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Ti 22

Titanium (Ti)

transition-metal
Periode: 4 Golongan: 4 Blok: d

Solid

Bobot Atom Standar

47,867 u

Konfigurasi elektron

[Ar] 4s2 3d2

Titik lebur

1667,85 °C

Titik didih

3286,85 °C

Massa jenis

4500 kg/m³

Bilangan oksidasi

−2, −1, 0, +1, +2, +3, +4

Keelektronegatifan (Pauling)

1,54

Energi ionisasi (ke-1)

6,82812 eV

Tahun penemuan

1791

Jari-jari atom

140 pm

Detail

Asal nama Greek: titanos (Titans).
Negara penemuan England
Penemu William Gregor

Titanium is a light, strong transition metal with a high melting point and exceptional resistance to corrosion in many natural and industrial environments. Its chemistry is dominated by the +4 oxidation state, although +3 and lower states occur in specialized compounds. The metal is abundant in Earth’s crust but is rarely found in concentrated metallic form because it bonds strongly to oxygen and nitrogen. Its combination of low density, strength, and passivation makes it important in aerospace, chemical equipment, pigments, and medical materials.

Titanium, when pure, is a lustrous, white metal. It has a low density, good strength, is easily fabricated, and has excellent corrosion resistance. It is ductile only when it is free of oxygen. The metal, which burns in air, is the only element that burns in nitrogen.

Titanium is resistant to dilute sulfuric and hydrochloric acid, most organic acids, most chlorine gas, and chloride solutions.

Natural titanium is reported to become very radioactive after bombardment with deuterons. The emitted radiations are mostly positrons and hard gamma rays. The metal is dimorphic. The hexagonal alpha form changes to the cubic beta form very slowly at about 880°C. The metal combines with oxygen at red heat, and with chlorine at 550°C.

Titanium metal is considered to be physiologically inert. When pure, titanium dioxide is relatively clear and has an extremely high index of refraction with an optical dispersion higher than diamond.

The name derives from the Latin titans, who were the mythological "first sons of the earth". It was originally discovered by the English clergyman William Gregor in the mineral ilmenite (FeTiO3) in 1791. He called this mineral menachanite and the element menachin, for the Menachan parish where it was found. It was rediscovered in 1795 by the German chemist Martin Heinrich Klaproth, who called it titanium because it had no characteristic properties to use as a name. Titanium metal was first isolated by the Swedish chemists Sven Otto Pettersson and Lars Fredrik Nilson.

Titanium was discovered in 1791 by the Reverend William Gregor, an English pastor. Pure titanium was first produced by Matthew A. Hunter, an American metallurgist, in 1910. Titanium is the ninth most abundant element in the earth's crust and is primarily found in the minerals rutile (TiO2), ilmenite (FeTiO3) and sphene (CaTiSiO5). Titanium makes up about 0.57% of the earth's crust.

From the Latin titans, the first sons of the Earth, Greek mythology.

Discovered by Gregor in 1791; named by Klaproth in 1795. Impure titanium was prepared by Nilson and Pettersson in 1887; however, the pure metal (99.9%) was not made until 1910 when Hunter heated TiCl4 with sodium in a steel bomb.

Gambar

Sifat

Fisika

Jari-jari atom (empiris)
140 pm Bandingkan Jari-jari atom (empiris) semua unsur →
Jari-jari kovalen
160 pm Bandingkan Jari-jari kovalen semua unsur →
Jari-jari van der Waals
187 pm Bandingkan Jari-jari van der Waals semua unsur →
Jari-jari logam
132 pm Bandingkan Jari-jari logam semua unsur →
Massa jenis
4500 kg/m³ Bandingkan Massa jenis semua unsur →
Volume molar
0,0106 L/mol
Fase pada STP
Padat Bandingkan Fase pada STP semua unsur →
Titik lebur
1667,85 °C Bandingkan Titik lebur semua unsur →
Titik didih
3286,85 °C Bandingkan Titik didih semua unsur →
Konduktivitas termal
21,9 W/(m·K) Bandingkan Konduktivitas termal semua unsur →
Kapasitas kalor spesifik
0,523 J/(g·K) Bandingkan Kapasitas kalor spesifik semua unsur →
Kapasitas kalor molar
25,06 J/(mol·K) Bandingkan Kapasitas kalor molar semua unsur →
Struktur kristal
Heksagonal susunan rapat Bandingkan Struktur kristal semua unsur →

Kimia

Keelektronegatifan (Pauling)
1,54 Bandingkan Keelektronegatifan (Pauling) semua unsur →
Keelektronegatifan (Allen)
1,38
Afinitas elektron
0,0755 eV
Energi ionisasi (ke-1)
6,82812 eV Bandingkan Energi ionisasi (ke-1) semua unsur →
Energi ionisasi (ke-2)
13,575547 eV Bandingkan Energi ionisasi (ke-2) semua unsur →
Energi ionisasi (ke-3)
27,491805 eV Bandingkan Energi ionisasi (ke-3) semua unsur →
Energi ionisasi (ke-4)
43,267319 eV Bandingkan Energi ionisasi (ke-4) semua unsur →
Energi ionisasi (ke-5)
99,299342 eV Bandingkan Energi ionisasi (ke-5) semua unsur →
Bilangan oksidasi
−2, −1, 0, +1, +2, +3, +4 Bandingkan Bilangan oksidasi semua unsur →
Elektron valensi
4 Bandingkan Elektron valensi semua unsur →
Konfigurasi elektron
[Ar] 4s2 3d2

Termodinamika

Kalor peleburan
0,14665492 eV Bandingkan Kalor peleburan semua unsur →
Kalor penguapan
4,40483 eV Bandingkan Kalor penguapan semua unsur →
Kalor sublimasi
4,851531 eV
Kalor atomisasi
4,851531 eV
Entalpi atomisasi
4,902316 eV

Nuklir

Proton
22 Bandingkan Proton semua unsur →
Neutron
26 Bandingkan Neutron semua unsur →
Isotop yang diketahui
29 Bandingkan Isotop yang diketahui semua unsur →
Isotop stabil
5 Bandingkan Isotop stabil semua unsur →
Isotop paling stabil
Ti-48
Tahun penemuan
1791

Kelimpahan

Kelimpahan (kerak Bumi)
5650 mg/kg Bandingkan Kelimpahan (kerak Bumi) semua unsur →
Kelimpahan (samudra)
0,001 mg/L Bandingkan Kelimpahan (samudra) semua unsur →

Struktur Kristal

Konstanta kisi a
295 pm

Struktur Elektronik

Elektron per kulit
2, 8, 10, 2 Bandingkan Elektron per kulit semua unsur →

Pengenal

Nomor CAS
7440-32-6 Bandingkan Nomor CAS semua unsur →
Simbol term
3F2
InChI
InChI=1S/Ti
Kunci InChI
RTAQQCXQSZGOHL-UHFFFAOYSA-N

Konfigurasi Elektron Diukur

Muatan ion
Proton 22
Elektron 22
Muatan Netral
Konfigurasi Ti: 3d² 4s²
Konfigurasi elektron
Diukur
[Ar] 3d² 4s²
1s² 2s² 2p⁶ 3s² 3p⁶ 3d² 4s²
Diagram orbital
1s
2/2
2s
2/2
2p
6/6
3s
2/2
3p
6/6
4s
2/2
3d
2/10 2↑
Total elektron: 22 Tidak berpasangan: 2 ?

Model atom

Proton 22
Neutron 26
Elektron 22
Nomor massa 48
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

4873,7200%468,2500%477,4400%495,4100%505,1800%Nomor massaKelimpahan alami (%)
Nomor massaMassa atom (u)Kelimpahan alamiWaktu paruh
46 Stabil45,95262772 ± 0,000000358,2500%Stabil
47 Stabil46,95175879 ± 0,000000387,4400%Stabil
48 Stabil47,94794198 ± 0,0000003873,7200%Stabil
49 Stabil48,94786568 ± 0,000000395,4100%Stabil
50 Stabil49,94478689 ± 0,000000395,1800%Stabil
Diukur

Fase / Wujud

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

Alasan: 1642,8 °C di bawah titik lebur (1667,85 °C)

Titik lebur 1667,85 °C
Titik didih 3286,85 °C
Di bawah titik lebur sebesar 1642,8 °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
1667,85 °C
Titik didih Literatur
3286,85 °C
Fase saat ini Dihitung
Padat

Energi transisi

Kalor peleburan Literatur
0,14665492 eV

Energi yang diperlukan untuk meleburkan 1 mol pada titik lebur

Kalor penguapan Literatur
4,40483 eV

Energi yang diperlukan untuk menguapkan 1 mol pada titik didih

Kalor sublimasi Literatur
4,851531 eV

Energi yang diperlukan untuk menyublimkan 1 mol pada titik sublimasi

Massa jenis

Massa jenis referensi Literatur
4500 kg/m³

Pada kondisi standar

Massa jenis saat ini Dihitung
4500 kg/m³

Pada kondisi standar

Spektrum Atom

Menampilkan 10 dari 22. Diurutkan berdasarkan muatan ion (menaik).

Data Garis Spektrum ?

IonMuatanTotal garisProbabilitas transisiPenamaan tingkat energi
Ti I 040294964029
Ti II +118724701872
Ti III +2819297819
Ti IV +3863986
Ti V +42524252
Ti VI +5711471
Ti VII +6921392
Ti VIII +7853785
Ti IX +8855085
Ti X +916278162
Data Garis Spektrum NIST →

Data Tingkat Energi ?

IonMuatanTingkat energi
Ti I 0559
Ti II +1253
Ti III +2200
Ti IV +340
Ti V +466
Ti VI +559
Ti VII +662
Ti VIII +744
Ti IX +832
Ti X +983
Data Tingkat Energi NIST →
22 Ti 47.867

Titanium — Visualisasi Orbital Atom

[Ar]4s23d2
Tingkat energi 2 8 10 2
Bilangan oksidasi -2, -1, 0, +1, +2, +3, +4
HOMO 3d n=3 · l=2 · m=-2
Titanium — Pratinjau Visualisasi Orbital Atom
Three.js hanya dimuat saat diminta
22 Ti 47.867

Titanium — Visualisasi Struktur Kristal

Heksagonal Primitif · Pearson hP2
Eksperimental
Pearson hP2
No. Koord. 12
Pengemasan 74.048%
Titanium — Pratinjau Visualisasi Struktur Kristal
Three.js hanya dimuat saat diminta

Jari-jari Ion

MuatanKoordinasiSpinJari-jari
+26Tidak tersedia86 pm
+36Tidak tersedia67 pm
+44Tidak tersedia42 pm
+45Tidak tersedia51 pm
+46Tidak tersedia60.5 pm
+48Tidak tersedia74 pm

Senyawa

Ti
47,867 u
Ti+4
47,867 u
Ti
44,958 u
Ti
43,960 u
Ti+2
47,867 u
Ti+3
47,867 u
Ti
46,952 u
Ti
50,947 u
Ti
51,947 u
Ti
45,953 u
Ti
47,948 u
Ti
48,948 u
Ti
49,945 u

Isotop (5)

Natural titanium consists of five isotopes with atomic masses from 46 to 50. All are stable. Eight other unstable isotopes are known.

Nomor massaMassa atom (u)Kelimpahan alamiWaktu paruhMode peluruhan
46 Stabil45,95262772 ± 0,000000358,2500% ± 0,0300%Stabil
stable
47 Stabil46,95175879 ± 0,000000387,4400% ± 0,0200%Stabil
stable
48 Stabil47,94794198 ± 0,0000003873,7200% ± 0,0300%Stabil
stable
49 Stabil48,94786568 ± 0,000000395,4100% ± 0,0200%Stabil
stable
50 Stabil49,94478689 ± 0,000000395,1800% ± 0,0200%Stabil
stable
46 Stabil
Massa atom (u) 45,95262772 ± 0,00000035
Kelimpahan alami 8,2500% ± 0,0300%
Waktu paruh Stabil
Mode peluruhan
stable
47 Stabil
Massa atom (u) 46,95175879 ± 0,00000038
Kelimpahan alami 7,4400% ± 0,0200%
Waktu paruh Stabil
Mode peluruhan
stable
48 Stabil
Massa atom (u) 47,94794198 ± 0,00000038
Kelimpahan alami 73,7200% ± 0,0300%
Waktu paruh Stabil
Mode peluruhan
stable
49 Stabil
Massa atom (u) 48,94786568 ± 0,00000039
Kelimpahan alami 5,4100% ± 0,0200%
Waktu paruh Stabil
Mode peluruhan
stable
50 Stabil
Massa atom (u) 49,94478689 ± 0,00000039
Kelimpahan alami 5,1800% ± 0,0200%
Waktu paruh Stabil
Mode peluruhan
stable

Garis Spektrum

Menampilkan 50 dari 1717. Secara bawaan, hanya garis spektrum dengan intensitas terukur yang ditampilkan.

Panjang gelombang (nm)IntensitasTahap ionisasiJenisTransisiAkurasiSumber
521.03843 nm21000Ti Iemission3d2.4s2 a 3F → 3d2.(3F).4s.4p.(3P*) z 3F*DiukurNIST
506.46526 nm17000Ti Iemission3d2.4s2 a 3F → 3d2.(3F).4s.4p.(3P*) z 3D*DiukurNIST
519.29686 nm17000Ti Iemission3d2.4s2 a 3F → 3d2.(3F).4s.4p.(3P*) z 3F*DiukurNIST
517.37431 nm15000Ti Iemission3d2.4s2 a 3F → 3d2.(3F).4s.4p.(3P*) z 3F*DiukurNIST
498.17305 nm14000Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5G*DiukurNIST
503.99574 nm14000Ti Iemission3d2.4s2 a 3F → 3d2.(3F).4s.4p.(3P*) z 3D*DiukurNIST
468.19089 nm13000Ti Iemission3d2.4s2 a 3F → 3d2.(3F).4s.4p.(3P*) z 3G*DiukurNIST
499.1066 nm13000Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5G*DiukurNIST
499.9503 nm12000Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5G*DiukurNIST
501.41861 nm11000Ti Iemission3d2.4s2 a 3F → 3d2.(3F).4s.4p.(3P*) z 3D*DiukurNIST
399.86363 nm10000Ti Iemission3d2.4s2 a 3F → 3d2.(3F).4s.4p.(1P*) y 3F*DiukurNIST
466.75845 nm10000Ti Iemission3d2.4s2 a 3F → 3d2.(3F).4s.4p.(3P*) z 3G*DiukurNIST
500.72093 nm10000Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5G*DiukurNIST
453.32394 nm9200Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5F*DiukurNIST
398.17616 nm8800Ti Iemission3d2.4s2 a 3F → 3d2.(3F).4s.4p.(1P*) y 3F*DiukurNIST
398.97582 nm8800Ti Iemission3d2.4s2 a 3F → 3d2.(3F).4s.4p.(1P*) y 3F*DiukurNIST
501.42762 nm8700Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5G*DiukurNIST
395.82055 nm8600Ti Iemission3d2.4s2 a 3F → 3d3.(4F).4p y 3D*DiukurNIST
465.64693 nm8400Ti Iemission3d2.4s2 a 3F → 3d2.(3F).4s.4p.(3P*) z 3G*DiukurNIST
395.63338 nm8000Ti Iemission3d2.4s2 a 3F → 3d3.(4F).4p y 3D*DiukurNIST
453.47761 nm7900Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5F*DiukurNIST
394.86705 nm7000Ti Iemission3d2.4s2 a 3F → 3d3.(4F).4p y 3D*DiukurNIST
484.08737 nm6600Ti Iemission3d2.4s2 a 1D → 3d2.(1D).4s.4p.(1P*) y 1D*DiukurNIST
430.59074 nm6400Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p x 5D*DiukurNIST
453.55686 nm6100Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5F*DiukurNIST
394.77683 nm5700Ti Iemission3d2.4s2 a 3F → 3d2.(1D).4s.4p.(3P*) 3P*DiukurNIST
502.00263 nm5100Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5G*DiukurNIST
430.10787 nm4900Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p x 5D*DiukurNIST
503.5903 nm4900Ti Iemission3d3.(4F).4s b 3F → 3d3.(4F).4p w 3G*DiukurNIST
502.28679 nm4800Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5G*DiukurNIST
453.59176 nm4700Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5F*DiukurNIST
430.05538 nm4400Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p x 5D*DiukurNIST
453.60403 nm4000Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5F*DiukurNIST
503.64639 nm4000Ti Iemission3d3.(4F).4s b 3F → 3d3.(4F).4p w 3G*DiukurNIST
501.61609 nm3800Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5G*DiukurNIST
451.8022 nm3700Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5F*DiukurNIST
488.50794 nm3700Ti Iemission3d3.(2G).4s a 3G → 3d3.(2G).4p y 3H*DiukurNIST
392.45264 nm3600Ti Iemission3d2.4s2 a 3F → 3d3.(4F).4p y 3D*DiukurNIST
402.45711 nm3600Ti Iemission3d2.4s2 a 3F → 3d2.(3F).4s.4p.(1P*) y 3F*DiukurNIST
390.47826 nm3500Ti Iemission3d2.4s2 a 1D → 3d2.(1D).4s.4p.(1P*) y 1F*DiukurNIST
452.2797 nm3500Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5F*DiukurNIST
502.48444 nm3500Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5G*DiukurNIST
398.24811 nm3400Ti Iemission3d2.4s2 a 3F → 3d2.(3P).4s.4p.(3P*) z 5S*DiukurNIST
454.87635 nm3400Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5F*DiukurNIST
455.24533 nm3400Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p y 5F*DiukurNIST
400.89274 nm3300Ti Iemission3d2.4s2 a 3F → 3d2.(3F).4s.4p.(1P*) y 3F*DiukurNIST
503.83979 nm3300Ti Iemission3d3.(4F).4s b 3F → 3d3.(4F).4p w 3G*DiukurNIST
392.98737 nm3200Ti Iemission3d2.4s2 a 3F → 3d3.(4F).4p y 3D*DiukurNIST
429.86657 nm3200Ti Iemission3d3.(4F).4s a 5F → 3d3.(4F).4p x 5D*DiukurNIST
489.99088 nm3200Ti Iemission3d3.(2G).4s a 3G → 3d3.(2G).4p y 3H*DiukurNIST

Sifat Lanjutan

Jari-jari Kovalen (Lanjutan)

Jari-jari kovalen (Pyykkö)
136 pm
Jari-jari kovalen (Pyykkö, ikatan rangkap dua)
117 pm
Jari-jari kovalen (Pyykkö, ikatan rangkap tiga)
108 pm
Jari-jari kovalen (Bragg)
140 pm

Jari-jari van der Waals

Batsanov
215 pm
Alvarez
246 pm
UFF
317,5 pm
MM3
239 pm

Jari-jari Atom & Logam

Jari-jari atom (Rahm)
257 pm
Jari-jari logam (C12)
147 pm

Skala Penomoran

Mendeleev
43
Pettifor
51
Glawe
51

Skala Keelektronegatifan

Ghosh
0
Miedema
4
Gunnarsson–Lundqvist
5
Robles–Bartolotti
4

Polarizabilitas & Dispersi

Polarizabilitas dipol
100 a.u.
Polarizabilitas dipol (ketidakpastian)
10 a.u.
C₆
1044 Ha·Bohr6
C₆ (Gould–Bučko)
1200 Ha·Bohr6

Afinitas Kimia

Afinitas proton
876 kJ/mol
Kebasaan fase gas
853,7 kJ/mol

Parameter Miedema

Volume molar Miedema
10,58 cm3/mol
Kerapatan elektron Miedema
4

Risiko Pasokan & Ekonomi

Konsentrasi produksi
21
Risiko pasokan relatif
5
Distribusi cadangan
29
Stabilitas politik (produsen terbesar)
81
Stabilitas politik (pemilik cadangan terbesar)
24

Transisi Fase & Alotrop

Titik lebur1943,15 K
Titik didih3560,15 K

Kategori Bilangan Oksidasi

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

Data Referensi Lanjutan

Konstanta Pemerisaian (7)
nOrbitalσ
1s0,5591
2p3,9352
2s6,6234
3d13,8586
3p11,8963
3s10,9669
4s17,1832
Detail Jari-jari Kristal (6)
MuatanCNSpinrcrystal (pm)Asal
2VI100estimated,
3VI81from r^3 vs V plots,
4IV56calculated,
4V65calculated,
4VI74,5from r^3 vs V plots,
4VIII88calculated,
Mode Peluruhan Isotop (47)
IsotopModeIntensitas
37p—
382p—
39B+100%
39B+p93,7%
392p—
40B+100%
40B+p95,8%
41B+100%
41B+p91,1%
42B+100%
Faktor Hamburan Sinar-X (530)
Energi (eV)f₁f₂
10—1,51668
10,1428—1,54246
10,3068—1,57217
10,4735—1,60245
10,6429—1,63331
10,8151—1,66477
10,99—1,70636
11,1677—1,75257
11,3484—1,80003
11,5319—1,84878

Data Tambahan

Sources

Sources of this element.

Titanium is present in meteorites and the sun. Rocks obtained during the Apollo 17 lunar mission showed presence of 12.1% TiO2; rocks obtained during earlier Apollo missions show lower percentages.

Titanium oxide bands are prominent in the spectra of M-type stars. The element is the ninth most abundant in the crust of the earth. Titanium is almost always present in igneous rocks and in the sediments derived from them.

It occurs in the minerals rutile, ilmenite, and sphene, and is present in titanates and in many iron ores. Titanium is present in ash of coal, in plants, and in human body.

The metal was a laboratory curiosity until Kroll, in 1946, showed that titanium could be produced commercially by reducing titanium tetrachloride with magnesium. This method is still largely used for producing the metal. The metal can be purified by decomposing the iodide.

Referensi (1)

Referensi

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

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)
Titanium

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
Titanium

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
Titanium

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
Titanium

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
Titanium

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

9 PubChem Elements
Titanium

The element property data was retrieved from publications.

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