Hafnium (Hf)
transition-metalSolid
प्रमाणित अणुभार
178.49 uइलेक्ट्रॉन संरूपण
[Xe] 6s2 4f14 5d2द्रवणांक
2232.85 °Cउत्कलनांक
4602.85 °Cघनता
1.33e+4 kg/m³ऑक्सिडीकरण अवस्था
−2, 0, +1, +2, +3, +4विद्युतऋणता (पॉलिंग)
1.3आयनीकरण ऊर्जा (पहिली)
6.82507 eVशोधाचे वर्ष
1911अणुत्रिज्या
155 pmतपशील
Hafnium is a dense, corrosion-resistant transition metal in group 4, chemically close to zirconium. It occurs almost entirely with zirconium minerals and is difficult to separate because the two elements have similar ionic sizes and chemistry. A defining technological feature is its very large thermal-neutron absorption cross section, which contrasts with zirconium's low absorption and makes high-purity separation important for nuclear applications.
Hafnium is a ductile metal with a brilliant silver luster. Its properties are considerably influenced by presence of zirconium impurities. Of all the elements, zirconium and hafnium are two of the most difficult to separate. Although their chemistry is almost identical, the density of zirconium is about half of hafnium. Very pure hafnium has been produced, with zirconium being the major impurity.
Hafnium has been successfully alloyed with iron, titanium, niobium, tantalum, and other metals. Hafnium carbide is the most refractory binary composition known, and the nitride is the most refractory of all known metal nitrides (m.p. 3310C). At 700 degrees C hafnium rapidly absorbs hydrogen to form the composition HfH1.86.
Hafnium is resistant to concentrated alkalis, but at elevated temperatures reacts with oxygen, nitrogen, carbon, boron, sulfur, and silicon. Halogens react directly to form tetrahalides.
The name derives from the Latin hafnia for Copenhagen. An element named celtium was erroneously claimed to have been discovered in 1911 by the French chemist Georges Urbain in rare earth samples, until the Danish physicist Niels Bohr, predicted hafnium's properties using his theory of electronic configuration of the elements. Bohr argued that hafnium would not be a rare earth element, but would be found in zirconium ore. Hafnium was discovered by the Dutch physicist Dirk Coster and the Hungarian physicist George von Hevesy in 1923, while working at Bohr's Institute in Copenhagen.
Hafnium was discovered by Dirk Coster, a Danish chemist, and George Charles de Hevesy, a Hungarian chemist, in 1923. They used a method known as X-ray spectroscopy to study the arrangement of the outer electrons of atoms in samples of zirconium ore. The electron structure of hafnium had been predicted by Niels Bohr and Coster and Hevesy found a pattern that matched. Hafnium is difficult to separate from zirconium and is present in all of its ores. It is obtained with the same methods used to extract zirconium.
From Hafinia, the Latin name for Copenhagen. Many years before its discovery in 1923 (credited to D. Coster and G. von Hevesey), Hafnium was thought to be present in various minerals and concentrations. On the basis of the Bohr theory, the new element was expected to be associated with zirconium.
It was finally identified in zircon from Norway, by means of X-ray spectroscope analysis. It was named in honor of the city in which the discovery was made. Most zirconium minerals contain 1 to 5 percent hafnium.
It was originally separated from zirconium by repeated recrystallization of the double ammonium or potassium fluorides by von Hevesey and Jantzen. Metallic hafnium was first prepared by van Arkel and deBoer by passing the vapor of the tetraiodide over a heated tungsten filament. Almost all hafnium metal now produced is made by reducing the tetrachloride with magnesium or with sodium (Kroll Process).
Pure hafnium is a lustrous, silvery-gray metal. It is solid and ductile under ordinary conditions and develops a thin protective oxide film in air. Finely divided hafnium can be much more reactive than bulk metal.
Hafnium is used chiefly where neutron absorption or high-temperature stability is valuable. Metallic hafnium is used in control rods and other neutron-absorbing components in some nuclear reactors. Hafnium-containing superalloys and refractory alloys can improve high-temperature strength and oxidation resistance. Hafnium dioxide, HfO₂, is used as a high-k dielectric material in semiconductor devices, replacing or supplementing silicon dioxide in advanced gate stacks. Hafnium compounds also appear in specialty ceramics, optical coatings, and catalysts, but these uses are smaller than zirconium-related industrial chemistry.
Hafnium is a good absorber of neutrons and is used in the control rods of nuclear reactors. Hafnium is also used in vacuum tubes as a getter, a material that combines with and removes trace gases from vacuum tubes. Hafnium has been used as an alloying agent in iron, titanium, niobium and other metals.
Melting near 3890°C, hafnium carbide (HfC) has the highest melting point of any known two-element compound. Hafnium nitride (HfN) also has a high melting point, around 3305°C. Other hafnium compounds include: hafnium chloride (HfCl4), hafnium fluoride (HfF4) and hafnium oxide (HfO2).
Because the element not only has a good absorption cross section for thermal neutrons (almost 600 times that of zirconium), but also excellent mechanical properties and is extremely corrosion-resistant, hafnium is used for reactor control rods. Such rods are used in nuclear submarines.
Hafnium is used in gas-filled and incandescent lamps, and is an efficient getter for scavenging oxygen and nitrogen.
Isotopes in Geochronology
Some 176Hf is radiogenic as a result of it being formed as a product of beta decay of radioactive 176Lu (half-life of 3.73×1010 years) [301] G. Faure. Principles of Isotope Geology, 2nd Edition. p. 608. Wiley, New York (1986).. Thus, relations between the isotope-amount ratiosn(176Hf)/n(177Hf) and n(176Hf)/n(176Lu) have been used to determine the ages of minerals and rocks. Because of the long half-life of 176Lu, these ratios have been used in geochronology studies that document some of the oldest rocks in the Solar System and on Earth (Fig. IUPAC.72.1).
Hafnium isotopic compositions of terrestrial materials evolved differently depending on the relative rates of 176Hf production. Geologists can use calculated lutetium-hafnium ages and the initial isotope-amount ratio n(176Hf)/n(177Hf) along with other isotopic data from the oldest rocks in the Earth to infer that the Earth’s crust differentiated within the first few hundred million years after condensation of the oldest solid matter in the Solar System [502] E. Scherer, C. Münker, K. Mezger. Science293, 683 (2001)..
Radioactive 182Hf decays to 182W with a half-life of 8.9×106 years, which is much less than the age of meteorites and the Earth. Therefore, measurements of the amounts of hafnium and tungsten isotopes in meteorites and terrestrial samples reveal the earlier presence of 182Hf. As a result, this provides information about chemical differentiation and evolution of the early Solar System [503] T. Kleine, M. Touboul, B. Bourdon, F. Nimmo, K. Mezger, H. Palme, S. B. Jacobsen, Q. Z. Yin, A. N. Halliday. Geochim. Cosmochim. Acta73, 5150 (2009)., [504] A. Schersten. Re-Os, Pt-Os and Hf-W Isotopes and Tracing the Core in Mantle Melts, MantlePlumes.org (2014), Feb. 25; http://www.mantleplumes.org/Os-W.html..
Hafnium chemistry is dominated by the +4 oxidation state, reflecting the stable Hf⁴⁺ ion and strong bonding to oxygen, halides, and other hard donor atoms. Hafnium dioxide, HfO₂, is a refractory, chemically durable oxide with high dielectric constant. Hafnium tetrachloride, HfCl₄, is a volatile moisture-sensitive chloride used in purification and chemical vapor or atomic layer deposition chemistry. Organometallic and amide precursors such as tetrakis(dimethylamido)hafnium, Hf[N(CH₃)₂]₄, are important for thin-film deposition. Lower oxidation states exist but are less common and often require specialized conditions.
See more information at the Hafnium compound page.
Bulk hafnium metal is generally of low acute chemical toxicity, but metal dust or powder can ignite and should be treated as a combustible solid. Hafnium compounds vary in hazard; soluble salts, halides, and organometallic precursors may be corrosive, moisture-sensitive, or toxic by inhalation or skin contact. Hafnium is not naturally radioactive in ordinary material, but reactor-exposed hafnium may contain activation products that require radiological control.
Finely divided hafnium is pyrophoric and can ignite spontaneously in air. Care should be taken when machining the metal or when handling hot sponge hafnium.
Hafnium is a trace lithophile element and follows zirconium in igneous rocks, sands, and resistant minerals. It is commonly hosted in zircon, ZrSiO₄, where hafnium substitutes for zirconium. The element has low mobility in most surface environments because its oxides and silicate-hosted forms are sparingly soluble. It has no known biological role, and environmental concentrations are normally controlled by the distribution and weathering resistance of zirconium minerals.
Hafnium is not usually mined as a primary product. It is recovered during the processing of zirconium minerals, especially when nuclear-grade zirconium is purified to remove neutron-absorbing impurities. Separation from zirconium is the central cost and supply constraint, commonly involving solvent extraction or related chemical fractionation followed by conversion to metal or compounds. Demand is concentrated in nuclear control materials, semiconductor precursors, and specialized high-temperature alloys. Supply is therefore tied to zirconium processing capacity and to the need for very low-hafnium zirconium in reactor fuel cladding, rather than to abundant independent hafnium ores.
Obtained from mineral zircon or baddeleyite.
Hafnium is a heavy element made mainly by neutron-capture processes in earlier generations of stars, with contributions from both slow and rapid neutron capture. It is far less abundant cosmically than lighter rock-forming elements. In planetary materials it behaves as a refractory lithophile element, condensing into high-temperature solids and concentrating with zirconium-bearing minerals rather than in metallic cores or volatile phases.
- Hafnium was one of the last stable elements to be identified in nature.
- Its name comes from Hafnia, the Latin name for Copenhagen.
- Zircon can contain enough hafnium to make separation important even when hafnium is not the desired product.
- Hafnium and zirconium are chemically so similar that early analytical work often missed hafnium.
- Hafnium carbide and tantalum hafnium carbide are noted for extremely high melting behavior.
प्रतिमा
गुणधर्म
भौतिक
- अणुत्रिज्या (अनुभवाधारित)
- 155 pm सर्व घटकांच्या अणुत्रिज्या (अनुभवाधारित) ची तुलना करा →
- सहसंयुजी त्रिज्या
- 175 pm सर्व घटकांच्या सहसंयुजी त्रिज्या ची तुलना करा →
- व्हॅन डर वाल्स त्रिज्या
- 212 pm सर्व घटकांच्या व्हॅन डर वाल्स त्रिज्या ची तुलना करा →
- धात्विक त्रिज्या
- 144 pm सर्व घटकांच्या धात्विक त्रिज्या ची तुलना करा →
- घनता
- 1.33 × 104 kg/m³ सर्व घटकांच्या घनता ची तुलना करा →
- मोलर आयतन
- 0.0136 L/mol
- STP येथे अवस्था
- घन सर्व घटकांच्या STP येथे अवस्था ची तुलना करा →
- द्रवणांक
- 2232.85 °C सर्व घटकांच्या द्रवणांक ची तुलना करा →
- उत्कलनांक
- 4602.85 °C सर्व घटकांच्या उत्कलनांक ची तुलना करा →
- उष्णता चालकता
- 23 W/(m·K) सर्व घटकांच्या उष्णता चालकता ची तुलना करा →
- विशिष्ट उष्माधारकता
- 0.144 J/(g·K) सर्व घटकांच्या विशिष्ट उष्माधारकता ची तुलना करा →
- मोलर उष्माधारकता
- 25.73 J/(mol·K) सर्व घटकांच्या मोलर उष्माधारकता ची तुलना करा →
- स्फटिक संरचना
- षट्कोणी निकट-संकुलित सर्व घटकांच्या स्फटिक संरचना ची तुलना करा →
रासायनिक
- विद्युतऋणता (पॉलिंग)
- 1.3 सर्व घटकांच्या विद्युतऋणता (पॉलिंग) ची तुलना करा →
- विद्युतऋणता (ॲलन)
- 1.16
- इलेक्ट्रॉन आसक्ती
- 0.178 eV
- आयनीकरण ऊर्जा (पहिली)
- 6.82507 eV सर्व घटकांच्या आयनीकरण ऊर्जा (पहिली) ची तुलना करा →
- आयनीकरण ऊर्जा (दुसरी)
- 14.61005 eV सर्व घटकांच्या आयनीकरण ऊर्जा (दुसरी) ची तुलना करा →
- आयनीकरण ऊर्जा (तिसरी)
- 22.550078 eV सर्व घटकांच्या आयनीकरण ऊर्जा (तिसरी) ची तुलना करा →
- आयनीकरण ऊर्जा (चौथी)
- 33.370115 eV सर्व घटकांच्या आयनीकरण ऊर्जा (चौथी) ची तुलना करा →
- आयनीकरण ऊर्जा (पाचवी)
- 68.370235 eV सर्व घटकांच्या आयनीकरण ऊर्जा (पाचवी) ची तुलना करा →
- ऑक्सिडीकरण अवस्था
- −2, 0, +1, +2, +3, +4 सर्व घटकांच्या ऑक्सिडीकरण अवस्था ची तुलना करा →
- संयुजा इलेक्ट्रॉन
- 4 सर्व घटकांच्या संयुजा इलेक्ट्रॉन ची तुलना करा →
- इलेक्ट्रॉन संरूपण
- [Xe] 6s2 4f14 5d2
उष्मागतिक
- द्रवण उष्मा
- 0.26667358 eV सर्व घटकांच्या द्रवण उष्मा ची तुलना करा →
- बाष्पीभवन उष्मा
- 5.959476 eV सर्व घटकांच्या बाष्पीभवन उष्मा ची तुलना करा →
- संप्लवन उष्मा
- 6.436234 eV
- अणूकरण उष्मा
- 6.436234 eV
- अणूकरण एन्थाल्पी
- 6.409286 eV
केंद्रकीय
- प्रोटॉन
- 72 सर्व घटकांच्या प्रोटॉन ची तुलना करा →
- न्यूट्रॉन
- 108 सर्व घटकांच्या न्यूट्रॉन ची तुलना करा →
- ज्ञात समस्थानिके
- 38 सर्व घटकांच्या ज्ञात समस्थानिके ची तुलना करा →
- स्थिर समस्थानिके
- 4 सर्व घटकांच्या स्थिर समस्थानिके ची तुलना करा →
- सर्वाधिक स्थिर समस्थानिक
- Hf-180
- शोधाचे वर्ष
- 1911
विपुलता
- विपुलता (पृथ्वीचे कवच)
- 3 mg/kg सर्व घटकांच्या विपुलता (पृथ्वीचे कवच) ची तुलना करा →
- विपुलता (महासागर)
- 7 × 10−6 mg/L सर्व घटकांच्या विपुलता (महासागर) ची तुलना करा →
स्फटिक संरचना
- जालक स्थिरांक a
- 320 pm
इलेक्ट्रॉन संरचना
- प्रत्येक कवचातील इलेक्ट्रॉन
- 2, 8, 18, 32, 10, 2 सर्व घटकांच्या प्रत्येक कवचातील इलेक्ट्रॉन ची तुलना करा →
ओळखचिन्हे
- CAS क्रमांक
- 7440-58-6 सर्व घटकांच्या CAS क्रमांक ची तुलना करा →
- टर्म चिन्ह
- 3F2
- InChI
- InChI=1S/Hf
- InChI की
- VBJZVLUMGGDVMO-UHFFFAOYSA-N
इलेक्ट्रॉन संरूपण मोजलेले
Hf: 4f¹⁴ 5d² 6s²[Xe] 4f¹⁴ 5d² 6s²1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d² 6s²अणुप्रतिमान
समस्थानिकांमुळे न्यूट्रॉन संख्या, वस्तुमान आणि स्थैर्य बदलते — विद्युतदृष्ट्या उदासीन अणूचे इलेक्ट्रॉन संरूपण बदलत नाही.
योजनात्मक अणुप्रतिमान, प्रमाणानुसार नाही.
अणूची विशिष्ट ओळख
उत्सर्जन / शोषण वर्णपट
समस्थानिक वितरण
| वस्तुमानांक | अणुवस्तुमान (u) | नैसर्गिक विपुलता | अर्धायुष्य |
|---|---|---|---|
| 176 स्थिर | १७५.९४१४०७६ ± ०.०००००२२ | 5.2600% | स्थिर |
| 178 स्थिर | १७७.९४३७०५८ ± ०.०००००२ | 27.2800% | स्थिर |
| 179 स्थिर | १७८.९४५८२३२ ± ०.०००००२ | 13.6200% | स्थिर |
| 180 स्थिर | १७९.९४६५५७ ± ०.०००००२ | 35.0800% | स्थिर |
अवस्था / स्थिती
कारण: द्रवणांकापेक्षा (2232.85 °C) 2207.8 °C कमी
योजनात्मक, प्रमाणानुसार नाही
अवस्थांतर बिंदू
अवस्थांतर ऊर्जा
द्रवणांकावर 1 mol वितळवण्यासाठी आवश्यक ऊर्जा
उत्कलनांकावर 1 mol चे बाष्पीभवन करण्यासाठी आवश्यक ऊर्जा
संप्लवनांकावर 1 mol चे संप्लवन करण्यासाठी आवश्यक ऊर्जा
घनता
प्रमाणित परिस्थितीत
प्रमाणित परिस्थितीत
अणुवर्णपट
72 पैकी 10 दाखवले आहेत. आयनाच्या विद्युतभारानुसार चढत्या क्रमाने मांडलेले.
वर्णरेषांचा संग्रह ?
| आयन | विद्युतभार | एकूण वर्णरेषा | संक्रमण संभाव्यता | पातळ्यांची नामांकने |
|---|---|---|---|---|
| Hf I | 0 | 5341 | 187 | 3821 |
| Hf II | +1 | 218 | 2 | 10 |
| Hf III | +2 | 37 | 0 | 0 |
| Hf IV | +3 | 27 | 0 | 0 |
| Hf V | +4 | 82 | 0 | 0 |
ऊर्जा पातळ्यांचा संग्रह ?
| आयन | विद्युतभार | पातळ्या |
|---|---|---|
| Hf I | 0 | 333 |
| Hf II | +1 | 125 |
| Hf III | +2 | 2 |
| Hf IV | +3 | 2 |
| Hf V | +4 | 2 |
| Hf VI | +5 | 2 |
| Hf VII | +6 | 2 |
| Hf VIII | +7 | 2 |
| Hf IX | +8 | 2 |
| Hf X | +9 | 2 |
आयनिक त्रिज्या
| विद्युतभार | समन्वय | प्रचक्रण | त्रिज्या |
|---|---|---|---|
| +4 | 4 | उपलब्ध नाही | 57.99999999999999 pm |
| +4 | 6 | उपलब्ध नाही | 71 pm |
| +4 | 7 | उपलब्ध नाही | 76 pm |
| +4 | 8 | उपलब्ध नाही | 83 pm |
संयुगे
समस्थानिके (4)
| वस्तुमानांक | अणुवस्तुमान (u) | नैसर्गिक विपुलता | अर्धायुष्य | क्षय प्रकार | |
|---|---|---|---|---|---|
| 176 स्थिर | १७५.९४१४०७६ ± ०.०००००२२ | 5.2600% ± 0.0700% | स्थिर | stable | |
| 178 स्थिर | १७७.९४३७०५८ ± ०.०००००२ | 27.2800% ± 0.0700% | स्थिर | stable | |
| 179 स्थिर | १७८.९४५८२३२ ± ०.०००००२ | 13.6200% ± 0.0200% | स्थिर | stable | |
| 180 स्थिर | १७९.९४६५५७ ± ०.०००००२ | 35.0800% ± 0.1600% | स्थिर | stable |
वर्णरेषा
1890 पैकी 50 दाखवले आहेत. मूलभूत सेटिंगनुसार केवळ मोजलेली तीव्रता असलेल्या वर्णरेषा दाखवल्या जातात.
| तरंगलांबी (nm) | तीव्रता | आयनीकरण टप्पा | प्रकार | संक्रमण | अचूकता | स्रोत | |
|---|---|---|---|---|---|---|---|
| 417.433998 nm | 48000 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p z 5D* | मोजलेले | NIST | |
| 380.03629 nm | 36000 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p z 5D* | मोजलेले | NIST | |
| 382.072307 nm | 34000 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p y 3F* | मोजलेले | NIST | |
| 723.71003 nm | 34000 | Hf I | emission | 5d2.6s2 a 3F → 5d.6s2.(a 2D).6p z 3D* | मोजलेले | NIST | |
| 384.917811 nm | 32000 | Hf I | emission | 5d2.6s2 a 1D → 5d2.(a 3F).6s.(a 2F).6p y 1D* | मोजलेले | NIST | |
| 713.1807 nm | 32000 | Hf I | emission | 5d2.6s2 a 3F → 5d.6s2.(a 2D).6p z 3D* | मोजलेले | NIST | |
| 389.993003 nm | 29000 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p z 5D* | मोजलेले | NIST | |
| 395.181289 nm | 26000 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p y 3F* | मोजलेले | NIST | |
| 385.830632 nm | 25000 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p y 3D* | मोजलेले | NIST | |
| 724.0873 nm | 21000 | Hf I | emission | 5d2.6s2 a 3F → 5d.6s2.(a 2D).6p z 3D* | मोजलेले | NIST | |
| 393.137246 nm | 19000 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p y 3D* | मोजलेले | NIST | |
| 480.049829 nm | 17000 | Hf I | emission | 5d2.6s2 a 1D → 5d.6s2.(a 2D).6p z 1P* | मोजलेले | NIST | |
| 397.347912 nm | 15000 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p z 5D* | मोजलेले | NIST | |
| 706.38474 nm | 15000 | Hf I | emission | 5d2.6s2 a 1D → 5d.6s2.(a 2D).6p z 3P* | मोजलेले | NIST | |
| 381.177553 nm | 14000 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p z 3G* | मोजलेले | NIST | |
| 555.06011 nm | 14000 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p z 5G* | मोजलेले | NIST | |
| 555.211884 nm | 14000 | Hf I | emission | 5d2.6s2 a 1D → 5d.6s2.(a 2D).6p z 1F* | मोजलेले | NIST | |
| 456.593715 nm | 13000 | Hf I | emission | 5d2.6s2 a 1D → 5d2.(a 3P).6s.(a 4P).6p y 5D* | मोजलेले | NIST | |
| 435.630591 nm | 12000 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p z 5D* | मोजलेले | NIST | |
| 445.734411 nm | 12000 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p z 5F* | मोजलेले | NIST | |
| 459.87979 nm | 12000 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p z 5F* | मोजलेले | NIST | |
| 462.086529 nm | 12000 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p z 5F* | मोजलेले | NIST | |
| 465.518924 nm | 12000 | Hf I | emission | 5d2.6s2 a 3P → 5d2.(a 3P).6s.(a 4P).6p z 3S* | मोजलेले | NIST | |
| 380.044548 nm | 11000 | Hf I | emission | 5d2.6s2 a 1D → 5d2.(a 3P).6s.(a 4P).6p z 5S* | मोजलेले | NIST | |
| 429.477692 nm | 11000 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p z 5D* | मोजलेले | NIST | |
| 681.89395 nm | 11000 | Hf I | emission | 5d2.6s2 a 3P → 5d.6s2.(a 2D).6p z 1F* | मोजलेले | NIST | |
| 396.799621 nm | 10000 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p z 5D* | मोजलेले | NIST | |
| 406.28356 nm | 10000 | Hf I | emission | 5d.6s2.(a 2D).6p z 1D* → 3512 | मोजलेले | NIST | |
| 497.525232 nm | 10000 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p z 5F* | मोजलेले | NIST | |
| 454.093108 nm | 8400 | Hf I | emission | 5d2.6s2 a 1D → 5d2.(a 3F).6s.(a 4F).6p y 3F* | मोजलेले | NIST | |
| 443.80364 nm | 8300 | Hf I | emission | 5d2.6s2 a 3P → 5d2.(a 3P).6s.(a 4P).6p z 3S* | मोजलेले | NIST | |
| 446.117576 nm | 8300 | Hf I | emission | 5d2.6s2 a 1D → 5d2.(a 3P).6s.(a 4P).6p z 3S* | मोजलेले | NIST | |
| 459.891547 nm | 8300 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p z 5D* | मोजलेले | NIST | |
| 408.33549 nm | 8000 | Hf I | emission | 5d.6s2.(a 2D).6p z 1D* → 3499 | मोजलेले | NIST | |
| 571.91718 nm | 7300 | Hf I | emission | 5d2.6s2 a 3P → 5d.6s2.(a 2D).6p z 1P* | मोजलेले | NIST | |
| 403.225898 nm | 7200 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p y 3F* | मोजलेले | NIST | |
| 478.27405 nm | 7100 | Hf I | emission | 5d.6s2.(a 2D).6p z 3F* → 6p2.(3P).5d.(2D).6s c 3D | मोजलेले | NIST | |
| 383.001314 nm | 6700 | Hf I | emission | 5d3.(b 4F).6s a 5F → 5d2.(b 1D).6s.(b 2D).6p v 3F* | मोजलेले | NIST | |
| 504.743848 nm | 6500 | Hf I | emission | 5d2.6s2 a 3P → 5d2.(a 3F).6s.(a 4F).6p y 3D* | मोजलेले | NIST | |
| 485.92338 nm | 6400 | Hf I | emission | 5d.6s2.(a 2D).6p z 3F* → 3512 | मोजलेले | NIST | |
| 386.09058 nm | 6300 | Hf I | emission | 5d2.6s2 a 3P → 5d2.(a 3F).6s.(a 2F).6p y 1F* | मोजलेले | NIST | |
| 441.790242 nm | 6200 | Hf I | emission | 5d2.6s2 a 1D → 5d2.(a 3F).6s.(a 4F).6p y 3D* | मोजलेले | NIST | |
| 388.935622 nm | 5900 | Hf I | emission | 5d2.6s2 a 1D → 5d2.(a 3P).6s.(a 4P).6p y 5D* | मोजलेले | NIST | |
| 469.90048 nm | 5900 | Hf I | emission | 5d2.(a 3F).6s.(a 4F).6p z 5G* → 5d2.(3F).6s.(a 4F).7s b 5F | मोजलेले | NIST | |
| 678.92714 nm | 5900 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p z 5G* | मोजलेले | NIST | |
| 433.027751 nm | 5800 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p y 3F* | मोजलेले | NIST | |
| 410.65431 nm | 5600 | Hf I | emission | 5d2.6s2 a 1G → 5d2.(a 3F).6s.(a 2F).6p y 1F* | मोजलेले | NIST | |
| 426.34428 nm | 5400 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p z 5F* | मोजलेले | NIST | |
| 477.37157 nm | 5400 | Hf I | emission | 5d2.6s2 a 3P → 5d.6s2.(a 2D).6p z 1P* | मोजलेले | NIST | |
| 590.29382 nm | 5400 | Hf I | emission | 5d2.6s2 a 3F → 5d2.(a 3F).6s.(a 4F).6p z 5G* | मोजलेले | NIST |
विस्तारित गुणधर्म
सहसंयुजी त्रिज्या (विस्तारित)
- सहसंयुजी त्रिज्या (प्युक्को)
- 152 pm
- सहसंयुजी त्रिज्या (प्युक्को, दुहेरी बंध)
- 128 pm
- सहसंयुजी त्रिज्या (प्युक्को, तिहेरी बंध)
- 122 pm
व्हॅन डर वाल्स त्रिज्या
- Batsanov
- 225 pm
- Alvarez
- 263 pm
- UFF
- 314.1 pm
- MM3
- 253 pm
अणुत्रिज्या आणि धात्विक त्रिज्या
- अणुत्रिज्या (राह्म)
- 264 pm
- धात्विक त्रिज्या (C12)
- 159 pm
क्रमांकन मापनपट्ट्या
- Mendeleev
- 45
- Pettifor
- 50
- Glawe
- 50
विद्युतऋणता मापनपट्ट्या
- Ghosh
- 0
- Miedema
- 4
- Gunnarsson–Lundqvist
- 5
- Robles–Bartolotti
- 4
ध्रुवणक्षमता आणि अपस्करण
- द्विध्रुव ध्रुवणक्षमता
- 103 a.u.
- द्विध्रुव ध्रुवणक्षमता (अनिश्चितता)
- 6 a.u.
- C₆ (Gould–Bučko)
- 1040 Ha·Bohr6
मिडेमा प्राचल
- मिडेमा मोलर आयतन
- 13.45 cm3/mol
- मिडेमा इलेक्ट्रॉन घनता
- 3
अवस्थांतरे आणि अपरूपे
| द्रवणांक | 2506.15 K |
| उत्कलनांक | 4873.15 K |
ऑक्सिडीकरण अवस्थांचे वर्ग
प्रगत संदर्भ माहिती
परिरक्षण स्थिरांक (14)
| n | कक्षिका | σ |
|---|---|---|
| 1 | s | 1.3984 |
| 2 | p | 4.4012 |
| 2 | s | 18.8102 |
| 3 | d | 13.5702 |
| 3 | p | 21.0168 |
| 3 | s | 21.6885 |
| 4 | d | 36.476 |
| 4 | f | 39.7904 |
| 4 | p | 34.0704 |
| 4 | s | 33.0228 |
स्फटिक त्रिज्यांचा तपशील (4)
| विद्युतभार | CN | प्रचक्रण | rcrystal (pm) | उत्पत्ती |
|---|---|---|---|---|
| 4 | IV | 72 | from r^3 vs V plots, | |
| 4 | VI | 85 | from r^3 vs V plots, | |
| 4 | VII | 90 | ||
| 4 | VIII | 97 |
समस्थानिक क्षय प्रकार (46)
| समस्थानिक | मोड | तीव्रता |
|---|---|---|
| 153 | B+ | — |
| 154 | B+ | 100% |
| 154 | A | 0% |
| 155 | B+ | 100% |
| 155 | A | — |
| 156 | A | 100% |
| 156 | B+ | — |
| 157 | A | 94% |
| 157 | B+ | 14% |
| 158 | B+ | 55.7% |
क्ष-किरण प्रकीर्णन गुणक (514)
| ऊर्जा (eV) | f₁ | f₂ |
|---|---|---|
| 10 | — | 2.62338 |
| 10.1617 | — | 2.71485 |
| 10.3261 | — | 2.80951 |
| 10.4931 | — | 2.90326 |
| 10.6628 | — | 2.98247 |
| 10.8353 | — | 3.06384 |
| 11.0106 | — | 3.14744 |
| 11.1886 | — | 3.21346 |
| 11.3696 | — | 3.27509 |
| 11.5535 | — | 3.33789 |
अतिरिक्त माहिती
Estimated Crustal Abundance
The estimated element abundance in the earth's crust.
3.0 milligrams per kilogram
संदर्भ (1)
Estimated Oceanic Abundance
The estimated element abundance in the earth's oceans.
7×10-6 milligrams per liter
संदर्भ (1)
संदर्भ
(9)
Data deposited in or computed by PubChem
The half-life and atomic mass data was provided by the Atomic Mass Data Center at the International Atomic Energy Agency.
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.
The information are cited from Pure Appl. Chem. 2018; 90(12): 1833-2092, https://doi.org/10.1515/pac-2015-0703.
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/
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.
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
This section provides all form of data related to element Hafnium.
The element property data was retrieved from publications.