Effect of capillary pressure in nanobubbles on their adhesion to particles under foam flotation. Part 3
The energy possibility of the transition of free bubbles A to adherent bubbles M , or the A → M (TAM) transition, is calculated on substrates with different wetting abilities: extremely hydrophilic (Φ), extremely hydrophobic (Γ), and with incomplete wetting ability ( H x ), where x is the substrate...
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creator | Melik-Gaikazyan, V. I. Emel’yanova, N. P. Dolzhenkov, D. V. |
description | The energy possibility of the transition of free bubbles
A
to adherent bubbles
M
, or the
A
→
M
(TAM) transition, is calculated on substrates with different wetting abilities: extremely hydrophilic (Φ), extremely hydrophobic (Γ), and with incomplete wetting ability (
H
x
), where
x
is the substrate surface fraction covered by a monolayer of collector molecules). Calculations of TAM for bubbles with a diameter (
d
e
) of 2 mm to 20 nm on Φ, Γ, and
H
x
substrates showed that the change in specific energy (Δ
G
/
V
) in a bubble in the case of TAM depends on the value of
d
e
, substrate wetting ability, and surface area of its contact with the bubble. According to the results of studies, high capillary pressure (
P
c
) in nanobubbles
M
promotes their instantaneous spreading over the substrate. Herewith,
P
c
decreases considerably. The adhesion and spreading processes occur as a single process, irreversibly, one-way, and fast, because they are not complicated by counterprocesses. Upon a decrease in equatorial diameter
d
e
and wetting ability of the substrate, the decrease in
G
/
V
reaches several million J/m
3
. The actual simultaneity of the processes of bubble adhesion and spreading is illustrated by microphotographs of larger bubbles with a luminescent apolar reagent eliminating the effect of wetting hysteresis that is easily overcome in nanobubbles in the case of high
P
c
values. |
doi_str_mv | 10.3103/S1067821214040117 |
format | Article |
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A
to adherent bubbles
M
, or the
A
→
M
(TAM) transition, is calculated on substrates with different wetting abilities: extremely hydrophilic (Φ), extremely hydrophobic (Γ), and with incomplete wetting ability (
H
x
), where
x
is the substrate surface fraction covered by a monolayer of collector molecules). Calculations of TAM for bubbles with a diameter (
d
e
) of 2 mm to 20 nm on Φ, Γ, and
H
x
substrates showed that the change in specific energy (Δ
G
/
V
) in a bubble in the case of TAM depends on the value of
d
e
, substrate wetting ability, and surface area of its contact with the bubble. According to the results of studies, high capillary pressure (
P
c
) in nanobubbles
M
promotes their instantaneous spreading over the substrate. Herewith,
P
c
decreases considerably. The adhesion and spreading processes occur as a single process, irreversibly, one-way, and fast, because they are not complicated by counterprocesses. Upon a decrease in equatorial diameter
d
e
and wetting ability of the substrate, the decrease in
G
/
V
reaches several million J/m
3
. The actual simultaneity of the processes of bubble adhesion and spreading is illustrated by microphotographs of larger bubbles with a luminescent apolar reagent eliminating the effect of wetting hysteresis that is easily overcome in nanobubbles in the case of high
P
c
values.</description><identifier>ISSN: 1067-8212</identifier><identifier>EISSN: 1934-970X</identifier><identifier>DOI: 10.3103/S1067821214040117</identifier><language>eng</language><publisher>Heidelberg: Allerton Press</publisher><subject>Adhesion ; Bubbles ; Chemistry and Materials Science ; Materials Science ; Mathematical analysis ; Metallic Materials ; Microphotographs ; Mineral Processing of Nonferrous Metals ; Nanostructure ; Nonferrous metals ; Spreading ; Wetting</subject><ispartof>Russian journal of non-ferrous metals, 2014-07, Vol.55 (4), p.309-317</ispartof><rights>Allerton Press, Inc. 2014</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c349t-59e435bc73045806479f51073a75b3c493d42b6e6b04c4d9c95737e39f514ab83</citedby></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.3103/S1067821214040117$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.3103/S1067821214040117$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,780,784,27924,27925,41488,42557,51319</link.rule.ids></links><search><creatorcontrib>Melik-Gaikazyan, V. I.</creatorcontrib><creatorcontrib>Emel’yanova, N. P.</creatorcontrib><creatorcontrib>Dolzhenkov, D. V.</creatorcontrib><title>Effect of capillary pressure in nanobubbles on their adhesion to particles under foam flotation. Part 3</title><title>Russian journal of non-ferrous metals</title><addtitle>Russ. J. Non-ferrous Metals</addtitle><description>The energy possibility of the transition of free bubbles
A
to adherent bubbles
M
, or the
A
→
M
(TAM) transition, is calculated on substrates with different wetting abilities: extremely hydrophilic (Φ), extremely hydrophobic (Γ), and with incomplete wetting ability (
H
x
), where
x
is the substrate surface fraction covered by a monolayer of collector molecules). Calculations of TAM for bubbles with a diameter (
d
e
) of 2 mm to 20 nm on Φ, Γ, and
H
x
substrates showed that the change in specific energy (Δ
G
/
V
) in a bubble in the case of TAM depends on the value of
d
e
, substrate wetting ability, and surface area of its contact with the bubble. According to the results of studies, high capillary pressure (
P
c
) in nanobubbles
M
promotes their instantaneous spreading over the substrate. Herewith,
P
c
decreases considerably. The adhesion and spreading processes occur as a single process, irreversibly, one-way, and fast, because they are not complicated by counterprocesses. Upon a decrease in equatorial diameter
d
e
and wetting ability of the substrate, the decrease in
G
/
V
reaches several million J/m
3
. The actual simultaneity of the processes of bubble adhesion and spreading is illustrated by microphotographs of larger bubbles with a luminescent apolar reagent eliminating the effect of wetting hysteresis that is easily overcome in nanobubbles in the case of high
P
c
values.</description><subject>Adhesion</subject><subject>Bubbles</subject><subject>Chemistry and Materials Science</subject><subject>Materials Science</subject><subject>Mathematical analysis</subject><subject>Metallic Materials</subject><subject>Microphotographs</subject><subject>Mineral Processing of Nonferrous Metals</subject><subject>Nanostructure</subject><subject>Nonferrous metals</subject><subject>Spreading</subject><subject>Wetting</subject><issn>1067-8212</issn><issn>1934-970X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNp1kE9LAzEQxYMoWKsfwFvAi5etySbZNEcp9Q8UFFTwtiTppN2yTdZk9-C3N0s9iOJpZni_N8w8hC4pmTFK2M0LJZWcl7SknHBCqTxCE6oYL5Qk78e5z3Ix6qfoLKUdIUIooSZos3QObI-Dw1Z3Tdvq-Im7CCkNEXDjsdc-mMGYFhIOHvdbaCLW6y2kZhwD7nTsGzvKg19DxC7oPXZt6HWfiRl-zjpm5-jE6TbBxXedore75evioVg93T8ubleFZVz1hVDAmTBWMsLFnFRcKicokUxLYZjliq15aSqoDOGWr5VVQjIJbKS4NnM2RdeHvV0MHwOkvt43yUL-y0MYUk2rkhCmcioZvfqF7sIQfb6upiJjUspqpOiBsjGkFMHVXWz2OaWaknqMvv4TffaUB0_KrN9A_LH5X9MX-2GD9A</recordid><startdate>20140701</startdate><enddate>20140701</enddate><creator>Melik-Gaikazyan, V. I.</creator><creator>Emel’yanova, N. P.</creator><creator>Dolzhenkov, D. V.</creator><general>Allerton Press</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>20140701</creationdate><title>Effect of capillary pressure in nanobubbles on their adhesion to particles under foam flotation. Part 3</title><author>Melik-Gaikazyan, V. I. ; Emel’yanova, N. P. ; Dolzhenkov, D. V.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c349t-59e435bc73045806479f51073a75b3c493d42b6e6b04c4d9c95737e39f514ab83</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>Adhesion</topic><topic>Bubbles</topic><topic>Chemistry and Materials Science</topic><topic>Materials Science</topic><topic>Mathematical analysis</topic><topic>Metallic Materials</topic><topic>Microphotographs</topic><topic>Mineral Processing of Nonferrous Metals</topic><topic>Nanostructure</topic><topic>Nonferrous metals</topic><topic>Spreading</topic><topic>Wetting</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Melik-Gaikazyan, V. I.</creatorcontrib><creatorcontrib>Emel’yanova, N. P.</creatorcontrib><creatorcontrib>Dolzhenkov, D. V.</creatorcontrib><collection>CrossRef</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Russian journal of non-ferrous metals</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Melik-Gaikazyan, V. I.</au><au>Emel’yanova, N. P.</au><au>Dolzhenkov, D. V.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Effect of capillary pressure in nanobubbles on their adhesion to particles under foam flotation. Part 3</atitle><jtitle>Russian journal of non-ferrous metals</jtitle><stitle>Russ. J. Non-ferrous Metals</stitle><date>2014-07-01</date><risdate>2014</risdate><volume>55</volume><issue>4</issue><spage>309</spage><epage>317</epage><pages>309-317</pages><issn>1067-8212</issn><eissn>1934-970X</eissn><abstract>The energy possibility of the transition of free bubbles
A
to adherent bubbles
M
, or the
A
→
M
(TAM) transition, is calculated on substrates with different wetting abilities: extremely hydrophilic (Φ), extremely hydrophobic (Γ), and with incomplete wetting ability (
H
x
), where
x
is the substrate surface fraction covered by a monolayer of collector molecules). Calculations of TAM for bubbles with a diameter (
d
e
) of 2 mm to 20 nm on Φ, Γ, and
H
x
substrates showed that the change in specific energy (Δ
G
/
V
) in a bubble in the case of TAM depends on the value of
d
e
, substrate wetting ability, and surface area of its contact with the bubble. According to the results of studies, high capillary pressure (
P
c
) in nanobubbles
M
promotes their instantaneous spreading over the substrate. Herewith,
P
c
decreases considerably. The adhesion and spreading processes occur as a single process, irreversibly, one-way, and fast, because they are not complicated by counterprocesses. Upon a decrease in equatorial diameter
d
e
and wetting ability of the substrate, the decrease in
G
/
V
reaches several million J/m
3
. The actual simultaneity of the processes of bubble adhesion and spreading is illustrated by microphotographs of larger bubbles with a luminescent apolar reagent eliminating the effect of wetting hysteresis that is easily overcome in nanobubbles in the case of high
P
c
values.</abstract><cop>Heidelberg</cop><pub>Allerton Press</pub><doi>10.3103/S1067821214040117</doi><tpages>9</tpages></addata></record> |
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issn | 1067-8212 1934-970X |
language | eng |
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source | SpringerNature Complete Journals |
subjects | Adhesion Bubbles Chemistry and Materials Science Materials Science Mathematical analysis Metallic Materials Microphotographs Mineral Processing of Nonferrous Metals Nanostructure Nonferrous metals Spreading Wetting |
title | Effect of capillary pressure in nanobubbles on their adhesion to particles under foam flotation. Part 3 |
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