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Al 13

Aluminum (Al)

post-transition-metal
Periode: 3 Golongan: 13 Blok: p

Solid

Bobot Atom Standar

26,981538 u

Konfigurasi elektron

[Ne] 3s2 3p1

Titik lebur

660,287 °C

Titik didih

2518,85 °C

Massa jenis

2700 kg/m³

Bilangan oksidasi

−2, −1, 0, +1, +2, +3

Keelektronegatifan (Pauling)

1,61

Energi ionisasi (ke-1)

5,985769 eV

Tahun penemuan

1825

Jari-jari atom

125 pm

Detail

Asal nama Latin: alumen, aluminis, (alum).
Negara penemuan Denmark
Penemu Hans Christian Oersted

Aluminum is a light, silvery post-transition metal and the most abundant metal in Earth’s crust. It is highly reactive thermodynamically, but a thin, adherent oxide film protects the metal from rapid corrosion in air and water. Its low density, electrical conductivity, formability, and alloying behavior make it one of the major structural and engineering metals.

Pure aluminum, a silvery-white metal, possesses many desirable characteristics. It is light, it is nonmagnetic and nonsparking, stands second among metals in the scale of malleability, and sixth in ductility.

The name derives from the Latin, alum and alumen for "stringent" because the early Romans called any substance with a stringent taste alum. The element was known in prehistoric times. In 1825, the Danish physicist, Hans Christian Oersted, isolated impure aluminium. The pure metal was first isolated by the German chemist Friedrich Wöhler in 1827.

Although aluminum is the most abundant metal in the earth's crust, it is never found free in nature. All of the earth's aluminum has combined with other elements to form compounds. Two of the most common compounds are alum, such as potassium aluminum sulfate (KAl(SO4)2·12H2O), and aluminum oxide (Al2O3). About 8.2% of the earth's crust is composed of aluminum. Scientists suspected than an unknown metal existed in alum as early as 1787, but they did not have a way to extract it until 1825. Hans Christian Oersted, a Danish chemist, was the first to produce tiny amounts of aluminum. Two years later, Friedrich Wöhler, a German chemist, developed a different way to obtain aluminum. By 1845, he was able to produce samples large enough to determine some of aluminum's basic properties. Wöhler's method was improved in 1854 by Henri Étienne Sainte-Claire Deville, a French chemist. Deville's process allowed for the commercial production of aluminum. As a result, the price of aluminum dropped from around $1200 per kilogram in 1852 to around $40 per kilogram in 1859. Unfortunately, aluminum remained too expensive to be widely used.

From the Latin word alumen, alum. The ancient Greeks and Romans used alum as an astringent and as a mordant in dyeing. In 1761 de Morveau proposed the name alumine for the base in alum, and Lavoisier, in 1787, thought this to be the oxide of a still undiscovered metal.

Friedrich Wohler is generally credited with having isolated the metal in 1827, although an impure form was prepared by Oersted two years earlier. In 1807, Davy proposed the name aluminium for the metal, undiscovered at that time, and later agreed to change it to aluminum. Shortly thereafter, the name aluminum was adopted to conform with the "ium" ending of most elements.

Aluminium was also the accepted spelling in the U.S. until 1925, at which time the American Chemical Society decided to use the name aluminum thereafter in their publications. See the Wikipedia entry on Aluminium for additional discussion on the spelling of this element.

Gambar

Sifat

Fisika

Jari-jari atom (empiris)
125 pm Bandingkan Jari-jari atom (empiris) semua unsur →
Jari-jari kovalen
121 pm Bandingkan Jari-jari kovalen semua unsur →
Jari-jari van der Waals
184 pm Bandingkan Jari-jari van der Waals semua unsur →
Jari-jari logam
125 pm Bandingkan Jari-jari logam semua unsur →
Massa jenis
2700 kg/m³ Bandingkan Massa jenis semua unsur →
Volume molar
0,01 L/mol
Fase pada STP
Padat Bandingkan Fase pada STP semua unsur →
Titik lebur
660,287 °C Bandingkan Titik lebur semua unsur →
Titik didih
2518,85 °C Bandingkan Titik didih semua unsur →
Konduktivitas termal
237 W/(m·K) Bandingkan Konduktivitas termal semua unsur →
Kapasitas kalor spesifik
0,897 J/(g·K) Bandingkan Kapasitas kalor spesifik semua unsur →
Kapasitas kalor molar
24,2 J/(mol·K) Bandingkan Kapasitas kalor molar semua unsur →
Struktur kristal
Kubik berpusat muka Bandingkan Struktur kristal semua unsur →

Kimia

Keelektronegatifan (Pauling)
1,61 Bandingkan Keelektronegatifan (Pauling) semua unsur →
Keelektronegatifan (Allen)
1,613
Afinitas elektron
0,4328 eV
Energi ionisasi (ke-1)
5,985769 eV Bandingkan Energi ionisasi (ke-1) semua unsur →
Energi ionisasi (ke-2)
18,828615 eV Bandingkan Energi ionisasi (ke-2) semua unsur →
Energi ionisasi (ke-3)
28,44774 eV Bandingkan Energi ionisasi (ke-3) semua unsur →
Energi ionisasi (ke-4)
119,992813 eV Bandingkan Energi ionisasi (ke-4) semua unsur →
Energi ionisasi (ke-5)
153,825729 eV Bandingkan Energi ionisasi (ke-5) semua unsur →
Bilangan oksidasi
−2, −1, 0, +1, +2, +3 Bandingkan Bilangan oksidasi semua unsur →
Elektron valensi
3 Bandingkan Elektron valensi semua unsur →
Konfigurasi elektron
[Ne] 3s2 3p1

Termodinamika

Titik kritis (suhu)
6427 °C
Kalor peleburan
0,11100171 eV Bandingkan Kalor peleburan semua unsur →
Kalor penguapan
3,047106 eV Bandingkan Kalor penguapan semua unsur →
Kalor sublimasi
3,382909 eV
Kalor atomisasi
3,382909 eV
Entalpi atomisasi
3,429549 eV

Nuklir

Proton
13 Bandingkan Proton semua unsur →
Neutron
14 Bandingkan Neutron semua unsur →
Isotop yang diketahui
23 Bandingkan Isotop yang diketahui semua unsur →
Isotop stabil
1 Bandingkan Isotop stabil semua unsur →
Isotop paling stabil
Al-27
Tahun penemuan
1825

Kelimpahan

Kelimpahan (kerak Bumi)
8,23e+4 mg/kg Bandingkan Kelimpahan (kerak Bumi) semua unsur →
Kelimpahan (samudra)
0,002 mg/L Bandingkan Kelimpahan (samudra) semua unsur →

Struktur Kristal

Konstanta kisi a
405 pm

Struktur Elektronik

Elektron per kulit
2, 8, 3 Bandingkan Elektron per kulit semua unsur →

Pengenal

Nomor CAS
7429-90-5 Bandingkan Nomor CAS semua unsur →
Simbol term
2P°1/2
InChI
InChI=1S/Al
Kunci InChI
XAGFODPZIPBFFR-UHFFFAOYSA-N

Konfigurasi Elektron Diukur

Muatan ion
Proton 13
Elektron 13
Muatan Netral
Konfigurasi Al: 3s² 3p¹
Konfigurasi elektron
Diukur
[Ne] 3s² 3p¹
1s² 2s² 2p⁶ 3s² 3p¹
Diagram orbital
1s
2/2
2s
2/2
2p
6/6
3s
2/2
3p
1/6 1↑
Total elektron: 13 Tidak berpasangan: 1 ?

Model atom

Proton 13
Neutron 14
Elektron 13
Nomor massa 27
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 / 50 (50 50 dengan intensitas)
Diukur
Emisi Tampak: 380–750 nm

Distribusi Isotop

Unsur monoisotopik
Satu-satunya isotop yang terdapat di alam: 27 — 100,0000%
27100,0000%Nomor massaKelimpahan alami (%)
Nomor massaMassa atom (u)Kelimpahan alamiWaktu paruh
27 Stabil26,98153853 ± 0,00000011100,0000%Stabil
Diukur

Fase / Wujud

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

Alasan: 635,3 °C di bawah titik lebur (660,287 °C)

Titik lebur 660,287 °C
Titik didih 2518,85 °C
Di bawah titik lebur sebesar 635,3 °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
660,287 °C
Titik didih Literatur
2518,85 °C
Fase saat ini Dihitung
Padat

Energi transisi

Kalor peleburan Literatur
0,11100171 eV

Energi yang diperlukan untuk meleburkan 1 mol pada titik lebur

Kalor penguapan Literatur
3,047106 eV

Energi yang diperlukan untuk menguapkan 1 mol pada titik didih

Kalor sublimasi Literatur
3,382909 eV

Energi yang diperlukan untuk menyublimkan 1 mol pada titik sublimasi

Massa jenis

Massa jenis referensi Literatur
2700 kg/m³

Pada kondisi standar

Massa jenis saat ini Dihitung
2700 kg/m³

Pada kondisi standar

Lanjutan

Titik kritis Literatur
6427 °C

Spektrum Atom

Menampilkan 10 dari 13. Diurutkan berdasarkan muatan ion (menaik).

Data Garis Spektrum ?

IonMuatanTotal garisProbabilitas transisiPenamaan tingkat energi
Al I 0589322560
Al II +114299861429
Al III +2344259344
Al IV +3409123409
Al V +4600444600
Al VI +5515491515
Al VII +6350339350
Al VIII +7440418438
Al IX +8372339372
Al X +9189169189
Data Garis Spektrum NIST →

Data Tingkat Energi ?

IonMuatanTingkat energi
Al I 0192
Al II +1219
Al III +284
Al IV +3121
Al V +4158
Al VI +587
Al VII +673
Al VIII +795
Al IX +869
Al X +961
Data Tingkat Energi NIST →
13 Al 26.9815385

Aluminum — Visualisasi Orbital Atom

[Ne]3s23p1
Tingkat energi 2 8 3
Bilangan oksidasi -2, -1, 0, +1, +2, +3
HOMO 3p n=3 · l=1 · m=-1
Aluminum — Pratinjau Visualisasi Orbital Atom
Three.js hanya dimuat saat diminta
13 Al 26.9815385

Aluminum — Visualisasi Struktur Kristal

Face-Centered Cubic · Pearson cF4
Eksperimental
Pearson cF4
No. Koord. 12
Pengemasan 74.000%
Aluminum — Pratinjau Visualisasi Struktur Kristal
Three.js hanya dimuat saat diminta

Jari-jari Ion

MuatanKoordinasiSpinJari-jari
+34Tidak tersedia39 pm
+35Tidak tersedia48 pm
+36Tidak tersedia53.5 pm

Senyawa

Al
26,982 u
Al+3
26,982 u
Al
25,987 u
Al
28,980 u
Al
26,982 u
Al
27,982 u
Al+3
26,982 u

Isotop (1)

Nomor massaMassa atom (u)Kelimpahan alamiWaktu paruhMode peluruhan
27 Stabil26,98153853 ± 0,00000011100,0000%Stabil
stable
27 Stabil
Massa atom (u) 26,98153853 ± 0,00000011
Kelimpahan alami 100,0000%
Waktu paruh Stabil
Mode peluruhan
stable

Garis Spektrum

Menampilkan 50 dari 341. Secara bawaan, hanya garis spektrum dengan intensitas terukur yang ditampilkan.

Panjang gelombang (nm)IntensitasTahap ionisasiJenisTransisiAkurasiSumber
466.3046 nm1000Al IIemission3p2 1D → 3s.4p 1P*DiukurNIST
559.33 nm800Al IIemission3s.4p 1P* → 3s.4d 1DDiukurNIST
458.5818 nm500Al IIemission3s.4d 3D → 3s.7f 3F*DiukurNIST
458.8199 nm400Al IIemission3s.4d 3D → 3s.7f 3F*DiukurNIST
464.8609 nm400Al IIemission3s.4d 1D → 3s.10p 1P*DiukurNIST
466.6799 nm400Al IIemission3s.5p 1P* → 3s.11s 1SDiukurNIST
458.975 nm300Al IIemission3s.4d 3D → 3s.7f 3F*DiukurNIST
444.7805 nm200Al IIemission3s.4d 1D → 3s.11p 1P*DiukurNIST
458.968 nm200Al IIemission3s.4d 3D → 3s.7f 3F*DiukurNIST
600.641 nm200Al IIemission3s.5p 3P* → 3s.7d 3DDiukurNIST
390.0675 nm100Al IIemission3s.3p 1P* → 3p2 1DDiukurNIST
528.3733 nm100Al IIemission3s.5p 3P* → 3s.8d 3DDiukurNIST
561.329 nm100Al IIemission3s.4d 1D → 3s.7f 1F*DiukurNIST
585.376 nm100Al IIemission3s.4d 3D → 3s.6f 3F*DiukurNIST
624.337 nm100Al IIemission3s.4p 3P* → 3s.4d 3DDiukurNIST
704.208 nm100Al IIemission3s.4s 3S → 3s.4p 3P*DiukurNIST
747.141 nm90Al IIemission3s.3d 1D → 3s.4f 1F*DiukurNIST
586.177 nm80Al IIemission3s.4d 3D → 3s.6f 3F*DiukurNIST
597.197 nm80Al IIemission3s.5p 1P* → 3s.7d 1DDiukurNIST
683.713 nm80Al IIemission3s.4p 3P* → 3s.5s 3SDiukurNIST
623.175 nm75Al IIemission3s.4p 3P* → 3s.4d 3DDiukurNIST
600.187 nm60Al IIemission3s.5p 3P* → 3s.7d 3DDiukurNIST
422.6816 nm50Al IIemission3s.4d 3D → 3s.8f 3F*DiukurNIST
422.7495 nm50Al IIemission3s.4d 3D → 3s.8f 3F*DiukurNIST
422.7987 nm50Al IIemission3s.4d 3D → 3s.8f 3F*DiukurNIST
586.79 nm50Al IIemission3s.4d 3D → 3s.6f 3F*DiukurNIST
607.32 nm50Al IIemission3s.5p 3P* → 3s.8s 3SDiukurNIST
622.619 nm50Al IIemission3s.4p 3P* → 3s.4d 3DDiukurNIST
682.339 nm50Al IIemission3s.4p 3P* → 3s.5s 3SDiukurNIST
705.671 nm50Al IIemission3s.4s 3S → 3s.4p 3P*DiukurNIST
744.944 nm50Al IIemission3s.5p 1P* → 3s.6d 1DDiukurNIST
399.5837 nm40Al IIemission3s.4d 3D → 3s.9f 3F*DiukurNIST
450.371 nm40Al IVemission2s2.2p5.(2P*<3/2>).4s 2[3/2]* → 2s2.2p5.(2P*<3/2>).4p 2[5/2]DiukurNIST
600.192 nm40Al IIemission3s.5p 3P* → 3s.7d 3DDiukurNIST
399.6141 nm30Al IIemission3s.4d 3D → 3s.9f 3F*DiukurNIST
450.237 nm30Al IVemission2s2.2p5.(2P*<1/2>).4s 2[1/2]* → 2s2.2p5.(2P*<1/2>).4p 2[3/2]DiukurNIST
463.576 nm30Al IIemission3s.5p 3P* → 3s.10d 3DDiukurNIST
528.5838 nm30Al IIemission3s.5p 1P* → 3s.8d 1DDiukurNIST
606.112 nm30Al IIemission3s.5p 1P* → 3s.8s 1SDiukurNIST
633.571 nm30Al IIemission3s.3d 1D → 3s.5p 1P*DiukurNIST
399.6368 nm20Al IIemission3s.4d 3D → 3s.9f 3F*DiukurNIST
402.6318 nm20Al IIemission3s.3d 1D → 3s.6p 1P*DiukurNIST
446.894 nm20Al IVemission2s2.2p5.(2P*<3/2>).4s 2[3/2]* → 2s2.2p5.(2P*<3/2>).4p 2[3/2]DiukurNIST
569.66 nm17Al IIIemission2p6.4s 2S → 2p6.4p 2P*DiukurNIST
572.273 nm16Al IIIemission2p6.4s 2S → 2p6.4p 2P*DiukurNIST
462.038 nm15Al IVemission2s2.2p5.(2P*<3/2>).4s 2[3/2]* → 2s2.2p5.(2P*<3/2>).4p 2[5/2]DiukurNIST
531.6073 nm15Al IIemission3s.5p 3P* → 3s.9s 3SDiukurNIST
452.919 nm14Al IIIemission2p6.4p 2P* → 2p6.4d 2DDiukurNIST
451.257 nm13Al IIIemission2p6.4p 2P* → 2p6.4d 2DDiukurNIST
669.6018 nm13Al Iemission3s2.4s 2S → 3s2.5p 2P*DiukurNIST

Sifat Lanjutan

Jari-jari Kovalen (Lanjutan)

Jari-jari kovalen (Pyykkö)
126 pm
Jari-jari kovalen (Pyykkö, ikatan rangkap dua)
113 pm
Jari-jari kovalen (Pyykkö, ikatan rangkap tiga)
111 pm
Jari-jari kovalen (Bragg)
135 pm

Jari-jari van der Waals

Truhlar
184 pm
Batsanov
210 pm
Alvarez
225 pm
UFF
449,9 pm
MM3
236 pm
Dreiding
439 pm

Jari-jari Atom & Logam

Jari-jari atom (Rahm)
239 pm
Jari-jari logam (C12)
143 pm

Skala Penomoran

Mendeleev
82
Pettifor
80
Glawe
78

Skala Keelektronegatifan

Ghosh
0
Miedema
4
Gunnarsson–Lundqvist
3
Robles–Bartolotti
3

Polarizabilitas & Dispersi

Polarizabilitas dipol
57,8 a.u.
Polarizabilitas dipol (ketidakpastian)
1 a.u.
C₆
528 Ha·Bohr6
C₆ (Gould–Bučko)
520 Ha·Bohr6

Parameter Miedema

Volume molar Miedema
10 cm3/mol
Kerapatan elektron Miedema
3

Risiko Pasokan & Ekonomi

Konsentrasi produksi
31
Risiko pasokan relatif
5
Distribusi cadangan
26
Stabilitas politik (produsen terbesar)
75
Stabilitas politik (pemilik cadangan terbesar)
5

Transisi Fase & Alotrop

Titik lebur933,47 K
Titik didih2792,15 K
Titik kritis (suhu)6700,15 K

Kategori Bilangan Oksidasi

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

Data Referensi Lanjutan

Konstanta Pemerisaian (5)
nOrbitalσ
1s0,409
2p4,0366
2s4,7864
3p8,9344
3s8,8828
Detail Jari-jari Kristal (3)
MuatanCNSpinrcrystal (pm)Asal
3IV53
3V62
3VI67,5from r^3 vs V plots,
Mode Peluruhan Isotop (51)
IsotopModeIntensitas
21p—
22B+100%
22B+p55%
222p1,1%
22B+A0%
23B+100%
23B+p1,2%
24B+100%
24B+A0%
24B+p0%
Faktor Hamburan Sinar-X (504)
Energi (eV)f₁f₂
10—3,1199
10,1617—3,05822
10,3261—2,99776
10,4931—2,9385
10,6628—2,88041
10,8353—2,82347
11,0106—2,76766
11,1886—2,722
11,3696—2,69148
11,5535—2,66129

Data Tambahan

Sources

Sources of this element.

The method of obtaining aluminum metal by the electrolysis of alumina dissolved in cryolite was discovered in 1886 by Hall in the U.S. and at about the same time by Heroult in France. Cryolite, a natural ore found in Greenland, is no longer widely used in commercial production, but has been replaced by an artificial mixture of sodium, aluminum, and calcium fluorides.

Aluminum can now be produced from clay, but the process is not economically feasible at present. Aluminum is the most abundant metal to be found in the earth's crust (8.1%), but is never found free in nature. In addition to the minerals mentioned above, it is also found in granite and in many other common minerals.

Referensi (1)

Referensi

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

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)
Aluminium

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
Aluminum

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
Aluminum

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
Aluminum

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
Aluminum

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

9 PubChem Elements
Aluminum

The element property data was retrieved from publications.

Terakhir diperbarui:

Data terverifikasi:

Konten ditinjau berdasarkan data ilmiah terbaru.