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Pb 82

Lead (Pb)

post-transition-metal
Période: 6 Groupe: 14 Bloc: p

Solid

Masse atomique relative standard

207,2 u [206,14, 207,94]

Configuration électronique

[Xe] 6s2 4f14 5d10 6p2

Point de fusion

327,46 °C

Point d’ébullition

1748,85 °C

Masse volumique

1,1342e+4 kg/m³

États d’oxydation

−4, −2, −1, 0, +1, +2, +3, +4

Électronégativité (Pauling)

2,33

Énergie d’ionisation (1re)

7,41668 eV

Année de découverte

2021

Rayon atomique

180 pm

Détails

Origine du nom Anglo-Saxon: lead; symbol from Latin: plumbum.
Découvreurs Known to the ancients.

Lead is a dense, soft post-transition metal with atomic number 82. It is chemically characterized by the +2 oxidation state, with +4 less stable except in selected compounds, a pattern influenced by the inert-pair effect. Lead has been used since antiquity because it is easily smelted and worked, but its toxicity now strongly limits dispersive uses. It remains important where high density, corrosion resistance, low melting point, and radiation attenuation are valuable.

Lead is a bluish-white metal of bright luster. It is very soft, highly malleable, ductile, and a poor conductor of electricity. It is very resistant to corrosion; lead pipes bearing the insignia of Roman emperors, used as drains from the baths, are still in service. It is used in containers for corrosive liquids (such as sulfuric acid) and may be toughened by the addition of a small percentage of antimony or other metals.

The name derives from the Anglo-Saxon lead, which is of unknown origin. The element was known from prehistoric times. The chemical symbol Pb is derived from the Latin plumbum.

<!-- --> <p class="caption">For more information about the natural variations of the atomic weight of lead please read IUPAC Technical Report Variation of lead isotopic composition and atomic weight in terrestrial materials (IUPAC Technical Report) <img src="images/pdf.gif" style="width:auto; margin:0; vertical-align:bottom;"> by Z.-K. Zhu et al Pure Appl. Chem. <strong>93</strong>, 155-166 (2021).

Lead has been known since ancient times. It is sometimes found free in nature, but is usually obtained from the ores galena (PbS), anglesite (PbSO4), cerussite (PbCO3) and minum (Pb3O4). Although lead makes up only about 0.0013% of the earth's crust, it is not considered to be a rare element since it is easily mined and refined. Most lead is obtained by roasting galena in hot air, although nearly one third of the lead used in the United States is obtained through recycling efforts.

Long known, mentioned in Exodus. The alchemists believed lead to be the oldest metal and associated with the planet Saturn. Native lead occurs in nature, but is rare.

Images

Propriétés

Propriétés chimiques

Électronégativité (Pauling)
2,33 Comparer : Électronégativité (Pauling) de tous les éléments →
Électronégativité (Allen)
1,854
Affinité électronique
0,364 eV
Énergie d’ionisation (1re)
7,41668 eV Comparer : Énergie d’ionisation (1re) de tous les éléments →
Énergie d’ionisation (2e)
15,032551 eV Comparer : Énergie d’ionisation (2e) de tous les éléments →
Énergie d’ionisation (3e)
31,93741 eV Comparer : Énergie d’ionisation (3e) de tous les éléments →
Énergie d’ionisation (4e)
42,332706 eV Comparer : Énergie d’ionisation (4e) de tous les éléments →
Énergie d’ionisation (5e)
68,800237 eV Comparer : Énergie d’ionisation (5e) de tous les éléments →
États d’oxydation
−4, −2, −1, 0, +1, +2, +3, +4 Comparer : États d’oxydation de tous les éléments →
Électrons de valence
4 Comparer : Électrons de valence de tous les éléments →
Configuration électronique
[Xe] 6s2 4f14 5d10 6p2

Propriétés thermodynamiques

Enthalpie de fusion
0,04943774 eV Comparer : Enthalpie de fusion de tous les éléments →
Enthalpie de vaporisation
1,860393 eV Comparer : Enthalpie de vaporisation de tous les éléments →
Enthalpie de sublimation
2,023112 eV
Enthalpie d’atomisation
2,023112 eV
Enthalpie d’atomisation
2,023112 eV

Propriétés nucléaires

Protons
82 Comparer : Protons de tous les éléments →
Neutrons
126 Comparer : Neutrons de tous les éléments →
Isotopes connus
43 Comparer : Isotopes connus de tous les éléments →
Isotopes stables
0 Comparer : Isotopes stables de tous les éléments →
Isotope le plus stable
Pb-208
Année de découverte
2021

Abondance

Abondance (croûte terrestre)
14 mg/kg Comparer : Abondance (croûte terrestre) de tous les éléments →
Abondance (océan)
3 × 10−5 mg/L Comparer : Abondance (océan) de tous les éléments →

Structure cristalline

Paramètre de maille a
495 pm

Structure électronique

Électrons par couche
2, 8, 18, 32, 18, 4 Comparer : Électrons par couche de tous les éléments →

Identifiants

Numéro CAS
7439-92-1 Comparer : Numéro CAS de tous les éléments →
Symbole de terme
(1/2,1/2)0
InChI
InChI=1S/Pb
Clé InChI
WABPQHHGFIMREM-UHFFFAOYSA-N

Configuration électronique Mesuré

Charge ionique
Protons 82
Électrons 82
Charge Neutre
Configuration Pb: 4f¹⁴ 5d¹⁰ 6s² 6p²
Configuration électronique
Mesuré
[Xe] 4f¹⁴ 5d¹⁰ 6s² 6p²
1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p²
Diagramme d’orbitales
1s
2/2
2s
2/2
2p
6/6
3s
2/2
3p
6/6
4s
2/2
3d
10/10
4p
6/6
5s
2/2
4d
10/10
5p
6/6
6s
2/2
4f
14/14
5d
10/10
6p
2/6 2↑
Nombre total d’électrons: 82 Non appariés: 2 ?

Modèle atomique

Protons 82
Neutrons 102
Électrons 82
Nombre de masse 184
Stabilité Radioactif

Les isotopes diffèrent par leur nombre de neutrons, leur masse et leur stabilité — pas par la configuration électronique de l’atome neutre.

Modèle atomique schématique, non à l’échelle.

Empreinte atomique

Spectre d’émission / d’absorption

25 / 26 (26 26 avec intensité)
Mesuré
Émission Visible : 380–750 nm

Distribution isotopique

Aucun isotope stable.

Nombre de masseMasse atomique (u)Abondance naturelleDemi-vie
183 Radioactif182,991872 ± 0,00003N/D535 ms
184 Radioactif183,988136 ± 0,000014N/D490 ms
178 Radioactif178,003831 ± 0,000026N/D250 us
215 Radioactif215,00474 ± 0,00011N/D142 secondes
204 Radioactif203,973044 ± 0,00000131,4000%140 Py
Mesuré

Phase / État

1 atm / 101,325 kPa
Solide 25 °C (298,15 K)

Explication: 302,5 °C en dessous du point de fusion (327,46 °C)

Point de fusion 327,46 °C
Point d’ébullition 1748,85 °C
Écart en dessous du point de fusion 302,5 °C
0 K Température actuelle: 25 °C 6000 K
Échelle des phases

Schématique, non à l’échelle

Solide
Liquide
Gaz
Fusion
Ébullition
25°C
Solide
Liquide
Gaz
Actuel

Points de transition de phase

Point de fusion Littérature scientifique
327,46 °C
Point d’ébullition Littérature scientifique
1748,85 °C
Phase actuelle Calculé
Solide

Énergies de transition

Enthalpie de fusion Littérature scientifique
0,04943774 eV

Énergie nécessaire pour faire fondre 1 mol au point de fusion

Enthalpie de vaporisation Littérature scientifique
1,860393 eV

Énergie nécessaire pour vaporiser 1 mol au point d’ébullition

Enthalpie de sublimation Littérature scientifique
2,023112 eV

Énergie nécessaire pour sublimer 1 mol au point de sublimation

Masse volumique

Masse volumique de référence Littérature scientifique
1,1342e+4 kg/m³

Dans les conditions standard

Masse volumique actuelle Calculé
1,1342e+4 kg/m³

Dans les conditions standard

Spectres atomiques

Affichage de 10 sur 82. Tri par charge ionique croissante.

Raies répertoriées ?

IonChargeNombre total de raiesProbabilités de transitionDésignations des niveaux
Pb I 013528135
Pb II +197312
Pb III +24100
Pb IV +39200
Pb V +49000
Raies répertoriées par le NIST →

Niveaux répertoriés ?

IonChargeNiveaux
Pb I 0136
Pb II +195
Pb III +2124
Pb IV +3108
Pb V +445
Pb VI +52
Pb VII +62
Pb VIII +72
Pb IX +82
Pb X +92
Niveaux répertoriés par le NIST →
82 Pb 207.2

Lead — Visualiseur d’orbitales atomiques

[Xe]6s24f145d106p2
Niveaux d’énergie 2 8 18 32 18 4
États d’oxydation -4, -2, -1, 0, +1, +2, +3, +4
HOMO 6p n=6 · l=1 · m=-1
Lead — Aperçu du visualiseur d’orbitales atomiques
Three.js se charge uniquement à la demande
82 Pb 207.2

Lead — Visualiseur de structure cristalline

Face-Centered Cubic · Pearson cF4
Expérimental
Pearson cF4
N° de coord. 12
Compacité 74.000%
Lead — Aperçu du visualiseur de structure cristalline
Three.js se charge uniquement à la demande

Rayons ioniques

Affichage de 10 sur 12.

ChargeCoordinenceSpinRayon
+24N/D98 pm
+26N/D119 pm
+27N/D123 pm
+28N/D129 pm
+29N/D135 pm
+210N/D140 pm
+211N/D145 pm
+212N/D149 pm
+44N/D65 pm
+45N/D73 pm

Composés

Pb
207,000 u
Pb+2
207,000 u
Pb
209,984 u
Pb
214,000 u
Pb
211,992 u
Pb
205,974 u
Pb
206,976 u
Pb
207,977 u
Pb
203,973 u
Pb
202,973 u
Pb
204,974 u
Pb
208,981 u
Pb
210,989 u
Pb
200,973 u
Pb
199,972 u
Pb
197,972 u
Pb
198,973 u
Pb
201,972 u
Pb
194,975 u
Pb
218,017 u
Pb+2
211,992 u
Pb
193,974 u
Pb
195,973 u
Pb
196,973 u
Pb
212,997 u

Isotopes (5)

Nombre de masseMasse atomique (u)Abondance naturelleDemi-vieMode de désintégration
183 Radioactif182,991872 ± 0,00003N/D535 ms
α ≈100%β+ ?
184 Radioactif183,988136 ± 0,000014N/D490 ms
α =80±1.1%β+ ?
178 Radioactif178,003831 ± 0,000026N/D250 us
α ≈100%β+ ?
215 Radioactif215,00474 ± 0,00011N/D142 secondes
β- =100%
204 Radioactif203,973044 ± 0,00000131,4000% ± 0,1000%140 Py
IS =1.4±0.6%α ?
183 Radioactif
Masse atomique (u) 182,991872 ± 0,00003
Abondance naturelle N/D
Demi-vie 535 ms
Mode de désintégration
α ≈100%β+ ?
184 Radioactif
Masse atomique (u) 183,988136 ± 0,000014
Abondance naturelle N/D
Demi-vie 490 ms
Mode de désintégration
α =80±1.1%β+ ?
178 Radioactif
Masse atomique (u) 178,003831 ± 0,000026
Abondance naturelle N/D
Demi-vie 250 us
Mode de désintégration
α ≈100%β+ ?
215 Radioactif
Masse atomique (u) 215,00474 ± 0,00011
Abondance naturelle N/D
Demi-vie 142 secondes
Mode de désintégration
β- =100%
204 Radioactif
Masse atomique (u) 203,973044 ± 0,0000013
Abondance naturelle 1,4000% ± 0,1000%
Demi-vie 140 Py
Mode de désintégration
IS =1.4±0.6%α ?

Raies spectrales

Longueur d’onde (nm)IntensitéDegré d’ionisationTypeTransitionPrécisionSource
401.96322 nm15000Pb Iemission6s2.6p2 (3/2,3/2) → 6s2.6p.(2P*<1/2>).6d 2[5/2]*MesuréeNIST
405.780659 nm95000Pb Iemission6s2.6p2 (3/2,1/2) → 6s2.6p.7s (1/2,1/2)*MesuréeNIST
406.213593 nm14000Pb Iemission6s2.6p2 (3/2,3/2) → 6s2.6p.(2P*<1/2>).6d 2[3/2]*MesuréeNIST
415.78144 nm10Pb Iemission6s2.6p2 (3/2,3/2) → 6s2.6p.9s (1/2,1/2)*MesuréeNIST
416.80327 nm10000Pb Iemission6s2.6p2 (3/2,3/2) → 6s2.6p.(2P*<1/2>).6d 2[5/2]*MesuréeNIST
434.041263 nm200Pb Iemission6s2.6p2 (3/2,3/2) → 6s2.6p.(2P*<1/2>).7d 2[3/2]*MesuréeNIST
500.54165 nm1000Pb Iemission6s2.6p2 (3/2,3/2) → 6s2.6p.7s (3/2,1/2)*MesuréeNIST
500.65724 nm100Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.9p (1/2,3/2)MesuréeNIST
507.6322 nm10Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.9p (1/2,1/2)MesuréeNIST
508.94835 nm50Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.9p (1/2,3/2)MesuréeNIST
509.00083 nm20Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.9p (1/2,3/2)MesuréeNIST
510.72427 nm10Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.9p (1/2,1/2)MesuréeNIST
520.14372 nm2000Pb Iemission6s2.6p2 (3/2,3/2) → 6s2.6p.8s (1/2,1/2)*MesuréeNIST
569.23465 nm40Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.(2P*<1/2>).5f 2[5/2]MesuréeNIST
589.56245 nm200Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.8p (1/2,3/2)MesuréeNIST
600.18624 nm2000Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.8p (1/2,3/2)MesuréeNIST
601.16667 nm500Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.8p (1/2,3/2)MesuréeNIST
605.93556 nm500Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.8p (1/2,1/2)MesuréeNIST
611.05203 nm50Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.8p (1/2,1/2)MesuréeNIST
623.52656 nm100Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.8p (1/2,1/2)MesuréeNIST
689.2117 nm10Pb Iemission6s2.6p.7p (1/2,1/2) → 6s2.6p.(2P*<1/2>).10d 2[5/2]*MesuréeNIST
712.893 nm5Pb Iemission6s2.6p.7p (1/2,1/2) → 6s2.6p.11s (1/2,1/2)*MesuréeNIST
722.89658 nm20000Pb Iemission6s2.6p2 (3/2,3/2) → 6s2.6p.7s (1/2,1/2)*MesuréeNIST
730.46753 nm5Pb Iemission6s2.6p.7p (1/2,1/2) → 6s2.6p.(2P*<1/2>).9d 2[3/2]*MesuréeNIST
733.0146 nm8Pb Iemission6s2.6p2 (3/2,1/2) → 6s2.6p2 (3/2,3/2)MesuréeNIST
734.6676 nm10Pb Iemission6s2.6p.7p (1/2,1/2) → 6s2.6p.(2P*<1/2>).9d 2[5/2]*MesuréeNIST

Propriétés étendues

Rayons covalents (données étendues)

Rayon covalent (Pyykkö)
144 pm
Rayon covalent (Pyykkö, liaison double)
135 pm
Rayon covalent (Pyykkö, liaison triple)
137 pm

Rayons de van der Waals

Bondi
202 pm
Batsanov
230 pm
Alvarez
260 pm
UFF
429,7 pm
MM3
274 pm

Rayons atomiques et métalliques

Rayon atomique (Rahm)
249 pm
Rayon métallique (C12)
170 pm

Échelles de numérotation

Mendeleev
91
Pettifor
82
Glawe
82

Échelles d’électronégativité

Ghosh
0
Miedema
4
Gunnarsson–Lundqvist
4
Robles–Bartolotti
4

Polarisabilité et dispersion

Polarisabilité dipolaire
47 a.u.
Polarisabilité dipolaire (incertitude)
3 a.u.
C₆ (Gould–Bučko)
534 Ha·Bohr6

Paramètres de Miedema

Volume molaire de Miedema
18,28 cm3/mol
Densité électronique de Miedema
2

Risque d’approvisionnement et économie

Concentration de la production
44
Risque relatif d’approvisionnement
6
Répartition des réserves
34
Stabilité politique (principal producteur)
24
Stabilité politique (principal détenteur de réserves)
75

Transitions de phase et allotropes

Point de fusion600,61 K
Point d’ébullition2022,15 K

Catégories d’états d’oxydation

+4 main
+2 main
0 extended
−2 extended
+1 extended
−1 extended
−4 extended
+3 extended

Données de référence avancées

Constantes d’écran (15)
nOrbitaleσ
1s1,5805
2p4,5234
2s21,57
3d13,4533
3p22,8505
3s23,8477
4d37,6804
4f38,0312
4p35,9664
4s35,1072
Détail des rayons cristallins (12)
ChargeCNSpinrcrystal (pm)Origine
2IVPY112calculated,
2VI133
2VII137calculated,
2VIII143calculated,
2IX149calculated,
2X154calculated,
2XI159calculated,
2XII163
4IV79estimated,
4V87estimated,
Modes de désintégration des isotopes (59)
IsotopeModeIntensité
178A100%
178B+—
179A100%
180A100%
181A100%
181B+—
182A100%
182B+—
183A100%
183B+—
Facteurs de diffusion des rayons X (516)
Énergie (eV)f₁f₂
10—4,6699
10,1617—4,72735
10,3261—4,78551
10,4931—4,84439
10,6628—4,83957
10,8353—4,83203
11,0106—4,82451
11,1886—4,817
11,3696—4,7889
11,5535—4,7596

Données complémentaires

Sources

Sources of this element.

Lead is obtained chiefly from galena (PbS) by a roasting process. Anglesite, cerussite, and minim are other common lead minerals.

Références (1)

Isotopes in Forensic Science and Anthropology

Information on the use of this element's isotopes in forensic science and anthropology.

Different geographic regions may have characteristic terrestrial lead isotopic compositions because of variations in the ages and chemical composition of the rocks and minerals in the local environment. Therefore, lead produced at a particular location can have a unique lead isotopic composition and it is possible to trace the history and origins of pollutants by measuring the relative amounts of the four stable isotopes of lead (208Pb, 207Pb, 206Pb, and 204Pb) (Fig. IUPAC.82.2) [547] I. Renberg, M. L. Brännvall, R. Bindler, O. Emteryd. Ambio29, 150 (2000)., [548] T. J. Chow, J. L. Earl. Science169, 577 (1970).. Using isotopic abundance data, the source of this toxic metal can be identified as it moves through air and water and eventually to living systems [547] I. Renberg, M. L. Brännvall, R. Bindler, O. Emteryd. Ambio29, 150 (2000)., [549] M. K. Reuer, D. J. Weiss. Math. Phys. Eng. Sci.360, 2889 (2002).. Scientists have analyzed lead in air pollution in California and found that it originated from Asia. Airborne particles from China have relatively higher amounts of 208Pb, which distinguishes the lead isotopic signature between airborne particles from Asia and North America. This knowledge could have implications in understanding the mixing of particles in the atmosphere and how pollutants are transported over vast distances [547] I. Renberg, M. L. Brännvall, R. Bindler, O. Emteryd. Ambio29, 150 (2000)., [549] M. K. Reuer, D. J. Weiss. Math. Phys. Eng. Sci.360, 2889 (2002)., [550] S. A. Ewing, J. N. Christensen, S. T. Brown, R. A. Vancuren, S. S. Cliff, D. J. Depaolo. Environ. Sci. Technol.44, 8911 (2010)., [551] D. Krotz. Lead Isotopes Yield Clues to How Asian Air Pollution Reaches California, Lawrence Berkeley National Laboratory News Center (2014), Feb. 25; http://newscenter.lbl.gov/feature-stories/2010/12/01/lead-isotopes-air-pollution/.. Mapping the distribution of lead pollution by studying 204Pb, 206Pb, 207Pb and 208Pb also allows the identification of those human activities that contribute the highest amounts of lead to the environment [547] I. Renberg, M. L. Brännvall, R. Bindler, O. Emteryd. Ambio29, 150 (2000)., [549] M. K. Reuer, D. J. Weiss. Math. Phys. Eng. Sci.360, 2889 (2002)., [552] D. Cicchella, B. De Vivo, A. Lima, S. Albanese, R. A. R. McGill, R. R. Parrish. Geochem. Explor. Environ. Anal.8, 103 (2008)..

The measurement of the isotopic composition of lead in blood can help to determine the source of this toxic element in the body [553] R. H. Gwiazda, D. R. Smith. Environ. Health Perspect.108, 1091 (2000).. Lead is stored in bones and teeth. If a person moves to a different geographical region, the isotopic composition of the lead in the teeth is maintained, recording their place of origin. Bone can store lead for long periods of time (about 20 years), and some skeletal lead may be older and have a different isotopic composition than other skeletal lead. These differences reflect exposure to lead of different origins. By studying the isotope-amount ratio n(206Pb)/n(204Pb) and n(207Pb)/n(206Pb) in bone and teeth, it is possible to determine someone’s place of origin. For example, isotopes of lead were analyzed in the teeth and bones of a human mummy, known as the “Iceman”, to help determine his place of origin [554] B. L. Gulson, B. R. Gillings. Environ. Health Perspect.105, 820 (1997)., [555] W. Müller, H. Fricke, A. N. Halliday, M. T. McCulloch, J. A. Wartho. Science302, 862 (2003)..

210Pb is a relatively short-lived radioactive isotope of lead that is constantly produced by the decay of 222Rn in the atmosphere. While living, humans naturally incorporate 210Pb from the environment into bones and tissues. The amount of 210Pb in the body reaches equilibrium such that the 210Pb ingested is in equilibrium with the 210Pb that decays. When a person dies, this incorporation of 210Pb ceases and the relative amount of this isotope in the body decreases. Therefore, measurement of the 210Pb activity in a corpse can help determine time of death [556] D. R. Smith, J. D. Osterloh, A. R. Flegal. Environ. Health Perspect.104, 60 (1996)., [557] P. Rincon. “Isotopes could improve forensics”, in BBC News Online..

Lead isotope-amount ratios n(206Pb)/n(204Pb), n(207Pb)/n(204Pb), and n(208Pb)/n(204Pb)) along with isotope-amount ratio of silver, n(107Ag)/n(109Ag), and isotope-amount ratio of copper n(65Cu)/n(63Cu) have been used to determine the origin of European coins and to investigate the flow of goods in the world market over time [237] A. M. Desaulty, P. Telouk, E. Albalat, F. Albarede. Proc. Natl. Acad. Sci.108, 9002 (2011).. Metals from Peru and Mexico and those from European mining have distinct isotopic signatures that enable the origin of the metal to be determined by examining the isotopic compositions of silver, copper, and lead in the coins. Abundant silver sources mined in Mexico and Peru in the 16 th century were used to mint coins, but were not a major influence in the European coin market until the 18 th century [237] A. M. Desaulty, P. Telouk, E. Albalat, F. Albarede. Proc. Natl. Acad. Sci.108, 9002 (2011)..

Références (13)
  • [237] A. M. Desaulty, P. Telouk, E. Albalat, F. Albarede. Proc. Natl. Acad. Sci.108, 9002 (2011).
  • [547] I. Renberg, M. L. Brännvall, R. Bindler, O. Emteryd. Ambio29, 150 (2000).
  • [548] T. J. Chow, J. L. Earl. Science169, 577 (1970).
  • [549] M. K. Reuer, D. J. Weiss. Math. Phys. Eng. Sci.360, 2889 (2002).
  • [550] S. A. Ewing, J. N. Christensen, S. T. Brown, R. A. Vancuren, S. S. Cliff, D. J. Depaolo. Environ. Sci. Technol.44, 8911 (2010).
  • [551] D. Krotz. Lead Isotopes Yield Clues to How Asian Air Pollution Reaches California, Lawrence Berkeley National Laboratory News Center (2014), Feb. 25; http://newscenter.lbl.gov/feature-stories/2010/12/01/lead-isotopes-air-pollution/.
  • [552] D. Cicchella, B. De Vivo, A. Lima, S. Albanese, R. A. R. McGill, R. R. Parrish. Geochem. Explor. Environ. Anal.8, 103 (2008).
  • [553] R. H. Gwiazda, D. R. Smith. Environ. Health Perspect.108, 1091 (2000).
  • [554] B. L. Gulson, B. R. Gillings. Environ. Health Perspect.105, 820 (1997).
  • [555] W. Müller, H. Fricke, A. N. Halliday, M. T. McCulloch, J. A. Wartho. Science302, 862 (2003).
  • [556] D. R. Smith, J. D. Osterloh, A. R. Flegal. Environ. Health Perspect.104, 60 (1996).
  • [557] P. Rincon. “Isotopes could improve forensics”, in BBC News Online.
  • [4] IUPAC Periodic Table of the Elements and Isotopes (IPTEI) https://doi.org/10.1515/pac-2015-0703

Références

(9)
2 Atomic Mass Data Center (AMDC), International Atomic Energy Agency (IAEA)
Pb

The half-life and atomic mass data was provided by the Atomic Mass Data Center at the International Atomic Energy Agency.

3 IUPAC Commission on Isotopic Abundances and Atomic Weights (CIAAW)
Lead

Element data are cited from the Atomic weights of the elements (an IUPAC Technical Report). The IUPAC periodic table of elements can be found at https://iupac.org/what-we-do/periodic-table-of-elements/. Additional information can be found within IUPAC publication doi:10.1515/pac-2015-0703 Copyright © 2020 International Union of Pure and Applied Chemistry.

4 IUPAC Periodic Table of the Elements and Isotopes (IPTEI)

The information are cited from Pure Appl. Chem. 2018; 90(12): 1833-2092, https://doi.org/10.1515/pac-2015-0703.

Note sur la licence: Copyright (c) 2020 International Union of Pure and Applied Chemistry. The International Union of Pure and Applied Chemistry (IUPAC) contribution within Pubchem is provided under a CC-BY-NC-ND 4.0 license, unless otherwise stated.
5 Jefferson Lab, U.S. Department of Energy
Lead

Thomas Jefferson National Accelerator Facility (Jefferson Lab) is one of 17 national laboratories funded by the U.S. Department of Energy. The lab's primary mission is to conduct basic research of the atom's nucleus using the lab's unique particle accelerator, known as the Continuous Electron Beam Accelerator Facility (CEBAF). For more information visit https://www.jlab.org/

Note sur la licence: Please see citation and linking information: https://education.jlab.org/faq/index.html
6 Los Alamos National Laboratory, U.S. Department of Energy
Lead

The periodic table at the LANL (Los Alamos National Laboratory) contains basic element information together with the history, source, properties, use, handling and more. The provenance data may be found from the link under the source name.

7 NIST Physical Measurement Laboratory
Lead

The periodic table contains NIST's critically-evaluated data on atomic properties of the elements. The provenance data that include data for atomic spectroscopy, X-ray and gamma ray, radiation dosimetry, nuclear physics, and condensed matter physics may be found from the link under the source name. Ref: https://www.nist.gov/pml/atomic-spectra-database

8 PubChem Elements
Lead

This section provides all form of data related to element Lead.

9 PubChem Elements
Lead

The element property data was retrieved from publications.

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