Physical properties of liquid and undercooled tungsten by levitation techniques
Maintaining deep undercooling melts represents a formidable challenge when dealing with tungsten due to its high vapor pressure, its melting temperature ( T m = 3695 K ) , and the risk of contamination. Using electrostatic levitation, properties of liquid tungsten were measured above the melting tem...
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Veröffentlicht in: | Applied physics letters 2005-01, Vol.86 (4), p.041901-041901-3 |
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creator | Paradis, Paul-François Ishikawa, Takehiko Fujii, Ryuichi Yoda, Shinichi |
description | Maintaining deep undercooling melts represents a formidable challenge when dealing with tungsten due to its high vapor pressure, its melting temperature
(
T
m
=
3695
K
)
, and the risk of contamination. Using electrostatic levitation, properties of liquid tungsten were measured above the melting temperature as well as in the undercooled phase. Over the
3125
-
3710
K
interval, the density was measured as
ρ
(
T
)
=
1.67
×
10
4
−
1.08
(
T
−
T
m
)
kg
m
−
3
. Similarly, the surface tension was measured as
σ
(
T
)
=
2.478
×
10
3
−
0.31
(
T
−
T
m
)
over the
3360
-
3700
K
range. At
T
m
, the data agree well with the literature values. The excellent processing conditions also offer opportunities to achieve reproducible and controlled formation of metastable phases. |
doi_str_mv | 10.1063/1.1853513 |
format | Article |
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(
T
m
=
3695
K
)
, and the risk of contamination. Using electrostatic levitation, properties of liquid tungsten were measured above the melting temperature as well as in the undercooled phase. Over the
3125
-
3710
K
interval, the density was measured as
ρ
(
T
)
=
1.67
×
10
4
−
1.08
(
T
−
T
m
)
kg
m
−
3
. Similarly, the surface tension was measured as
σ
(
T
)
=
2.478
×
10
3
−
0.31
(
T
−
T
m
)
over the
3360
-
3700
K
range. At
T
m
, the data agree well with the literature values. The excellent processing conditions also offer opportunities to achieve reproducible and controlled formation of metastable phases.</description><identifier>ISSN: 0003-6951</identifier><identifier>EISSN: 1077-3118</identifier><identifier>DOI: 10.1063/1.1853513</identifier><identifier>CODEN: APPLAB</identifier><language>eng</language><publisher>American Institute of Physics</publisher><ispartof>Applied physics letters, 2005-01, Vol.86 (4), p.041901-041901-3</ispartof><rights>2005 American Institute of Physics</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c283t-58b1a1a69c0c7a9e9b615fc76623dfc93aa5d3c2fff1b7d0b0847a6228674cab3</citedby><cites>FETCH-LOGICAL-c283t-58b1a1a69c0c7a9e9b615fc76623dfc93aa5d3c2fff1b7d0b0847a6228674cab3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/apl/article-lookup/doi/10.1063/1.1853513$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>314,780,784,794,1558,4502,27915,27916,76145,76151</link.rule.ids></links><search><creatorcontrib>Paradis, Paul-François</creatorcontrib><creatorcontrib>Ishikawa, Takehiko</creatorcontrib><creatorcontrib>Fujii, Ryuichi</creatorcontrib><creatorcontrib>Yoda, Shinichi</creatorcontrib><title>Physical properties of liquid and undercooled tungsten by levitation techniques</title><title>Applied physics letters</title><description>Maintaining deep undercooling melts represents a formidable challenge when dealing with tungsten due to its high vapor pressure, its melting temperature
(
T
m
=
3695
K
)
, and the risk of contamination. Using electrostatic levitation, properties of liquid tungsten were measured above the melting temperature as well as in the undercooled phase. Over the
3125
-
3710
K
interval, the density was measured as
ρ
(
T
)
=
1.67
×
10
4
−
1.08
(
T
−
T
m
)
kg
m
−
3
. Similarly, the surface tension was measured as
σ
(
T
)
=
2.478
×
10
3
−
0.31
(
T
−
T
m
)
over the
3360
-
3700
K
range. At
T
m
, the data agree well with the literature values. The excellent processing conditions also offer opportunities to achieve reproducible and controlled formation of metastable phases.</description><issn>0003-6951</issn><issn>1077-3118</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2005</creationdate><recordtype>article</recordtype><recordid>eNp1kEtLxDAUhYMoWEcX_oNsXXTM7Z0k7cKFDL5gYFzouqR5OJHajkkq9N9bmYorV5cD3zlcPkIugS2BCbyGJZQcOeARyYBJmSNAeUwyxhjmouJwSs5ifJ8iLxAzsn3ejdFr1dJ96Pc2JG8j7R1t_efgDVWdoUNnbNB931pD09C9xWQ72oy0tV8-qeT7jiard93UsPGcnDjVRnsx3wV5vb97WT_mm-3D0_p2k-uixJTzsgEFSlSaaakqWzUCuNNSiAKN0xUqxQ3qwjkHjTSsYeVKKlEUpZArrRpckKvDrg59jMG6eh_8hwpjDaz-MVFDPZuY2JsDG_X88P_wr476Twd-A1cyZ24</recordid><startdate>20050124</startdate><enddate>20050124</enddate><creator>Paradis, Paul-François</creator><creator>Ishikawa, Takehiko</creator><creator>Fujii, Ryuichi</creator><creator>Yoda, Shinichi</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20050124</creationdate><title>Physical properties of liquid and undercooled tungsten by levitation techniques</title><author>Paradis, Paul-François ; Ishikawa, Takehiko ; Fujii, Ryuichi ; Yoda, Shinichi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c283t-58b1a1a69c0c7a9e9b615fc76623dfc93aa5d3c2fff1b7d0b0847a6228674cab3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2005</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Paradis, Paul-François</creatorcontrib><creatorcontrib>Ishikawa, Takehiko</creatorcontrib><creatorcontrib>Fujii, Ryuichi</creatorcontrib><creatorcontrib>Yoda, Shinichi</creatorcontrib><collection>CrossRef</collection><jtitle>Applied physics letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Paradis, Paul-François</au><au>Ishikawa, Takehiko</au><au>Fujii, Ryuichi</au><au>Yoda, Shinichi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Physical properties of liquid and undercooled tungsten by levitation techniques</atitle><jtitle>Applied physics letters</jtitle><date>2005-01-24</date><risdate>2005</risdate><volume>86</volume><issue>4</issue><spage>041901</spage><epage>041901-3</epage><pages>041901-041901-3</pages><issn>0003-6951</issn><eissn>1077-3118</eissn><coden>APPLAB</coden><abstract>Maintaining deep undercooling melts represents a formidable challenge when dealing with tungsten due to its high vapor pressure, its melting temperature
(
T
m
=
3695
K
)
, and the risk of contamination. Using electrostatic levitation, properties of liquid tungsten were measured above the melting temperature as well as in the undercooled phase. Over the
3125
-
3710
K
interval, the density was measured as
ρ
(
T
)
=
1.67
×
10
4
−
1.08
(
T
−
T
m
)
kg
m
−
3
. Similarly, the surface tension was measured as
σ
(
T
)
=
2.478
×
10
3
−
0.31
(
T
−
T
m
)
over the
3360
-
3700
K
range. At
T
m
, the data agree well with the literature values. The excellent processing conditions also offer opportunities to achieve reproducible and controlled formation of metastable phases.</abstract><pub>American Institute of Physics</pub><doi>10.1063/1.1853513</doi></addata></record> |
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identifier | ISSN: 0003-6951 |
ispartof | Applied physics letters, 2005-01, Vol.86 (4), p.041901-041901-3 |
issn | 0003-6951 1077-3118 |
language | eng |
recordid | cdi_crossref_primary_10_1063_1_1853513 |
source | AIP Journals Complete; AIP Digital Archive |
title | Physical properties of liquid and undercooled tungsten by levitation techniques |
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