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Pb 82

Lead (Pb)

post-transition-metal
Periodo: 6 Grupo: 14 Bloque: p

Solid

Peso atómico estándar

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

Configuración electrónica

[Xe] 6s2 4f14 5d10 6p2

Punto de fusión

327,46 °C

Punto de ebullición

1748,85 °C

Densidad

1,1342e+4 kg/m³

Estados de oxidación

−4, −2, −1, 0, +1, +2, +3, +4

Electronegatividad (Pauling)

2,33

Energía de ionización (1.ª)

7,41668 eV

Año de descubrimiento

2021

Radio atómico

180 pm

Detalles

Origen del nombre Anglo-Saxon: lead; symbol from Latin: plumbum.
Descubridores 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.

Imágenes

Propiedades

Químicas

Electronegatividad (Pauling)
2,33 Comparar Electronegatividad (Pauling) de todos los elementos →
Electronegatividad (Allen)
1,854
Afinidad electrónica
0,364 eV
Energía de ionización (1.ª)
7,41668 eV Comparar Energía de ionización (1.ª) de todos los elementos →
Energía de ionización (2.ª)
15,032551 eV Comparar Energía de ionización (2.ª) de todos los elementos →
Energía de ionización (3.ª)
31,93741 eV Comparar Energía de ionización (3.ª) de todos los elementos →
Energía de ionización (4.ª)
42,332706 eV Comparar Energía de ionización (4.ª) de todos los elementos →
Energía de ionización (5.ª)
68,800237 eV Comparar Energía de ionización (5.ª) de todos los elementos →
Estados de oxidación
−4, −2, −1, 0, +1, +2, +3, +4 Comparar Estados de oxidación de todos los elementos →
Electrones de valencia
4 Comparar Electrones de valencia de todos los elementos →
Configuración electrónica
[Xe] 6s2 4f14 5d10 6p2

Termodinámicas

Calor de fusión
0,04943774 eV Comparar Calor de fusión de todos los elementos →
Calor de vaporización
1,860393 eV Comparar Calor de vaporización de todos los elementos →
Calor de sublimación
2,023112 eV
Calor de atomización
2,023112 eV
Entalpía de atomización
2,023112 eV

Nucleares

Protones
82 Comparar Protones de todos los elementos →
Neutrones
126 Comparar Neutrones de todos los elementos →
Isótopos conocidos
43 Comparar Isótopos conocidos de todos los elementos →
Isótopos estables
0 Comparar Isótopos estables de todos los elementos →
Isótopo más estable
Pb-208
Año de descubrimiento
2021

Abundancia

Abundancia (corteza terrestre)
14 mg/kg Comparar Abundancia (corteza terrestre) de todos los elementos →
Abundancia (océano)
3 × 10−5 mg/L Comparar Abundancia (océano) de todos los elementos →

Estructura cristalina

Constante de red a
495 pm

Estructura electrónica

Electrones por capa
2, 8, 18, 32, 18, 4 Comparar Electrones por capa de todos los elementos →

Identificadores

Número CAS
7439-92-1 Comparar Número CAS de todos los elementos →
Símbolo del término
(1/2,1/2)0
InChI
InChI=1S/Pb
Clave InChI
WABPQHHGFIMREM-UHFFFAOYSA-N

Configuración electrónica Medido

Carga del ion
Protones 82
Electrones 82
Carga Neutro
Configuración Pb: 4f¹⁴ 5d¹⁰ 6s² 6p²
Configuración electrónica
Medido
[Xe] 4f¹⁴ 5d¹⁰ 6s² 6p²
1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p²
Diagrama de 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↑
Total de electrones: 82 Desapareados: 2 ?

Modelo atómico

Protones 82
Neutrones 102
Electrones 82
Número másico 184
Estabilidad Radiactivo

Los isótopos cambian el número de neutrones, la masa y la estabilidad, pero no la configuración electrónica de un átomo neutro.

Modelo atómico esquemático, no a escala.

Huella atómica

Espectro de emisión / absorción

25 / 26 (26 26 con intensidad)
Medido
Emisión Visible: 380–750 nm

Distribución isotópica

No hay isótopos estables.

Número másicoMasa atómica (u)Abundancia naturalPeriodo de semidesintegración
183 Radiactivo182,991872 ± 0,00003N/D535 ms
184 Radiactivo183,988136 ± 0,000014N/D490 ms
178 Radiactivo178,003831 ± 0,000026N/D250 us
215 Radiactivo215,00474 ± 0,00011N/D142 segundos
204 Radiactivo203,973044 ± 0,00000131,4000%140 Py
Medido

Fase / Estado

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

Motivo: 302,5 °C por debajo del punto de fusión (327,46 °C)

Punto de fusión 327,46 °C
Punto de ebullición 1748,85 °C
Por debajo del punto de fusión en 302,5 °C
0 K Temperatura actual: 25 °C 6000 K
Secuencia de fases

Esquemático, no a escala

Sólido
Líquido
Gas
Fusión
Ebullición
25°C
Sólido
Líquido
Gas
Actual

Puntos de transición de fase

Punto de fusión Bibliografía
327,46 °C
Punto de ebullición Bibliografía
1748,85 °C
Fase actual Calculado
Sólido

Energías de transición

Calor de fusión Bibliografía
0,04943774 eV

Energía necesaria para fundir 1 mol en el punto de fusión

Calor de vaporización Bibliografía
1,860393 eV

Energía necesaria para vaporizar 1 mol en el punto de ebullición

Calor de sublimación Bibliografía
2,023112 eV

Energía necesaria para sublimar 1 mol en el punto de sublimación

Densidad

Densidad de referencia Bibliografía
1,1342e+4 kg/m³

En condiciones estándar

Densidad actual Calculado
1,1342e+4 kg/m³

En condiciones estándar

Espectros atómicos

Se muestran 10 de 82. Ordenado por carga del ion (ascendente).

Líneas disponibles ?

IonCargaTotal de líneasProbabilidades de transiciónDesignaciones de los niveles
Pb I 013528135
Pb II +197312
Pb III +24100
Pb IV +39200
Pb V +49000
Líneas disponibles en el NIST →

Niveles disponibles ?

IonCargaNiveles
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
Niveles disponibles en el NIST →
82 Pb 207.2

Lead — Visualizador de orbitales atómicos

[Xe]6s24f145d106p2
Niveles de energía 2 8 18 32 18 4
Estados de oxidación -4, -2, -1, 0, +1, +2, +3, +4
HOMO 6p n=6 · l=1 · m=-1
Lead — Vista previa del visualizador de orbitales atómicos
Three.js solo se carga cuando se solicita
82 Pb 207.2

Lead — Visualizador de estructuras cristalinas

Face-Centered Cubic · Pearson cF4
Experimental
Pearson cF4
N.º de coord. 12
Empaquetamiento 74.000%
Lead — Vista previa del visualizador de estructuras cristalinas
Three.js solo se carga cuando se solicita

Radios iónicos

Se muestran 10 de 12.

CargaCoordinaciónEspínRadio
+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

Compuestos

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

Isótopos (5)

Número másicoMasa atómica (u)Abundancia naturalPeriodo de semidesintegraciónModo de desintegración
183 Radiactivo182,991872 ± 0,00003N/D535 ms
α ≈100%β+ ?
184 Radiactivo183,988136 ± 0,000014N/D490 ms
α =80±1.1%β+ ?
178 Radiactivo178,003831 ± 0,000026N/D250 us
α ≈100%β+ ?
215 Radiactivo215,00474 ± 0,00011N/D142 segundos
β- =100%
204 Radiactivo203,973044 ± 0,00000131,4000% ± 0,1000%140 Py
IS =1.4±0.6%α ?
183 Radiactivo
Masa atómica (u) 182,991872 ± 0,00003
Abundancia natural N/D
Periodo de semidesintegración 535 ms
Modo de desintegración
α ≈100%β+ ?
184 Radiactivo
Masa atómica (u) 183,988136 ± 0,000014
Abundancia natural N/D
Periodo de semidesintegración 490 ms
Modo de desintegración
α =80±1.1%β+ ?
178 Radiactivo
Masa atómica (u) 178,003831 ± 0,000026
Abundancia natural N/D
Periodo de semidesintegración 250 us
Modo de desintegración
α ≈100%β+ ?
215 Radiactivo
Masa atómica (u) 215,00474 ± 0,00011
Abundancia natural N/D
Periodo de semidesintegración 142 segundos
Modo de desintegración
β- =100%
204 Radiactivo
Masa atómica (u) 203,973044 ± 0,0000013
Abundancia natural 1,4000% ± 0,1000%
Periodo de semidesintegración 140 Py
Modo de desintegración
IS =1.4±0.6%α ?

Líneas espectrales

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

Propiedades ampliadas

Radios covalentes (ampliados)

Radio covalente (Pyykkö)
144 pm
Radio covalente (Pyykkö, enlace doble)
135 pm
Radio covalente (Pyykkö, enlace triple)
137 pm

Radios de van der Waals

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

Radios atómicos y metálicos

Radio atómico (Rahm)
249 pm
Radio metálico (C12)
170 pm

Escalas de numeración

Mendeleev
91
Pettifor
82
Glawe
82

Escalas de electronegatividad

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

Polarizabilidad y dispersión

Polarizabilidad dipolar
47 a.u.
Polarizabilidad dipolar (incert.)
3 a.u.
C₆ (Gould–Bučko)
534 Ha·Bohr6

Parámetros de Miedema

Volumen molar de Miedema
18,28 cm3/mol
Densidad electrónica de Miedema
2

Riesgo de suministro y economía

Concentración de la producción
44
Riesgo relativo de suministro
6
Distribución de las reservas
34
Estabilidad política (principal productor)
24
Estabilidad política (país con mayores reservas)
75

Transiciones de fase y alótropos

Punto de fusión600,61 K
Punto de ebullición2022,15 K

Categorías de estados de oxidación

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

Datos de referencia avanzados

Constantes de apantallamiento (15)
nOrbitalσ
1s1,5805
2p4,5234
2s21,57
3d13,4533
3p22,8505
3s23,8477
4d37,6804
4f38,0312
4p35,9664
4s35,1072
Detalle de los radios cristalinos (12)
CargaCNEspínrcrystal (pm)Origen
2IVPY112calculated,
2VI133
2VII137calculated,
2VIII143calculated,
2IX149calculated,
2X154calculated,
2XI159calculated,
2XII163
4IV79estimated,
4V87estimated,
Modos de desintegración de los isótopos (59)
IsótopoModoIntensidad
178A100%
178B+—
179A100%
180A100%
181A100%
181B+—
182A100%
182B+—
183A100%
183B+—
Factores de dispersión de rayos X (516)
Energía (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

Datos adicionales

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.

Referencias (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)..

Referencias (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).
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Referencias

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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 sobre la licencia: 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 sobre la licencia: 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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