The experimental apparatus for electrical resistivity measurements of liquid metals and alloys under microgravity due to the launch of a rocket

Masaki, T. ; Itami, T. ; Kuribayashi, K. ; Hinada, M. ; Kawasaki, K.

[S.l.] : American Institute of Physics (AIP)
Published 1996
ISSN:
1089-7623
Source:
AIP Digital Archive
Topics:
Physics
Electrical Engineering, Measurement and Control Technology
Notes:
The experimental apparatus was developed for electrical resistivity measurements of liquid metals and alloys under microgravity due to the launch of rocket; whole assembly, contained in the small space of 360 mm(length)×360 mm(width)×97 mm(height), was composed of the cell box, the electronic circuit box, and the battery box. The cell for electrical resistivity measurements due to the dc four probe method was made of Ti metal because of its strength and no reaction to corrosive liquid alloys at high temperatures. The application of this method was made successfully to the measurement of electrical resistivity for liquid Bi–Ga alloys with critical mixing both under gravity condition and under microgravity condition due to the launch of the rocket. The far larger temperature coefficients of resistivity were observed near the critical point. This may indicate the appearance of larger concentration fluctuations under microgravity. © 1996 American Institute of Physics.
Type of Medium:
Electronic Resource
URL:
_version_ 1798289699291267072
autor Masaki, T.
Itami, T.
Kuribayashi, K.
Hinada, M.
Kawasaki, K.
autorsonst Masaki, T.
Itami, T.
Kuribayashi, K.
Hinada, M.
Kawasaki, K.
book_url http://dx.doi.org/10.1063/1.1146940
datenlieferant nat_lic_papers
hauptsatz hsatz_simple
identnr NLZ219444765
issn 1089-7623
journal_name Review of Scientific Instruments
materialart 1
notes The experimental apparatus was developed for electrical resistivity measurements of liquid metals and alloys under microgravity due to the launch of rocket; whole assembly, contained in the small space of 360 mm(length)×360 mm(width)×97 mm(height), was composed of the cell box, the electronic circuit box, and the battery box. The cell for electrical resistivity measurements due to the dc four probe method was made of Ti metal because of its strength and no reaction to corrosive liquid alloys at high temperatures. The application of this method was made successfully to the measurement of electrical resistivity for liquid Bi–Ga alloys with critical mixing both under gravity condition and under microgravity condition due to the launch of the rocket. The far larger temperature coefficients of resistivity were observed near the critical point. This may indicate the appearance of larger concentration fluctuations under microgravity. © 1996 American Institute of Physics.
package_name American Institute of Physics (AIP)
publikationsjahr_anzeige 1996
publikationsjahr_facette 1996
publikationsjahr_intervall 8004:1995-1999
publikationsjahr_sort 1996
publikationsort [S.l.]
publisher American Institute of Physics (AIP)
reference 67 (1996), S. 2325-2331
search_space articles
shingle_author_1 Masaki, T.
Itami, T.
Kuribayashi, K.
Hinada, M.
Kawasaki, K.
shingle_author_2 Masaki, T.
Itami, T.
Kuribayashi, K.
Hinada, M.
Kawasaki, K.
shingle_author_3 Masaki, T.
Itami, T.
Kuribayashi, K.
Hinada, M.
Kawasaki, K.
shingle_author_4 Masaki, T.
Itami, T.
Kuribayashi, K.
Hinada, M.
Kawasaki, K.
shingle_catch_all_1 Masaki, T.
Itami, T.
Kuribayashi, K.
Hinada, M.
Kawasaki, K.
The experimental apparatus for electrical resistivity measurements of liquid metals and alloys under microgravity due to the launch of a rocket
The experimental apparatus was developed for electrical resistivity measurements of liquid metals and alloys under microgravity due to the launch of rocket; whole assembly, contained in the small space of 360 mm(length)×360 mm(width)×97 mm(height), was composed of the cell box, the electronic circuit box, and the battery box. The cell for electrical resistivity measurements due to the dc four probe method was made of Ti metal because of its strength and no reaction to corrosive liquid alloys at high temperatures. The application of this method was made successfully to the measurement of electrical resistivity for liquid Bi–Ga alloys with critical mixing both under gravity condition and under microgravity condition due to the launch of the rocket. The far larger temperature coefficients of resistivity were observed near the critical point. This may indicate the appearance of larger concentration fluctuations under microgravity. © 1996 American Institute of Physics.
1089-7623
10897623
American Institute of Physics (AIP)
shingle_catch_all_2 Masaki, T.
Itami, T.
Kuribayashi, K.
Hinada, M.
Kawasaki, K.
The experimental apparatus for electrical resistivity measurements of liquid metals and alloys under microgravity due to the launch of a rocket
The experimental apparatus was developed for electrical resistivity measurements of liquid metals and alloys under microgravity due to the launch of rocket; whole assembly, contained in the small space of 360 mm(length)×360 mm(width)×97 mm(height), was composed of the cell box, the electronic circuit box, and the battery box. The cell for electrical resistivity measurements due to the dc four probe method was made of Ti metal because of its strength and no reaction to corrosive liquid alloys at high temperatures. The application of this method was made successfully to the measurement of electrical resistivity for liquid Bi–Ga alloys with critical mixing both under gravity condition and under microgravity condition due to the launch of the rocket. The far larger temperature coefficients of resistivity were observed near the critical point. This may indicate the appearance of larger concentration fluctuations under microgravity. © 1996 American Institute of Physics.
1089-7623
10897623
American Institute of Physics (AIP)
shingle_catch_all_3 Masaki, T.
Itami, T.
Kuribayashi, K.
Hinada, M.
Kawasaki, K.
The experimental apparatus for electrical resistivity measurements of liquid metals and alloys under microgravity due to the launch of a rocket
The experimental apparatus was developed for electrical resistivity measurements of liquid metals and alloys under microgravity due to the launch of rocket; whole assembly, contained in the small space of 360 mm(length)×360 mm(width)×97 mm(height), was composed of the cell box, the electronic circuit box, and the battery box. The cell for electrical resistivity measurements due to the dc four probe method was made of Ti metal because of its strength and no reaction to corrosive liquid alloys at high temperatures. The application of this method was made successfully to the measurement of electrical resistivity for liquid Bi–Ga alloys with critical mixing both under gravity condition and under microgravity condition due to the launch of the rocket. The far larger temperature coefficients of resistivity were observed near the critical point. This may indicate the appearance of larger concentration fluctuations under microgravity. © 1996 American Institute of Physics.
1089-7623
10897623
American Institute of Physics (AIP)
shingle_catch_all_4 Masaki, T.
Itami, T.
Kuribayashi, K.
Hinada, M.
Kawasaki, K.
The experimental apparatus for electrical resistivity measurements of liquid metals and alloys under microgravity due to the launch of a rocket
The experimental apparatus was developed for electrical resistivity measurements of liquid metals and alloys under microgravity due to the launch of rocket; whole assembly, contained in the small space of 360 mm(length)×360 mm(width)×97 mm(height), was composed of the cell box, the electronic circuit box, and the battery box. The cell for electrical resistivity measurements due to the dc four probe method was made of Ti metal because of its strength and no reaction to corrosive liquid alloys at high temperatures. The application of this method was made successfully to the measurement of electrical resistivity for liquid Bi–Ga alloys with critical mixing both under gravity condition and under microgravity condition due to the launch of the rocket. The far larger temperature coefficients of resistivity were observed near the critical point. This may indicate the appearance of larger concentration fluctuations under microgravity. © 1996 American Institute of Physics.
1089-7623
10897623
American Institute of Physics (AIP)
shingle_title_1 The experimental apparatus for electrical resistivity measurements of liquid metals and alloys under microgravity due to the launch of a rocket
shingle_title_2 The experimental apparatus for electrical resistivity measurements of liquid metals and alloys under microgravity due to the launch of a rocket
shingle_title_3 The experimental apparatus for electrical resistivity measurements of liquid metals and alloys under microgravity due to the launch of a rocket
shingle_title_4 The experimental apparatus for electrical resistivity measurements of liquid metals and alloys under microgravity due to the launch of a rocket
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timestamp 2024-05-06T08:04:59.487Z
titel The experimental apparatus for electrical resistivity measurements of liquid metals and alloys under microgravity due to the launch of a rocket
titel_suche The experimental apparatus for electrical resistivity measurements of liquid metals and alloys under microgravity due to the launch of a rocket
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