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Pb 82

Lead (Pb)

post-transition-metal
Periodo: 6 Gruppo: 14 Blocco: p

Solid

Peso atomico standard

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

Configurazione elettronica

[Xe] 6s2 4f14 5d10 6p2

Punto di fusione

327,46 °C

Punto di ebollizione

1748,85 °C

Densità

1,1342e+4 kg/m³

Stati di ossidazione

−4, −2, −1, 0, +1, +2, +3, +4

Elettronegatività (Pauling)

2,33

Energia di ionizzazione (1ª)

7,41668 eV

Anno della scoperta

2021

Raggio atomico

180 pm

Dettagli

Origine del nome Anglo-Saxon: lead; symbol from Latin: plumbum.
Scopritori 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.

Immagini

Proprietà

Chimiche

Elettronegatività (Pauling)
2,33 Confronta Elettronegatività (Pauling) di tutti gli elementi →
Elettronegatività (Allen)
1,854
Affinità elettronica
0,364 eV
Energia di ionizzazione (1ª)
7,41668 eV Confronta Energia di ionizzazione (1ª) di tutti gli elementi →
Energia di ionizzazione (2ª)
15,032551 eV Confronta Energia di ionizzazione (2ª) di tutti gli elementi →
Energia di ionizzazione (3ª)
31,93741 eV Confronta Energia di ionizzazione (3ª) di tutti gli elementi →
Energia di ionizzazione (4ª)
42,332706 eV Confronta Energia di ionizzazione (4ª) di tutti gli elementi →
Energia di ionizzazione (5ª)
68,800237 eV Confronta Energia di ionizzazione (5ª) di tutti gli elementi →
Stati di ossidazione
−4, −2, −1, 0, +1, +2, +3, +4 Confronta Stati di ossidazione di tutti gli elementi →
Elettroni di valenza
4 Confronta Elettroni di valenza di tutti gli elementi →
Configurazione elettronica
[Xe] 6s2 4f14 5d10 6p2

Termodinamiche

Calore di fusione
0,04943774 eV Confronta Calore di fusione di tutti gli elementi →
Calore di vaporizzazione
1,860393 eV Confronta Calore di vaporizzazione di tutti gli elementi →
Calore di sublimazione
2,023112 eV
Calore di atomizzazione
2,023112 eV
Entalpia di atomizzazione
2,023112 eV

Abbondanza

Abbondanza (crosta terrestre)
14 mg/kg Confronta Abbondanza (crosta terrestre) di tutti gli elementi →
Abbondanza (oceano)
3 × 10−5 mg/L Confronta Abbondanza (oceano) di tutti gli elementi →

Struttura cristallina

Costante reticolare a
495 pm

Struttura elettronica

Elettroni per guscio
2, 8, 18, 32, 18, 4 Confronta Elettroni per guscio di tutti gli elementi →

Identificativi

Numero CAS
7439-92-1 Confronta Numero CAS di tutti gli elementi →
Simbolo di termine
(1/2,1/2)0
InChI
InChI=1S/Pb
Chiave InChI
WABPQHHGFIMREM-UHFFFAOYSA-N

Configurazione elettronica Misurato

Carica ionica
Protoni 82
Elettroni 82
Carica Neutro
Configurazione Pb: 4f¹⁴ 5d¹⁰ 6s² 6p²
Configurazione elettronica
Misurato
[Xe] 4f¹⁴ 5d¹⁰ 6s² 6p²
1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p²
Diagramma degli orbitali
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↑
Elettroni totali: 82 Spaiati: 2 ?

Modello atomico

Protoni 82
Neutroni 102
Elettroni 82
Numero di massa 184
Stabilità Radioattivo

Gli isotopi modificano il numero di neutroni, la massa e la stabilità — non la configurazione elettronica di un atomo neutro.

Modello atomico schematico, non in scala.

Impronta atomica

Spettro di emissione / assorbimento

25 / 26 (26 26 con intensità)
Misurato
Emissione Visibile: 380–750 nm

Distribuzione isotopica

Nessun isotopo stabile.

Numero di massaMassa atomica (u)Abbondanza naturaleEmivita
183 Radioattivo182,991872 ± 0,00003N/D535 ms
184 Radioattivo183,988136 ± 0,000014N/D490 ms
178 Radioattivo178,003831 ± 0,000026N/D250 us
215 Radioattivo215,00474 ± 0,00011N/D142 secondi
204 Radioattivo203,973044 ± 0,00000131,4000%140 Py
Misurato

Fase / Stato

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

Motivo: 302,5 °C sotto il punto di fusione (327,46 °C)

Punto di fusione 327,46 °C
Punto di ebollizione 1748,85 °C
Sotto il punto di fusione di 302,5 °C
0 K Temperatura attuale: 25 °C 6000 K
Sequenza delle fasi

Schema non in scala

Solido
Liquido
Gas
Fusione
Ebollizione
25°C
Solido
Liquido
Gas
Attuale

Punti di transizione di fase

Punto di fusione Letteratura
327,46 °C
Punto di ebollizione Letteratura
1748,85 °C
Fase attuale Calcolato
Solido

Energie di transizione

Calore di fusione Letteratura
0,04943774 eV

Energia necessaria per fondere 1 mol al punto di fusione

Calore di vaporizzazione Letteratura
1,860393 eV

Energia necessaria per vaporizzare 1 mol al punto di ebollizione

Calore di sublimazione Letteratura
2,023112 eV

Energia necessaria per sublimare 1 mol al punto di sublimazione

Densità

Densità di riferimento Letteratura
1,1342e+4 kg/m³

In condizioni standard

Densità attuale Calcolato
1,1342e+4 kg/m³

In condizioni standard

Spettri atomici

Sono visualizzati 10 di 82. Ordinamento per carica ionica crescente.

Righe disponibili ?

IoneCaricaRighe totaliProbabilità di transizioneDesignazioni dei livelli
Pb I 013528135
Pb II +197312
Pb III +24100
Pb IV +39200
Pb V +49000
Righe disponibili nel NIST →

Livelli disponibili ?

IoneCaricaLivelli
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
Livelli disponibili nel NIST →
82 Pb 207.2

Lead — Visualizzatore degli orbitali atomici

[Xe]6s24f145d106p2
Livelli energetici 2 8 18 32 18 4
Stati di ossidazione -4, -2, -1, 0, +1, +2, +3, +4
HOMO 6p n=6 · l=1 · m=-1
Lead — Anteprima del visualizzatore degli orbitali atomici
Three.js viene caricato soltanto su richiesta
82 Pb 207.2

Lead — Visualizzatore della struttura cristallina

Face-Centered Cubic · Pearson cF4
Sperimentale
Pearson cF4
N. coord. 12
Impacchettamento 74.000%
Lead — Anteprima del visualizzatore della struttura cristallina
Three.js viene caricato soltanto su richiesta

Raggi ionici

Sono visualizzati 10 di 12.

CaricaCoordinazioneSpinRaggio
+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

Composti

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

Isotopi (5)

Numero di massaMassa atomica (u)Abbondanza naturaleEmivitaModalità di decadimento
183 Radioattivo182,991872 ± 0,00003N/D535 ms
α ≈100%β+ ?
184 Radioattivo183,988136 ± 0,000014N/D490 ms
α =80±1.1%β+ ?
178 Radioattivo178,003831 ± 0,000026N/D250 us
α ≈100%β+ ?
215 Radioattivo215,00474 ± 0,00011N/D142 secondi
β- =100%
204 Radioattivo203,973044 ± 0,00000131,4000% ± 0,1000%140 Py
IS =1.4±0.6%α ?
183 Radioattivo
Massa atomica (u) 182,991872 ± 0,00003
Abbondanza naturale N/D
Emivita 535 ms
Modalità di decadimento
α ≈100%β+ ?
184 Radioattivo
Massa atomica (u) 183,988136 ± 0,000014
Abbondanza naturale N/D
Emivita 490 ms
Modalità di decadimento
α =80±1.1%β+ ?
178 Radioattivo
Massa atomica (u) 178,003831 ± 0,000026
Abbondanza naturale N/D
Emivita 250 us
Modalità di decadimento
α ≈100%β+ ?
215 Radioattivo
Massa atomica (u) 215,00474 ± 0,00011
Abbondanza naturale N/D
Emivita 142 secondi
Modalità di decadimento
β- =100%
204 Radioattivo
Massa atomica (u) 203,973044 ± 0,0000013
Abbondanza naturale 1,4000% ± 0,1000%
Emivita 140 Py
Modalità di decadimento
IS =1.4±0.6%α ?

Righe spettrali

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

Proprietà estese

Raggi covalenti (dati estesi)

Raggio covalente (Pyykkö)
144 pm
Raggio covalente (Pyykkö, legame doppio)
135 pm
Raggio covalente (Pyykkö, legame triplo)
137 pm

Raggi di van der Waals

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

Raggi atomici e metallici

Raggio atomico (Rahm)
249 pm
Raggio metallico (C12)
170 pm

Scale di numerazione

Mendeleev
91
Pettifor
82
Glawe
82

Scale di elettronegatività

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

Polarizzabilità e dispersione

Polarizzabilità dipolare
47 a.u.
Polarizzabilità dipolare (inc.)
3 a.u.
C₆ (Gould–Bučko)
534 Ha·Bohr6

Parametri di Miedema

Volume molare di Miedema
18,28 cm3/mol
Densità elettronica di Miedema
2

Rischio di approvvigionamento ed economia

Concentrazione della produzione
44
Rischio relativo di approvvigionamento
6
Distribuzione delle riserve
34
Stabilità politica (principale produttore)
24
Stabilità politica (principale detentore di riserve)
75

Transizioni di fase e allotropi

Punto di fusione600,61 K
Punto di ebollizione2022,15 K

Categorie degli stati di ossidazione

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

Dati di riferimento avanzati

Costanti di schermaggio (15)
nOrbitaleσ
1s1,5805
2p4,5234
2s21,57
3d13,4533
3p22,8505
3s23,8477
4d37,6804
4f38,0312
4p35,9664
4s35,1072
Dettaglio dei raggi cristallini (12)
CaricaCNSpinrcrystal (pm)Origine
2IVPY112calculated,
2VI133
2VII137calculated,
2VIII143calculated,
2IX149calculated,
2X154calculated,
2XI159calculated,
2XII163
4IV79estimated,
4V87estimated,
Modalità di decadimento degli isotopi (59)
IsotopoModalitàIntensità
178A100%
178B+—
179A100%
180A100%
181A100%
181B+—
182A100%
182B+—
183A100%
183B+—
Fattori di diffusione dei raggi X (516)
Energia (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

Dati aggiuntivi

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.

Riferimenti (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)..

Riferimenti (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/.
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Riferimenti

(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.

Nota sulla licenza: 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/

Nota sulla licenza: 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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