146
- ^ Klein & Cardinale 1992, pp. 184‒85
- ^ Appalakondaiah et al. 2012, pp. 035105‒6
- ^ Sundara Rao 1950; Sundara Rao 1954; Ravindran 1998, pp. 4897‒98
- ^ Lindegaard & Dahle 1966, p. 264
- ^ Leith 1966, pp. 38‒39
- ^ Donohoe 1982; Russell & Lee 2005
- ^ Gupta et al. 2005, p. 502
- ^ Walker, Newman & Enache 2013, p. 25
- ^ Wiberg 2001, p. 143
- ^ Batsanov & Batsanov 2012, p. 275
- ^ Clementi & Raimondi 1963; Clementi, Raimondi & Reinhardt 1967
- ^ Addison 1964; Donohoe 1982
- ^ Vernon 2013, p. 1704
- ^ Parish 1977, pp. 34, 48, 112, 142, 156, 178
- ^ a b Emsley 2001, p. 12
- ^ Russell 1981, p. 628
- ^ Herzfeld 1927; Edwards 2000, pp. 100–103
- ^ Edwards 1999, p. 416
- ^ Edwards & Sienko 1983, p. 695
- ^ a b Edwards & Sienko 1983, p. 691
- ^ Edwards et al. 2010
- ^ Desai, James & Ho 1984, p. 1160; Matula 1979, p. 1260
- ^ Choppin & Johnsen 1972, p. 351
- ^ Schaefer 1968, p. 76; Carapella 1968, p. 30
- ^ Glazov, Chizhevskaya & Glagoleva 1969 p. 86
- ^ Kozyrev 1959, p. 104
- ^ Chizhikov & Shchastlivyi 1968, p. 25
- ^ Bogoroditskii & Pasynkov 1967, p. 77; Jenkins & Kawamura 1976, p. 88
- ^ Rao & Ganguly 1986
- ^ Mott & Davis 2012, p. 177
- ^ Anita 1998
- ^ Cverna 2002, p.1
- ^ Cordes & Scaheffer 1973, p. 79
- ^ Hill & Holman 2000, p. 42
- ^ Tilley 2004, p. 487
- ^ Russell & Lee 2005, p. 466
- ^ Orton 2004, pp. 11–12
- ^ Zhigal'skii & Jones 2003, p. 66: 'Bismuth, antimony, arsenic and graphite are considered to be semimetals ... In bulk semimetals ... the resistivity will increase with temperature ... to give a positive temperature coefficient of resistivity ...'
- ^ Jauncey 1948, p. 500: 'Nonmetals mostly have negative temperature coefficients. For instance, carbon ... [has a] resistance [that] decreases with a rise in temperature. However, recent experiments on very pure graphite, which is a form of carbon, have shown that pure carbon in this form behaves similarly to metals in regard to its resistance.'
- ^ Reynolds 1969, pp. 91–92
- ^ a b Wilson 1966, p. 260
- ^ Wittenberg 1972, p. 4526
- ^ Habashi 2003, p. 73
- ^ Bailar et al. 1989, p. 742
- ^ Cox 2004, p. 27
- ^ Hiller & Herber 1960, inside front cover; p. 225
- ^ Beveridge et al. 1997, p. 185
- ^ a b Young & Sessine 2000, p. 849
- ^ Bailar et al. 1989, p. 417
- ^ Metcalfe, Williams & Castka 1966, p. 72
- ^ Chang 1994, p. 311
- ^ Pauling 1988, p. 183
- ^ Mann et al. 2000, p. 2783
- ^ Chedd 1969, pp. 24–25
- ^ Adler 1969, pp. 18–19
- ^ Hultgren 1966, p. 648
- ^ Bassett et al. 1966, p. 602
- ^ Rochow 1966, p. 34
- ^ Martienssen & Warlimont 2005, p. 257
- ^ Sidorov 1960
- ^ Brasted 1974, p. 814
- ^ Atkins 2006 et al., pp. 8, 122–23
- ^ Rao 2002, p. 22
- ^ Wickleder, Pley & Büchner 2006; Betke & Wickleder 2011
- ^ Cotton 1994, p. 3606
- ^ Keogh 2005, p. 16
- ^ Raub & Griffith 1980, p. 167
- ^ Nemodruk & Karalova 1969, p. 48
- ^ Sneed 1954, p. 472; Gillespie & Robinson 1959, p. 407
- ^ Zuckerman & Hagen 1991, p. 303
- ^ Sanderson 1967, p. 178
- ^ Iler 1979, p. 190
- ^ Sanderson 1960, p. 162; Greenwood & Earnshaw 2002, p. 387
- ^ Mercier & Douglade 1982
- ^ Douglade & Mercier 1982
- ^ Wiberg 2001, p. 764
- ^ Wickleder 2007, p. 350
- ^ Bagnall 1966, pp. 140−41
- ^ Berei & Vasáros 1985, pp. 221, 229
- ^ Wiberg 2001, p. 795
- ^ Lidin 1996, pp. 266, 270; Brescia et al. 1975, p. 453
- ^ Greenwood & Earnshaw 2002, p. 786
- ^ Furuseth et al. 1974
- ^ Holtzclaw, Robinson & Odom 1991, pp. 706–07; Keenan, Kleinfelter & Wood 1980, pp. 693–95
- ^ Kneen, Rogers & Simpson 1972, p. 278
- ^ Heslop & Robinson 1963, p. 417
- ^ Rochow 1966, pp. 28–29
- ^ Bagnall 1966, pp. 108, 120; Lidin 1996, passim
- ^ a b Smith 1921, p. 295; Sidgwick 1950, pp. 605, 608; Dunstan 1968, pp. 408, 438
- ^ Dunstan 1968, pp. 312, 408
- ^ Georgievskii 1982, p. 58
- ^ Lide & Frederikse 1998, p. 14–6
- ^ Hem 1985, p. 7
- ^ Perkins 1998, p. 350
- ^ Sanderson 2012