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H 1

Hydrogen (H)

nonmetal
Periode: 1 Golongan: 1 Blok: s

Gas

Bobot Atom Standar

1,008 u [1,00784, 1,00811]

Konfigurasi elektron

1s1

Titik lebur

-259,34 °C

Titik didih

-252,87 °C

Massa jenis

0,08988 kg/m³

Bilangan oksidasi

−1, +1

Keelektronegatifan (Pauling)

2,2

Energi ionisasi (ke-1)

13,598435 eV

Tahun penemuan

1766

Jari-jari atom

25 pm

Detail

Asal nama Greek: hydro (water) and genes (generate)
Negara penemuan England
Penemu Henry Cavendish

The lightest chemical element, hydrogen sits above the alkali metals but is a nonmetal under ordinary conditions. Its single proton and one electron make it the simplest atom and a reference point for much of chemistry. On Earth it is usually bound in water and organic matter, while industry uses it as a chemical feedstock, reducing agent, fuel, and energy carrier.

Colourless, odourless gaseous chemical element. Lightest and most abundant element in the universe. Present in water and in all organic compounds. Chemically reacts with most elements. Discovered by Henry Cavendish in 1776.

The name derives from the Greek hydro for "water" and genes for "forming" because it burned in air to form water. Hydrogen was discovered by the English physicist Henry Cavendish in 1766.

Scientists had been producing hydrogen for years before it was recognized as an element. Written records indicate that Robert Boyle produced hydrogen gas as early as 1671 while experimenting with iron and acids. Hydrogen was first recognized as a distinct element by Henry Cavendish in 1766. Composed of a single proton and a single electron, hydrogen is the simplest and most abundant element in the universe. It is estimated that 90% of the visible universe is composed of hydrogen.

Hydrogen is the raw fuel that most stars 'burn' to produce energy. The same process, known as fusion, is being studied as a possible power source for use on earth. The sun's supply of hydrogen is expected to last another 5 billion years.

From the Greek word hydro (water), and genes (forming). Hydrogen was recognized as a distinct substance by Henry Cavendish in 1776. Diagram of a simple hydrogen atom.

Hydrogen is the most abundant of all elements in the universe. The heavier elements were originally made from hydrogen atoms or from other elements that were originally made from hydrogen atoms.

Gambar

Sifat

Fisika

Jari-jari atom (empiris)
25 pm Bandingkan Jari-jari atom (empiris) semua unsur →
Jari-jari kovalen
31 pm Bandingkan Jari-jari kovalen semua unsur →
Jari-jari van der Waals
120 pm Bandingkan Jari-jari van der Waals semua unsur →
Massa jenis
0,08988 kg/m³ Bandingkan Massa jenis semua unsur →
Volume molar
0,0141 L/mol
Fase pada STP
Gas Bandingkan Fase pada STP semua unsur →
Titik lebur
-259,34 °C Bandingkan Titik lebur semua unsur →
Titik didih
-252,87 °C Bandingkan Titik didih semua unsur →
Konduktivitas termal
0,181 W/(m·K) Bandingkan Konduktivitas termal semua unsur →
Kapasitas kalor spesifik
14,304 J/(g·K) Bandingkan Kapasitas kalor spesifik semua unsur →
Kapasitas kalor molar
28,836 J/(mol·K) Bandingkan Kapasitas kalor molar semua unsur →
Struktur kristal
Heksagonal susunan rapat Bandingkan Struktur kristal semua unsur →

Kimia

Keelektronegatifan (Pauling)
2,2 Bandingkan Keelektronegatifan (Pauling) semua unsur →
Keelektronegatifan (Allen)
2,3
Afinitas elektron
0,75419 eV
Energi ionisasi (ke-1)
13,598435 eV Bandingkan Energi ionisasi (ke-1) semua unsur →
Bilangan oksidasi
−1, +1 Bandingkan Bilangan oksidasi semua unsur →
Elektron valensi
1 Bandingkan Elektron valensi semua unsur →
Konfigurasi elektron
1s1

Termodinamika

Titik tripel (suhu)
-259,3467 °C
Titik tripel (tekanan)
7041 Pa
Titik kritis (suhu)
-240,212 °C
Titik kritis (tekanan)
1,2858e+6 Pa
Kalor peleburan
0,00121262 eV Bandingkan Kalor peleburan semua unsur →
Kalor penguapan
0,00936933 eV Bandingkan Kalor penguapan semua unsur →
Kalor atomisasi
2,259398 eV
Entalpi atomisasi
2,259398 eV

Nuklir

Proton
1 Bandingkan Proton semua unsur →
Neutron
0 Bandingkan Neutron semua unsur →
Isotop yang diketahui
7 Bandingkan Isotop yang diketahui semua unsur →
Isotop stabil
2 Bandingkan Isotop stabil semua unsur →
Isotop paling stabil
H-1
Tahun penemuan
1766

Kelimpahan

Kelimpahan (kerak Bumi)
1400 mg/kg Bandingkan Kelimpahan (kerak Bumi) semua unsur →
Kelimpahan (samudra)
1,08 × 105 mg/L Bandingkan Kelimpahan (samudra) semua unsur →

Struktur Kristal

Konstanta kisi a
375 pm

Struktur Elektronik

Elektron per kulit
1 Bandingkan Elektron per kulit semua unsur →

Pengenal

Nomor CAS
1333-74-0 Bandingkan Nomor CAS semua unsur →
Simbol term
2S1/2
InChI
InChI=1S/H
Kunci InChI
YZCKVEUIGOORGS-UHFFFAOYSA-N

Konfigurasi Elektron Diukur

Muatan ion
Proton 1
Elektron 1
Muatan Netral
Konfigurasi H: 1s¹
Konfigurasi elektron
Diukur
1s¹
1s¹
Diagram orbital
1s
1/2 1↑
Total elektron: 1 Tidak berpasangan: 1 ?

Model atom

Proton 1
Neutron 0
Elektron 1
Nomor massa 1
Kestabilan Stabil

Isotop mengubah jumlah neutron, massa, dan kestabilan — bukan konfigurasi elektron atom netral.

Model atom skematis, tidak sesuai skala.

Sidik Jari Atom

Spektrum Emisi / Absorpsi

25 / 91 (7 7 dengan intensitas)
Diukur
Emisi Tampak: 380–750 nm

Distribusi Isotop

199,9885%20,0115%Nomor massaKelimpahan alami (%)
Nomor massaMassa atom (u)Kelimpahan alamiWaktu paruh
1 Stabil1,00782503223 ± 0,0000000000999,9885%Stabil
2 Stabil2,01410177812 ± 0,000000000120,0115%Stabil
Diukur

Fase / Wujud

1 atm / 101.325 kPa
Gas 25 °C (298,15 K)

Alasan: 277,9 °C di atas titik didih (-252,87 °C)

Titik lebur -259,34 °C
Titik didih -252,87 °C
Di atas titik didih sebesar 277,9 °C
0 K Suhu saat ini: 25 °C 6000 K
Linimasa fase

Skematis, tidak sesuai skala

Padat
Cair
Gas
Peleburan
Pendidihan
25°C
Padat
Cair
Gas
Saat ini

Titik transisi fase

Titik lebur Literatur
-259,34 °C
Titik didih Literatur
-252,87 °C
Fase saat ini Dihitung
Gas

Energi transisi

Kalor peleburan Literatur
0,00121262 eV

Energi yang diperlukan untuk meleburkan 1 mol pada titik lebur

Kalor penguapan Literatur
0,00936933 eV

Energi yang diperlukan untuk menguapkan 1 mol pada titik didih

Massa jenis

Massa jenis referensi Literatur
0,08988 kg/m³

Pada kondisi standar

Massa jenis saat ini Diperkirakan
0,04120002 kg/m³

Diperkirakan menggunakan hukum gas ideal pada T saat ini

Lanjutan

Titik tripel Literatur
-259,3467 °C
Titik kritis Literatur
-240,212 °C

Spektrum Atom

Data Garis Spektrum ?

IonMuatanTotal garisProbabilitas transisiPenamaan tingkat energi
D I Isotop0364161341
H I 0568441535
T I Isotop0111111
Data Garis Spektrum NIST →

Data Tingkat Energi ?

IonMuatanTingkat energi
D I Isotop078
H I 0106
T I Isotop010
Data Tingkat Energi NIST →
1 H 1.007975

Hydrogen — Visualisasi Orbital Atom

1s1
Tingkat energi 1
Bilangan oksidasi -1, +1
HOMO 1s n=1 · l=0 · m=0
Hydrogen — Pratinjau Visualisasi Orbital Atom
Three.js hanya dimuat saat diminta
1 H 1.007975

Hydrogen — Visualisasi Struktur Kristal

Heksagonal Primitif · Pearson hP2
Eksperimental
Pearson hP2
No. Koord. 12
Pengemasan 74.048%
Tidak memiliki struktur kristal pada kondisi standar — gas pada 298 K, 1 atm
Struktur fase padat pada 293 K
Hydrogen — Pratinjau Visualisasi Struktur Kristal
Three.js hanya dimuat saat diminta

Senyawa

H+
1,008 u
H
1,008 u
H-
1,008 u
H+
1,008 u
H+
2,014 u
H+
3,016 u
H
3,016 u
H
2,014 u
H-
3,016 u
H-
2,014 u
H-
1,008 u
H
1,008 u

Isotop (2)

The ordinary isotope of hydrogen, H, is known as Protium, the other two isotopes are Deuterium (a proton and a neutron) and Tritium (a protron and two neutrons). Hydrogen is the only element whose isotopes have been given different names. Deuterium and Tritium are both used as fuel in nuclear fusion reactors. One atom of Deuterium is found in about 6000 ordinary hydrogen atoms.

Nomor massaMassa atom (u)Kelimpahan alamiWaktu paruhMode peluruhan
1 Stabil1,00782503223 ± 0,0000000000999,9885% ± 0,0070%Stabil
stable
2 Stabil2,01410177812 ± 0,000000000120,0115% ± 0,0070%Stabil
stable
1 Stabil
Massa atom (u) 1,00782503223 ± 0,00000000009
Kelimpahan alami 99,9885% ± 0,0070%
Waktu paruh Stabil
Mode peluruhan
stable
2 Stabil
Massa atom (u) 2,01410177812 ± 0,00000000012
Kelimpahan alami 0,0115% ± 0,0070%
Waktu paruh Stabil
Mode peluruhan
stable

Garis Spektrum

Panjang gelombang (nm)IntensitasTahap ionisasiJenisTransisiAkurasiSumber
383.5355892 nmTidak tersediaH Iemission2p 2P* → 9d 2DDiukurNIST
383.5356424 nmTidak tersediaH Iemission2p 2P* → 9s 2SDiukurNIST
383.53587 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
383.5361082 nmTidak tersediaH Iemission2s 2S → 9p 2P*DiukurNIST
383.5361616 nmTidak tersediaH Iemission2s 2S → 9s 2SDiukurNIST
383.5361673 nmTidak tersediaH Iemission2s 2S → 9p 2P*DiukurNIST
383.53839 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
383.53909 nm30000H Iemission2 → 9DiukurNIST
383.5409535 nmTidak tersediaH Iemission2p 2P* → 9d 2DDiukurNIST
383.54096 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
383.5409732 nmTidak tersediaH Iemission2p 2P* → 9d 2DDiukurNIST
383.5410263 nmTidak tersediaH Iemission2p 2P* → 9s 2SDiukurNIST
388.9019815 nmTidak tersediaH Iemission2p 2P* → 8d 2DDiukurNIST
388.9020595 nmTidak tersediaH Iemission2p 2P* → 8s 2SDiukurNIST
388.90227 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
388.9024865 nmTidak tersediaH Iemission2s 2S → 8d 2DDiukurNIST
388.9025152 nmTidak tersediaH Iemission2s 2S → 8p 2P*DiukurNIST
388.9025154 nmTidak tersediaH Iemission2s 2S → 8d 2DDiukurNIST
388.9025933 nmTidak tersediaH Iemission2s 2S → 8s 2SDiukurNIST
388.9026017 nmTidak tersediaH Iemission2s 2S → 8p 2P*DiukurNIST
388.90486 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
388.90557 nm70000H Iemission2 → 8DiukurNIST
388.9074883 nmTidak tersediaH Iemission2p 2P* → 8d 2DDiukurNIST
388.90749 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
388.9075172 nmTidak tersediaH Iemission2p 2P* → 8d 2DDiukurNIST
388.9075951 nmTidak tersediaH Iemission2p 2P* → 8s 2SDiukurNIST
397.0041763 nmTidak tersediaH Iemission2p 2P* → 7d 2DDiukurNIST
397.0042976 nmTidak tersediaH Iemission2p 2P* → 7s 2SDiukurNIST
397.00448 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
397.0047325 nmTidak tersediaH Iemission2s 2S → 7p 2P*DiukurNIST
397.0048539 nmTidak tersediaH Iemission2s 2S → 7s 2SDiukurNIST
397.004867 nmTidak tersediaH Iemission2s 2S → 7p 2P*DiukurNIST
397.00719 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
397.00788 nm30000H Iemission2 → 7DiukurNIST
397.0099002 nmTidak tersediaH Iemission2p 2P* → 7d 2DDiukurNIST
397.00991 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
397.009945 nmTidak tersediaH Iemission2p 2P* → 7d 2DDiukurNIST
397.0100663 nmTidak tersediaH Iemission2p 2P* → 7s 2SDiukurNIST
410.1702284 nmTidak tersediaH Iemission2p 2P* → 6d 2DDiukurNIST
410.1704339 nmTidak tersediaH Iemission2p 2P* → 6s 2SDiukurNIST
410.17056 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
410.1707462 nmTidak tersediaH Iemission2s 2S → 6d 2DDiukurNIST
410.1708218 nmTidak tersediaH Iemission2s 2S → 6p 2P*DiukurNIST
410.1710277 nmTidak tersediaH Iemission2s 2S → 6s 2SDiukurNIST
410.1710499 nmTidak tersediaH Iemission2s 2S → 6p 2P*DiukurNIST
410.17346 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
410.17415 nm70000H Iemission2 → 6DiukurNIST
410.17631 nmTidak tersediaH Iemission2p 2P* → 6d 2DDiukurNIST
410.17632 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
410.176386 nmTidak tersediaH Iemission2p 2P* → 6d 2DDiukurNIST
410.1765915 nmTidak tersediaH Iemission2p 2P* → 6s 2SDiukurNIST
434.0426937 nmTidak tersediaH Iemission2p 2P* → 5d 2DDiukurNIST
434.04309 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
434.0430904 nmTidak tersediaH Iemission2p 2P* → 5s 2SDiukurNIST
434.0433568 nmTidak tersediaH Iemission2s 2S → 5p 2P*DiukurNIST
434.0437554 nmTidak tersediaH Iemission2s 2S → 5s 2SDiukurNIST
434.0437982 nmTidak tersediaH Iemission2s 2S → 5p 2P*DiukurNIST
434.04634 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
434.0471 nm90000H Iemission2 → 5DiukurNIST
434.0494419 nmTidak tersediaH Iemission2p 2P* → 5d 2DDiukurNIST
434.04947 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
434.0495889 nmTidak tersediaH Iemission2p 2P* → 5d 2DDiukurNIST
434.0499857 nmTidak tersediaH Iemission2p 2P* → 5s 2SDiukurNIST
486.1278624 nmTidak tersediaH Iemission2p 2P* → 4d 2DDiukurNIST
486.1283363 nmTidak tersediaH Iemission2s 2S → 4d 2DDiukurNIST
486.12841 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
486.1286949 nmTidak tersediaH Iemission2s 2S → 4p 2P*DiukurNIST
486.128837 nmTidak tersediaH Iemission2p 2P* → 4s 2SDiukurNIST
486.1296711 nmTidak tersediaH Iemission2s 2S → 4s 2SDiukurNIST
486.1297761 nmTidak tersediaH Iemission2s 2S → 4p 2P*DiukurNIST
486.1325 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
486.1333 nm180000H Iemission2 → 4DiukurNIST
486.1361516 nmTidak tersediaH Iemission2p 2P* → 4d 2DDiukurNIST
486.13622 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
486.1365118 nmTidak tersediaH Iemission2p 2P* → 4d 2DDiukurNIST
486.1374864 nmTidak tersediaH Iemission2p 2P* → 4s 2SDiukurNIST
656.27097 nmTidak tersediaH Iemission2p 2P* → 3d 2DDiukurNIST
656.2714 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
656.2722 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
656.272483 nmTidak tersediaH Iemission2s 2S → 3p 2P*DiukurNIST
656.275181 nmTidak tersediaH Iemission2p 2P* → 3s 2SDiukurNIST
656.276701 nmTidak tersediaH Iemission2s 2S → 3s 2SDiukurNIST
656.277 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
656.277153 nmTidak tersediaH Iemission2s 2S → 3p 2P*DiukurNIST
656.2795 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
656.2819 nm500000H Iemission2 → 3DiukurNIST
656.285177 nmTidak tersediaH Iemission2p 2P* → 3d 2DDiukurNIST
656.28533 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
656.2854 nmTidak tersediaH IemissionTidak tersediaDiukurNIST
656.286734 nmTidak tersediaH Iemission2p 2P* → 3d 2DDiukurNIST
656.290944 nmTidak tersediaH Iemission2p 2P* → 3s 2SDiukurNIST

Sifat Lanjutan

Jari-jari Kovalen (Lanjutan)

Jari-jari kovalen (Pyykkö)
32 pm

Jari-jari van der Waals

Bondi
120 pm
Alvarez
120 pm
UFF
288,6 pm
MM3
162 pm
Dreiding
319,5 pm
Rowland–Taylor
110 pm

Jari-jari Atom & Logam

Jari-jari atom (Rahm)
154 pm
Jari-jari logam (C12)
78 pm

Skala Penomoran

Mendeleev
105
Pettifor
103
Glawe
103

Skala Keelektronegatifan

Ghosh
0
Miedema
5
Gunnarsson–Lundqvist
6
Robles–Bartolotti
5

Polarizabilitas & Dispersi

Polarizabilitas dipol
4,5071 a.u.
Polarizabilitas dipol (ketidakpastian)
0 a.u.
C₆
6,499 Ha·Bohr6
C₆ (Gould–Bučko)
6,51 Ha·Bohr6

Parameter Miedema

Volume molar Miedema
1,7 cm3/mol
Kerapatan elektron Miedema
3

Transisi Fase & Alotrop

Titik lebur13,99 K
Titik didih20,27 K
Titik kritis (suhu)32,94 K
Titik kritis (tekanan)1,29 MPa
Titik tripel (suhu)13,8 K
Titik tripel (tekanan)7,04 kPa

Kategori Bilangan Oksidasi

+1 main
−1 main

Data Referensi Lanjutan

Konstanta Pemerisaian (1)
nOrbitalσ
1s0
Detail Jari-jari Kristal (2)
MuatanCNSpinrcrystal (pm)Asal
1I-24
1II-4
Mode Peluruhan Isotop (6)
IsotopModeIntensitas
3B-100%
4n100%
52n100%
6n—
63n—
72n—
Faktor Hamburan Sinar-X (501)
Energi (eV)f₁f₂
10—0
10,1617—0
10,3261—0
10,4931—0
10,6628—0
10,8353—0
11,0106—0
11,1886—0
11,3696—0
11,5535—0

Data Tambahan

Sources

Sources of this element.

Hydrogen is estimated to make up more than 90% of all the atoms three quarters of the mass of the universe! This element is found in the stars, and plays an important part in powering the universe through both the proton-proton reaction and carbon-nitrogen cycle. Stellar hydrogen fusion processes release massive amounts of energy by combining hydrogens to form helium.

Production of hydrogen in the U.S. alone amounts to about 3 billion cubic feet per year. Hydrogen is prepared by

▸ steam on heated carbon,

▸ decomposition of certain hydrocarbons with heat,

▸ reaction of sodium or potassium hydroxide on aluminum

▸ electrolysis of water, or

▸ displacement from acids by certain metals.

Liquid hydrogen is important in cryogenics and in the study of superconductivity, as its melting point is only 20 degrees above absolute zero.

Tritium is readily produced in nuclear reactors and is used in the production of the hydrogen bomb.

Hydrogen is the primary component of Jupiter and the other gas giant planets. At some depth in the planet's interior the pressure is so great that solid molecular hydrogen is converted to solid metallic hydrogen.

In 1973, a group of Russian experimenters may have produced metallic hydrogen at a pressure of 2.8 Mbar. At the transition the density changed from 1.08 to 1.3 g/cm3. Earlier, in 1972, at Livermore, California, a group also reported on a similar experiment in which they observed a pressure-volume point centered at 2 Mbar. Predictions say that metallic hydrogen may be metastable; others have predicted it would be a superconductor at room temperature.

Referensi (1)

Isotopes in Forensic Science and Anthropology

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

Measurements of relative 2H abundances are used to determine the breeding grounds of many species of migrant songbirds. These species of songbirds only grow their feathers before migration, and they grow them on or close to their breeding grounds. Therefore, the isotopic composition of a bird’s feathers correlates to the isotopic composition of the growing season’s precipitation [18] Z. D. Sharp, V. Atudorei, H. O. Panarello, J. Fernández, C. Douthitt. J. Archaeolog. Sci.30, 1709 (2003)., [19] K. A. Hobson. Oecologia120, 314 (1999)., [20] K. A. Hobson, L. I. Wassenaar. Oecologia.109, 142 (1996)..

Measurements of relative 2H abundances of human hair samples collected at archeological sites are used to determine the geographic region in which a subject lived based on the hydrogen isotopic composition of the water they drank. This is possible because hair stores a daily record of the hydrogen isotopic composition of intake water, which correlates to local meteoric water [18] Z. D. Sharp, V. Atudorei, H. O. Panarello, J. Fernández, C. Douthitt. J. Archaeolog. Sci.30, 1709 (2003)., [21] T. B. Coplen, H. Qi. Forensic Sci. Int.266, 222 (2016)..

Referensi (5)
  • [18] Z. D. Sharp, V. Atudorei, H. O. Panarello, J. Fernández, C. Douthitt. J. Archaeolog. Sci.30, 1709 (2003).
  • [19] K. A. Hobson. Oecologia120, 314 (1999).
  • [20] K. A. Hobson, L. I. Wassenaar. Oecologia.109, 142 (1996).
  • [21] T. B. Coplen, H. Qi. Forensic Sci. Int.266, 222 (2016).
  • [4] IUPAC Periodic Table of the Elements and Isotopes (IPTEI) https://doi.org/10.1515/pac-2015-0703

Referensi

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

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)
Hydrogen

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.

Catatan lisensi: 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
Hydrogen

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/

Catatan lisensi: Please see citation and linking information: https://education.jlab.org/faq/index.html
6 Los Alamos National Laboratory, U.S. Department of Energy
Hydrogen

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
Hydrogen

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
Hydrogen

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

9 PubChem Elements
Hydrogen

The element property data was retrieved from publications.

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