Yttrium (Y)
transition-metalSolid
मानक परमाणु भार
88.90584 uइलेक्ट्रॉन विन्यास
[Kr] 5s2 4d1गलनांक
1521.85 °Cक्वथनांक
3344.85 °Cघनत्व
4470 kg/m³ऑक्सीकरण अवस्थाएँ
0, +1, +2, +3विद्युतऋणात्मकता (पॉलिंग)
1.22आयनन ऊर्जा (प्रथम)
6.21726 eVखोज का वर्ष
1794परमाणु त्रिज्या
180 pmविवरण
Yttrium is a silvery transition metal grouped with the rare-earth elements because it commonly occurs with lanthanides and forms predominantly trivalent cations. Its chemistry is close to the heavier lanthanides, especially holmium and erbium, rather than to scandium. Although not itself a lanthanide, yttrium is a key component of phosphors, ceramics, lasers, and high-temperature oxide materials.
Yttrium has a silver-metallic luster and is relatively stable in air. Turnings of the metal, however, ignite in air if their temperature exceeds 400°C. Finely divided yttrium is very unstable in air.
The name derives from the Swedish village of Ytterby where the mineral gadolinite was found. In 1794, the Finnish chemist Johan Gadolin discovered yttrium in the mineral ytterbite, which was later renamed gadolinite for Gadolin. Gadolin originally called the element ytterbium after ytterbite. The name was subsequently shortened to yttrium, and later another element was given the name ytterbium.
Yttrium was discovered by Johan Gadolin, a Finnish chemist, while analyzing the composition of the mineral gadolinite ((Ce, La, Nd, Y)2FeBe2Si2O10) in 1789. Gadolinite, which was named for Johan Gadolin, was discovered several years earlier in a quarry near the town of Ytterby, Sweden. Today, yttrium is primarily obtained through an ion exchange process from monazite sand ((Ce, La, Th, Nd, Y)PO4), a material rich in rare earth elements.
Namded after Ytterby, a village in Sweden near Vauxholm. Yttria earth containing yttrium was discovered by Gadolin in 1794. Ytterby is the site of a quarry which yielded many unusual minerals containing rare earths and other elements. This small town, near Stockholm, bears the honor of giving names to erbium, terbium, and ytterbium as well as yttrium.
In 1843 Mosander showed that yttira could be resolved into the oxides (or earths) of three elements. The name yttria was reserved for the most basic one; the others were named erbia and terbia.
Pure yttrium is a soft, silvery-white metal with a metallic luster. It is reasonably stable in dry air at room temperature because a thin oxide film forms, but finely divided metal is more reactive and can ignite when heated.
Yttrium is used mainly through its compounds and oxide ceramics. Yttrium oxide, Y₂O₃, is a host and stabilizer in red phosphors, optical ceramics, and refractory materials. Yttrium aluminum garnet, Y₃Al₅O₁₂, is the host crystal for Nd:YAG lasers. Yttria-stabilized zirconia is used in oxygen sensors, thermal-barrier coatings, and solid oxide fuel cells. Small additions of yttrium improve oxidation resistance and grain behavior in some alloys.
Although metallic yttrium is not widely used, several of its compounds are. Yttrium oxide (Y2O3) and yttrium orthovanadate (YVO4) are both combined with europium to produce the red phosphor used in color televisions. Garnets made from yttrium and iron (Y3Fe5O12) are used as microwave filters in microwave communications equipment. Garnets made from yttrium and aluminum (Y3Al5O12) are used in jewelry as simulated diamond.
Yttrium oxide is one of the most important compounds of yttrium and accounts for the largest use. It is widely used in making YVO4 europium, and Y2O3 europium phosphors to give the red color in color television tubes. Hundreds of thousands of pounds are now used in this application.
Yttrium oxide also is used to produce yttrium-iron-garnets, which are very effective microwave filters.
Yttrium iron, aluminum, and gadolinium garnets, with formulas such as Y3Fe5O12 and Y3Al5O12, have interesting magnetic properties. Yttrium iron garnet is also exceptionally efficient as both a transmitter and transducer of acoustic energy. Yttrium aluminum garnet, with a hardness of 8.5, is also finding use as a gemstone (simulated diamond).
Small amounts of yttrium (0.1 to 0.2%) can be used to reduce the grain size in chromium, molybdenum, zirconium, and titanium, and to increase strength of aluminum and magnesium alloys.
Alloys with other useful properties can be obtained by using yttrium as an additive. The metal can be used as a deoxidizer for vanadium and other nonferrous metals. The metal has a low cross section for nuclear capture. 90Y, one of the isotopes of yttrium, exists in equilibrium with its parent 90Sr, a product of nuclear explosions. Yttrium has been considered for use as a nodulizer for producing nodular cast iron, in which the graphite forms compact nodules instead of the usual flakes. Such iron has increased ductility.
Yttrium also can be used in laser systems and as a catalyst for ethylene polymerization reactions.
It also has potential use in ceramic and glass formulas, as the oxide has a high melting point and imparts shock resistance and low expansion characteristics to glass.
Isotopes in Medicine
Carbon nanotubes (CNT), which are nano-scaled carbon tubes, are being examined in nanobiotechnology research studies because it has been discovered that CNTs labeled with 86Y (with a half-life of 0.6 day) are soluble when they are injected into mice. This discovery was made after mice were given an intravenous or intraperitoneal (directly into a body cavity) injection with the 86Y CNT and then were examined using positron emission tomography (PET) scans to observe whether the 86Y had been flushed from their systems. The PET scan determined that accumulation of 86Y occurred in the liver, kidney, and spleen with very rapid blood clearance. This has broad implications for developing drug treatments [303] M. R. McDevitt, D. Chattopadhyay, J. S. Jaggi, R. D. Finn, P. B. Zanzonico, C. Villa, D. Rey, J. Mendenhall, C. A. Batt, J. T. Njardarson, D. A. Scheinberg. PLoS One2, e907 (2007).. Radiomicrosphere therapy (RT) that uses 90Y (with a half-life of 64 h) microspheres is a proven therapy that helps treat hepatic (liver) cancer (Fig. IUPAC.39.1) [304] C. D. South, M. M. Meyer, G. Meis, E. Y. Kim, F. B. Thomas, A. A. Rikabi, H. Khabiri, M. Bloomston. World J. Surg. Oncol.6, 93 (2008).. 90Y is also used in radiosynovectomy to reduce joint pain [305] E. ‐C. Rodríguez‐Merchán, L. A. Valentino (Eds.), Current and Future Issues in Hemophilia Care, John Wiley & Sons, New York (2011)..
Yttrium most often occurs in the +3 oxidation state, forming colorless or white salts because Y³⁺ has no f electrons. Yttrium oxide, Y₂O₃, is basic and refractory, and yttrium fluoride, YF₃, is a stable, sparingly soluble fluoride. Yttrium chloride, YCl₃, and yttrium nitrate, Y(NO₃)₃, are common soluble laboratory precursors. Mixed oxides such as yttrium barium copper oxide, YBa₂Cu₃O₇−δ, are important in superconductivity, with properties strongly dependent on oxygen content.
See more information at the Yttrium compound page.
Massive yttrium metal has low acute toxicity, but metal dust is a fire hazard and can irritate the lungs or skin. Soluble yttrium salts can be harmful if inhaled or ingested in significant amounts, and insoluble dusts require ordinary industrial dust control. Radioisotope ⁹⁰Y is a strong beta emitter used medically; its hazard is isotope-specific and mainly radiological, not a property of stable natural yttrium.
Yttrium is dispersed in the crust and is usually associated with rare-earth minerals rather than concentrated in its own ores. It is relatively immobile under neutral to alkaline conditions because Y³⁺ hydrolyzes and binds to oxides, phosphates, and organic matter. Weathering can concentrate yttrium with heavy rare earths in ion-adsorption clays and lateritic deposits. No essential biological role is known.
Yttrium is produced as part of rare-earth mining and separation, not as an independent primary metal commodity. Important sources include xenotime, monazite, bastnäsite fractions, and heavy-rare-earth-rich ion-adsorption clays. Separation is difficult because yttrium tracks the heavy lanthanides chemically, so solvent extraction and ion-exchange processes are central to supply. Demand is tied to phosphors, ceramics, lasers, and stabilized zirconia, with substitution possible in some phosphor applications but harder in structural ceramic uses. Recycling is limited and mostly associated with specialized phosphor and electronic waste streams.
Yttrium occurs in nearly all of the rare-earth minerals. Analysis of lunar rock samples obtained during the Apollo missions show a relatively high yttrium content.
It is recovered commercially from monazite sand, which contains about 3%, and from bastnasite, which contains about 0.2%. Wohler obtained the impure element in 1828 by reduction of the anhydrous chloride with potassium. The metal is now produced commercially by reduction of the fluoride with calcium metal. It can also be prepared by other techniques.
Yttrium is a trace element in the cosmos, made mainly by slow and rapid neutron-capture processes in evolved stars and explosive stellar environments. In the Solar System it is far less abundant than iron-group elements but more abundant than many neighboring heavy elements. Its single stable isotope, ⁸⁹Y, makes extraterrestrial yttrium isotopically simple compared with many rare earths.
- Yttrium has only one stable isotope, ⁸⁹Y.
- It was named from Ytterby, the Swedish village linked to several rare-earth discoveries.
- Y³⁺ is diamagnetic, unlike many neighboring lanthanide ions.
- Yttrium is often counted with the heavy rare earths in mining and trade.
- Nd:YAG laser crystals contain yttrium in the host lattice, not as the lasing ion.
- Yttria-stabilized zirconia conducts oxide ions at high temperature.
चित्र
गुण
भौतिक
- परमाणु त्रिज्या (आनुभविक)
- 180 pm सभी तत्वों की परमाणु त्रिज्या (आनुभविक) की तुलना करें →
- सहसंयोजक त्रिज्या
- 190 pm सभी तत्वों की सहसंयोजक त्रिज्या की तुलना करें →
- वान डर वाल्स त्रिज्या
- 219 pm सभी तत्वों की वान डर वाल्स त्रिज्या की तुलना करें →
- धात्विक त्रिज्या
- 162 pm सभी तत्वों की धात्विक त्रिज्या की तुलना करें →
- घनत्व
- 4470 kg/m³ सभी तत्वों की घनत्व की तुलना करें →
- मोलर आयतन
- 0.0198 L/mol
- STP पर प्रावस्था
- ठोस सभी तत्वों की STP पर प्रावस्था की तुलना करें →
- गलनांक
- 1521.85 °C सभी तत्वों की गलनांक की तुलना करें →
- क्वथनांक
- 3344.85 °C सभी तत्वों की क्वथनांक की तुलना करें →
- विशिष्ट ऊष्मा धारिता
- 0.298 J/(g·K) सभी तत्वों की विशिष्ट ऊष्मा धारिता की तुलना करें →
- मोलर ऊष्मा धारिता
- 26.53 J/(mol·K) सभी तत्वों की मोलर ऊष्मा धारिता की तुलना करें →
- क्रिस्टल संरचना
- षट्कोणीय सघन संकुलित सभी तत्वों की क्रिस्टल संरचना की तुलना करें →
रासायनिक
- विद्युतऋणात्मकता (पॉलिंग)
- 1.22 सभी तत्वों की विद्युतऋणात्मकता (पॉलिंग) की तुलना करें →
- विद्युतऋणात्मकता (ऐलन)
- 1.12
- इलेक्ट्रॉन बंधुता
- 0.307 eV
- आयनन ऊर्जा (प्रथम)
- 6.21726 eV सभी तत्वों की आयनन ऊर्जा (प्रथम) की तुलना करें →
- आयनन ऊर्जा (द्वितीय)
- 12.223642 eV सभी तत्वों की आयनन ऊर्जा (द्वितीय) की तुलना करें →
- आयनन ऊर्जा (तृतीय)
- 20.524481 eV सभी तत्वों की आयनन ऊर्जा (तृतीय) की तुलना करें →
- आयनन ऊर्जा (चतुर्थ)
- 60.607409 eV सभी तत्वों की आयनन ऊर्जा (चतुर्थ) की तुलना करें →
- आयनन ऊर्जा (पंचम)
- 75.350259 eV सभी तत्वों की आयनन ऊर्जा (पंचम) की तुलना करें →
- ऑक्सीकरण अवस्थाएँ
- 0, +1, +2, +3 सभी तत्वों की ऑक्सीकरण अवस्थाएँ की तुलना करें →
- संयोजकता इलेक्ट्रॉन
- 3 सभी तत्वों की संयोजकता इलेक्ट्रॉन की तुलना करें →
- इलेक्ट्रॉन विन्यास
- [Kr] 5s2 4d1
ऊष्मागतिक
- गलन ऊष्मा
- 0.11836037 eV सभी तत्वों की गलन ऊष्मा की तुलना करें →
- वाष्पन ऊष्मा
- 3.762243 eV सभी तत्वों की वाष्पन ऊष्मा की तुलना करें →
- ऊर्ध्वपातन ऊष्मा
- 4.394465 eV
- परमाणुकरण ऊष्मा
- 4.394465 eV
- परमाणुकरण एन्थैल्पी
- 4.40172 eV
नाभिकीय
- प्रोटॉन
- 39 सभी तत्वों की प्रोटॉन की तुलना करें →
- न्यूट्रॉन
- 50 सभी तत्वों की न्यूट्रॉन की तुलना करें →
- ज्ञात समस्थानिक
- 35 सभी तत्वों की ज्ञात समस्थानिक की तुलना करें →
- स्थिर समस्थानिक
- 1 सभी तत्वों की स्थिर समस्थानिक की तुलना करें →
- सबसे स्थिर समस्थानिक
- Y-89
- खोज का वर्ष
- 1794
प्रचुरता
- प्रचुरता (भूपर्पटी)
- 33 mg/kg सभी तत्वों की प्रचुरता (भूपर्पटी) की तुलना करें →
- प्रचुरता (महासागर)
- 1.3 × 10−5 mg/L सभी तत्वों की प्रचुरता (महासागर) की तुलना करें →
क्रिस्टल संरचना
- जालक स्थिरांक a
- 365 pm
इलेक्ट्रॉनिक संरचना
- प्रति कोश इलेक्ट्रॉन
- 2, 8, 18, 9, 2 सभी तत्वों की प्रति कोश इलेक्ट्रॉन की तुलना करें →
पहचानकर्ता
- CAS संख्या
- 7440-65-5 सभी तत्वों की CAS संख्या की तुलना करें →
- टर्म प्रतीक
- 2D3/2
- InChI
- InChI=1S/Y
- InChI कुंजी
- VWQVUPCCIRVNHF-UHFFFAOYSA-N
इलेक्ट्रॉन विन्यास मापित
Y: 4d¹ 5s²[Kr] 4d¹ 5s²1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹ 5s²परमाणु मॉडल
समस्थानिक न्यूट्रॉन की संख्या, द्रव्यमान और स्थिरता बदलते हैं — उदासीन परमाणु का इलेक्ट्रॉन विन्यास नहीं।
सांकेतिक परमाणु मॉडल, वास्तविक अनुपात में नहीं।
परमाणु पहचान-चिह्न
उत्सर्जन / अवशोषण स्पेक्ट्रम
समस्थानिक वितरण
| द्रव्यमान संख्या | परमाणु द्रव्यमान (u) | प्राकृतिक प्रचुरता | अर्धायु |
|---|---|---|---|
| 89 स्थिर | 88.9058403 ± 0.0000024 | 100.0000% | स्थिर |
प्रावस्था / अवस्था
कारण: गलनांक (1521.85 °C) से 1496.8 °C कम
सांकेतिक, वास्तविक अनुपात में नहीं
प्रावस्था संक्रमण बिंदु
संक्रमण ऊर्जाएँ
गलनांक पर 1 mol को पिघलाने के लिए आवश्यक ऊर्जा
क्वथनांक पर 1 mol को वाष्पित करने के लिए आवश्यक ऊर्जा
ऊर्ध्वपातनांक पर 1 mol के ऊर्ध्वपातन के लिए आवश्यक ऊर्जा
घनत्व
मानक परिस्थितियों में
मानक परिस्थितियों में
परमाणु स्पेक्ट्रम
39 में से 10 दिखाए जा रहे हैं। आयन के आवेश के अनुसार आरोही क्रम में व्यवस्थित।
उपलब्ध स्पेक्ट्रमी रेखा डेटा ?
| आयन | आवेश | कुल रेखाएँ | संक्रमण प्रायिकताएँ | स्तर पदनाम |
|---|---|---|---|---|
| Y I | 0 | 361 | 189 | 351 |
| Y II | +1 | 116 | 66 | 116 |
| Y III | +2 | 113 | 0 | 0 |
| Y IV | +3 | 25 | 0 | 0 |
| Y V | +4 | 632 | 632 | 632 |
| Y VII | +6 | 168 | 168 | 168 |
| Y VIII | +7 | 70 | 70 | 70 |
उपलब्ध ऊर्जा स्तर डेटा ?
| आयन | आवेश | स्तर |
|---|---|---|
| Y I | 0 | 194 |
| Y II | +1 | 249 |
| Y III | +2 | 51 |
| Y IV | +3 | 130 |
| Y V | +4 | 114 |
| Y VI | +5 | 2 |
| Y VII | +6 | 57 |
| Y VIII | +7 | 33 |
| Y IX | +8 | 2 |
| Y X | +9 | 2 |
आयनिक त्रिज्याएँ
| आवेश | उपसहसंयोजन | प्रचक्रण | त्रिज्या |
|---|---|---|---|
| +3 | 6 | उपलब्ध नहीं | 90 pm |
| +3 | 7 | उपलब्ध नहीं | 96 pm |
| +3 | 8 | उपलब्ध नहीं | 101.89999999999999 pm |
| +3 | 9 | उपलब्ध नहीं | 107.5 pm |
यौगिक
समस्थानिक (1)
Natural yttrium contains one isotope, 89Y. Nineteen other unstable isotopes have been characterized.
| द्रव्यमान संख्या | परमाणु द्रव्यमान (u) | प्राकृतिक प्रचुरता | अर्धायु | क्षय का प्रकार | |
|---|---|---|---|---|---|
| 89 स्थिर | 88.9058403 ± 0.0000024 | 100.0000% | स्थिर | stable |
स्पेक्ट्रमी रेखाएँ
266 में से 50 दिखाए जा रहे हैं। डिफ़ॉल्ट रूप से केवल मापित तीव्रता वाली स्पेक्ट्रमी रेखाएँ दिखाई जाती हैं।
| तरंगदैर्घ्य (nm) | तीव्रता | आयनन अवस्था | प्रकार | संक्रमण | सटीकता | स्रोत | |
|---|---|---|---|---|---|---|---|
| 410.23691 nm | 9900 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(1D).5p y 2F* | मापित | NIST | |
| 407.735998 nm | 9400 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(1D).5p y 2F* | मापित | NIST | |
| 412.829876 nm | 8900 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(1D).5p y 2D* | मापित | NIST | |
| 414.28358 nm | 7500 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(1D).5p y 2D* | मापित | NIST | |
| 404.76281 nm | 2400 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(3D).5p y 2P* | मापित | NIST | |
| 416.750671 nm | 2400 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(1D).5p y 2F* | मापित | NIST | |
| 423.5934 nm | 2200 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(1D).5p y 2D* | मापित | NIST | |
| 408.37033 nm | 2000 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(3D).5p y 2P* | मापित | NIST | |
| 417.41339 nm | 2000 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(3D).5p y 2P* | मापित | NIST | |
| 464.368813 nm | 2000 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(3D).5p z 2F* | मापित | NIST | |
| 467.48486 nm | 2000 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(3D).5p z 2F* | मापित | NIST | |
| 619.17183 nm | 1200 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(3D).5p z 2D* | मापित | NIST | |
| 643.50036 nm | 1000 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(3D).5p z 2D* | मापित | NIST | |
| 403.982219 nm | 940 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(1D).5p y 2D* | मापित | NIST | |
| 452.72342 nm | 890 | Y I | emission | 4d2.(3F).5s a 4F → 4d2.(3F).5p y 4D* | मापित | NIST | |
| 483.9861 nm | 770 | Y I | emission | 4d2.(3F).5s a 4F → 4d2.(3F).5p y 4F* | मापित | NIST | |
| 552.75472 nm | 740 | Y I | emission | 4d2.(3F).5s a 4F → 4d2.(3F).5p z 4G* | मापित | NIST | |
| 546.6464 nm | 710 | Y I | emission | 4d2.(3F).5s a 4F → 4d2.(3F).5p z 4G* | मापित | NIST | |
| 558.18694 nm | 620 | Y I | emission | 4d2.(3F).5s a 4F → 4d2.(3F).5p z 4G* | मापित | NIST | |
| 563.01301 nm | 560 | Y I | emission | 4d2.(3F).5s a 4F → 4d2.(3F).5p z 4G* | मापित | NIST | |
| 484.56655 nm | 550 | Y I | emission | 4d2.(3F).5s a 4F → 4d2.(3F).5p y 4F* | मापित | NIST | |
| 450.59441 nm | 500 | Y I | emission | 4d2.(3F).5s a 4F → 4d2.(3F).5p y 4D* | मापित | NIST | |
| 452.77815 nm | 440 | Y I | emission | 4d2.(3F).5s a 4F → 4d2.(3F).5p y 4D* | मापित | NIST | |
| 476.09753 nm | 410 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(3D).5p z 2F* | मापित | NIST | |
| 485.26766 nm | 410 | Y I | emission | 4d2.(3F).5s a 4F → 4d2.(3F).5p y 4F* | मापित | NIST | |
| 485.98428 nm | 330 | Y I | emission | 4d2.(3F).5s a 4F → 4d2.(3F).5p y 4F* | मापित | NIST | |
| 425.11994 nm | 300 | Y I | emission | 4d.5s.(3D).5p z 4F* → 4d.5s.(3D).5d e 4G | मापित | NIST | |
| 448.74634 nm | 300 | Y I | emission | 4d2.(3F).5s a 4F → 4d2.(3F).5p y 4D* | मापित | NIST | |
| 550.3466 nm | 300 | Y I | emission | 4d2.(3F).5s a 2F → 4d2.(3F).5p x 2F* | मापित | NIST | |
| 622.25784 nm | 300 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(3D).5p z 2D* | मापित | NIST | |
| 543.82242 nm | 190 | Y I | emission | 4d2.(3F).5s a 2F → 4d2.(3F).5p x 2D* | मापित | NIST | |
| 546.62434 nm | 190 | Y I | emission | 4d.5s.(3D).5p z 4F* → 4d.5s.(3D).6s e 4D | मापित | NIST | |
| 679.37029 nm | 190 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(3D).5p z 4F* | मापित | NIST | |
| 524.08001 nm | 181 | Y I | emission | 4d2.(1G).5s a 2G → 4d2.(1G).5p z 2H* | मापित | NIST | |
| 447.69471 nm | 180 | Y I | emission | 4d2.(3F).5s a 4F → 4d2.(3F).5p x 2F* | मापित | NIST | |
| 469.67994 nm | 180 | Y I | emission | 4d2.(1D).5s b 2D → 4d2.(1D).5p w 2F* | मापित | NIST | |
| 479.92999 nm | 180 | Y I | emission | 4d2.(3F).5s a 4F → 4d2.(3F).5p y 4F* | मापित | NIST | |
| 513.51993 nm | 180 | Y I | emission | 4d2.(1G).5s a 2G → 4d2.(1G).5p z 2H* | मापित | NIST | |
| 557.74153 nm | 180 | Y I | emission | 4d2.(3F).5s a 2F → 4d2.(3F).5p z 2G* | मापित | NIST | |
| 447.57178 nm | 170 | Y I | emission | 4d2.(3F).5s a 4F → 4d2.(3F).5p y 4D* | मापित | NIST | |
| 472.8516 nm | 170 | Y I | emission | 5s2.5p z 2P* → 5s2.6s e 2S | मापित | NIST | |
| 478.68762 nm | 170 | Y I | emission | 4d2.(3P).5s a 4P → 4d2.(3P).5p x 4D* | मापित | NIST | |
| 421.77985 nm | 160 | Y I | emission | 5s2.5p z 2P* → 5s2.(2D).5d e 2D | मापित | NIST | |
| 447.74436 nm | 160 | Y I | emission | 4d2.(3F).5s a 4F → 4d2.(3F).5p y 4D* | मापित | NIST | |
| 475.2787 nm | 160 | Y I | emission | 4d2.(3F).5s a 2F → 4d2.(3P).5p x 4D* | मापित | NIST | |
| 570.67133 nm | 160 | Y I | emission | 4d.5s.(3D).5p z 4F* → 4d.5s.(3D).6s e 4D | मापित | NIST | |
| 492.18769 nm | 150 | Y I | emission | 5s2.5p z 2P* → 5s2.6s e 2S | मापित | NIST | |
| 613.84349 nm | 150 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(3D).5p z 4D* | मापित | NIST | |
| 668.75669 nm | 150 | Y I | emission | 4d.5s2 a 2D → 4d.5s.(3D).5p z 4F* | मापित | NIST | |
| 465.37837 nm | 140 | Y I | emission | 4d2.(1D).5s b 2D → 4d2.(3P).5p y 4P* | मापित | NIST |
विस्तृत गुण
सहसंयोजक त्रिज्याएँ (विस्तृत)
- सहसंयोजक त्रिज्या (प्यूक्को)
- 163 pm
- सहसंयोजक त्रिज्या (प्यूक्को, द्विबंध)
- 130 pm
- सहसंयोजक त्रिज्या (प्यूक्को, त्रिबंध)
- 124 pm
वान डर वाल्स त्रिज्याएँ
- Batsanov
- 240 pm
- Alvarez
- 275 pm
- UFF
- 334.5 pm
- MM3
- 271 pm
परमाणु और धात्विक त्रिज्याएँ
- परमाणु त्रिज्या (राह्म)
- 274 pm
- धात्विक त्रिज्या (C12)
- 180 pm
संख्यांकन मापक्रम
- Mendeleev
- 12
- Pettifor
- 19
- Glawe
- 21
विद्युतऋणात्मकता मापक्रम
- Ghosh
- 0
- Miedema
- 3
- Gunnarsson–Lundqvist
- 3
- Robles–Bartolotti
- 3
ध्रुवणीयता और परिक्षेपण
- द्विध्रुव ध्रुवणीयता
- 162 a.u.
- द्विध्रुव ध्रुवणीयता (अनिश्चितता)
- 12 a.u.
- C₆ (Gould–Bučko)
- 2600 Ha·Bohr6
रासायनिक बंधुता
- प्रोटॉन बंधुता
- 967 kJ/mol
- गैसीय क्षारकता
- 945.9 kJ/mol
मीडेमा प्राचल
- मीडेमा मोलर आयतन
- 19.9 cm3/mol
- मीडेमा इलेक्ट्रॉन घनत्व
- 2
आपूर्ति जोखिम और अर्थशास्त्र
- उत्पादन संकेंद्रण
- 97
- सापेक्ष आपूर्ति जोखिम
- 10
- भंडार वितरण
- 50
- राजनीतिक स्थिरता (प्रमुख उत्पादक)
- 24
- राजनीतिक स्थिरता (सबसे अधिक भंडार वाला देश)
- 24
प्रावस्था संक्रमण और अपररूप
| गलनांक | 1795.15 K |
| क्वथनांक | 3618.15 K |
ऑक्सीकरण अवस्था की श्रेणियाँ
उन्नत संदर्भ डेटा
परिरक्षण स्थिरांक (10)
| n | कक्षक | σ |
|---|---|---|
| 1 | s | 0.8244 |
| 2 | p | 3.9968 |
| 2 | s | 10.3778 |
| 3 | d | 13.6029 |
| 3 | p | 15.9075 |
| 3 | s | 15.4485 |
| 4 | d | 23.0416 |
| 4 | p | 26.2544 |
| 4 | s | 24.7364 |
| 5 | s | 32.744 |
क्रिस्टल त्रिज्याओं का विवरण (4)
| आवेश | CN | प्रचक्रण | rcrystal (pm) | उत्पत्ति |
|---|---|---|---|---|
| 3 | VI | 104 | from r^3 vs V plots, | |
| 3 | VII | 110 | ||
| 3 | VIII | 115.9 | from r^3 vs V plots, | |
| 3 | IX | 121.5 | from r^3 vs V plots, |
समस्थानिक क्षय के प्रकार (60)
| समस्थानिक | मोड | तीव्रता |
|---|---|---|
| 75 | B+ | — |
| 75 | B+p | — |
| 75 | p | — |
| 76 | B+ | — |
| 76 | p | — |
| 76 | B+p | — |
| 77 | B+ | 100% |
| 77 | B+p | — |
| 77 | p | — |
| 78 | B+ | 100% |
एक्स-रे प्रकीर्णन गुणक (619)
| ऊर्जा (eV) | f₁ | f₂ |
|---|---|---|
| 10 | — | 2.26036 |
| 10.1617 | — | 2.25621 |
| 10.3261 | — | 2.25207 |
| 10.4931 | — | 2.24793 |
| 10.6628 | — | 2.2438 |
| 10.8353 | — | 2.23968 |
| 11.0105 | — | 2.23344 |
| 11.1886 | — | 2.21122 |
| 11.3696 | — | 2.18921 |
| 11.5535 | — | 2.16742 |
अतिरिक्त डेटा
Estimated Crustal Abundance
The estimated element abundance in the earth's crust.
3.3×101 milligrams per kilogram
संदर्भ (1)
Estimated Oceanic Abundance
The estimated element abundance in the earth's oceans.
1.3×10-5 milligrams per liter
संदर्भ (1)
Sources
Sources of this element.
Yttrium occurs in nearly all of the rare-earth minerals. Analysis of lunar rock samples obtained during the Apollo missions show a relatively high yttrium content.
It is recovered commercially from monazite sand, which contains about 3%, and from bastnasite, which contains about 0.2%. Wohler obtained the impure element in 1828 by reduction of the anhydrous chloride with potassium. The metal is now produced commercially by reduction of the fluoride with calcium metal. It can also be prepared by other techniques.
संदर्भ (1)
- [6] Yttrium https://periodic.lanl.gov/39.shtml
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 Yttrium.
The element property data was retrieved from publications.