LrgpV1, PascalFrancis, Curation, bibRecord, 000960

A mass conservative approach to model the ultrasonic de-agglomeration of ZnO nanoparticle suspension in water

Identifieur interne : 000960 ( PascalFrancis/Curation ); précédent : 000959; suivant : 000961

A mass conservative approach to model the ultrasonic de-agglomeration of ZnO nanoparticle suspension in water

Auteurs : J.-P. Guillemin [France] ; E. Schaer [France] ; P. Marchal [France] ; C. Lemaitre [France] ; H. Nonnet [France] ; A. Ledieu [France]

Source :

Powder technology [ 0032-5910 ] ; 2012.

RBID : Pascal:12-0170340

Descripteurs français

Pascal (Inist)
- Modélisation, Agglomération, Nanoparticule, Densité, Diffusion lumière, Distribution masse, Dimension fractale, Méthode discrétisation, Fragmentation, Dispersion, Distribution dimension particule, Bulle cavitation, Ultrason, Consommation énergie, Puissance thermique.
Wicri :
- topic : Agglomération.

English descriptors

KwdEn :
- Agglomeration, Cavitation bubble, Density, Discretization method, Dispersion, Energy consumption, Fractal dimension, Fragmentation, Light scattering, Mass distribution, Modeling, Nanoparticle, Particle size distribution, Thermal power, Ultrasound.

Abstract

This paper deals with the non conservation of volume during ultrasonic breakage of ZnO particles whose density varies against size. The observed volumetric particle distributions, obtained by light scattering measurements, are transformed into mass distributions using an expression of the density variation against size based on the fractal dimension. Calculations are then performed using a discretization method given in literature. To validate calculated results, ultrasonic fragmentation of zinc dioxide nanopowder in water is performed in cell dispersion to follow the evolution of the particle size distribution against time. Furthermore, calculated results are adjusted to the experimental particle size distribution curves to determine the breakage frequency constant. This parameter varies with the energy released by the collapse of the cavitation bubbles. Most work on mechanisms of fragmentation by ultrasound is based on the electrical power consumption required for the dispersion of agglomerate. Here, the study focuses on the thermal power which is correlated to the breakage frequency constant. Finally it is found that this parameter is also function of the square root of the thermal power.

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A02	`01`			`@0 POTEBX`
A03		`1`		`@0 Powder technol.`
A05				`@2 219`
A08	`01`	`1`	`ENG`	`@1 A mass conservative approach to model the ultrasonic de-agglomeration of ZnO nanoparticle suspension in water`
A11	`01`	`1`		`@1 GUILLEMIN (J.-P.)`
A11	`02`	`1`		`@1 SCHAER (E.)`
A11	`03`	`1`		`@1 MARCHAL (P.)`
A11	`04`	`1`		`@1 LEMAITRE (C.)`
A11	`05`	`1`		`@1 NONNET (H.)`
A11	`06`	`1`		`@1 LEDIEU (A.)`
A14	`01`			`@1 Davey Bickford, le Moulin Gaspard @2 89550 Héry @3 FRA @Z 1 aut.`
A14	`02`			`@1 CEA, DEN, DTCD, SECM, Laboratoire d'étude et développement de matrices de conditionnement - Centre de Marcoule - BP 17171 @2 30207 Bagnols-sur-Cèze @3 FRA @Z 5 aut. @Z 6 aut.`
A14	`03`			`@1 Laboratoire de Réaction et de Genie des Procédé, GEMICO/LRGP/ENSIC (CNRS UPR3349), 1 rue Grandville - BP 20451 @2 54001 Nancy @3 FRA @Z 2 aut. @Z 3 aut. @Z 4 aut.`
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A21				`@1 2012`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 13653 @5 354000509777770080`
A44				`@0 0000 @1 © 2012 INIST-CNRS. All rights reserved.`
A45				`@0 24 ref.`
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C01	`01`		`ENG`	@0 This paper deals with the non conservation of volume during ultrasonic breakage of ZnO particles whose density varies against size. The observed volumetric particle distributions, obtained by light scattering measurements, are transformed into mass distributions using an expression of the density variation against size based on the fractal dimension. Calculations are then performed using a discretization method given in literature. To validate calculated results, ultrasonic fragmentation of zinc dioxide nanopowder in water is performed in cell dispersion to follow the evolution of the particle size distribution against time. Furthermore, calculated results are adjusted to the experimental particle size distribution curves to determine the breakage frequency constant. This parameter varies with the energy released by the collapse of the cavitation bubbles. Most work on mechanisms of fragmentation by ultrasound is based on the electrical power consumption required for the dispersion of agglomerate. Here, the study focuses on the thermal power which is correlated to the breakage frequency constant. Finally it is found that this parameter is also function of the square root of the thermal power.
C02	`01`	`X`		`@0 001D07Q07`
C02	`02`	`X`		`@0 001D07Q04`
C03	`01`	`X`	`FRE`	`@0 Modélisation @5 01`
C03	`01`	`X`	`ENG`	`@0 Modeling @5 01`
C03	`01`	`X`	`SPA`	`@0 Modelización @5 01`
C03	`02`	`X`	`FRE`	`@0 Agglomération @5 02`
C03	`02`	`X`	`ENG`	`@0 Agglomeration @5 02`
C03	`02`	`X`	`SPA`	`@0 Aglomeración @5 02`
C03	`03`	`X`	`FRE`	`@0 Nanoparticule @5 03`
C03	`03`	`X`	`ENG`	`@0 Nanoparticle @5 03`
C03	`03`	`X`	`SPA`	`@0 Nanopartícula @5 03`
C03	`04`	`X`	`FRE`	`@0 Densité @5 04`
C03	`04`	`X`	`ENG`	`@0 Density @5 04`
C03	`04`	`X`	`SPA`	`@0 Densidad @5 04`
C03	`05`	`X`	`FRE`	`@0 Diffusion lumière @5 05`
C03	`05`	`X`	`ENG`	`@0 Light scattering @5 05`
C03	`05`	`X`	`SPA`	`@0 Difusión luz @5 05`
C03	`06`	`3`	`FRE`	`@0 Distribution masse @5 06`
C03	`06`	`3`	`ENG`	`@0 Mass distribution @5 06`
C03	`07`	`X`	`FRE`	`@0 Dimension fractale @5 07`
C03	`07`	`X`	`ENG`	`@0 Fractal dimension @5 07`
C03	`07`	`X`	`SPA`	`@0 Dimensión fractal @5 07`
C03	`08`	`X`	`FRE`	`@0 Méthode discrétisation @5 08`
C03	`08`	`X`	`ENG`	`@0 Discretization method @5 08`
C03	`08`	`X`	`SPA`	`@0 Método discretización @5 08`
C03	`09`	`X`	`FRE`	`@0 Fragmentation @5 09`
C03	`09`	`X`	`ENG`	`@0 Fragmentation @5 09`
C03	`09`	`X`	`SPA`	`@0 Fragmentación @5 09`
C03	`10`	`X`	`FRE`	`@0 Dispersion @5 10`
C03	`10`	`X`	`ENG`	`@0 Dispersion @5 10`
C03	`10`	`X`	`SPA`	`@0 Dispersión @5 10`
C03	`11`	`X`	`FRE`	`@0 Distribution dimension particule @5 11`
C03	`11`	`X`	`ENG`	`@0 Particle size distribution @5 11`
C03	`11`	`X`	`SPA`	`@0 Distribución dimensión partícula @5 11`
C03	`12`	`X`	`FRE`	`@0 Bulle cavitation @5 12`
C03	`12`	`X`	`ENG`	`@0 Cavitation bubble @5 12`
C03	`12`	`X`	`SPA`	`@0 Burbuja cavitación @5 12`
C03	`13`	`X`	`FRE`	`@0 Ultrason @5 13`
C03	`13`	`X`	`ENG`	`@0 Ultrasound @5 13`
C03	`13`	`X`	`SPA`	`@0 Ultrasonido @5 13`
C03	`14`	`X`	`FRE`	`@0 Consommation énergie @5 14`
C03	`14`	`X`	`ENG`	`@0 Energy consumption @5 14`
C03	`14`	`X`	`SPA`	`@0 Consumo energía @5 14`
C03	`15`	`X`	`FRE`	`@0 Puissance thermique @5 15`
C03	`15`	`X`	`ENG`	`@0 Thermal power @5 15`
C03	`15`	`X`	`SPA`	`@0 Potencia térmica @5 15`
N21				`@1 129`
N44	`01`			`@1 OTO`
N82				`@1 OTO`

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Le document en format XML

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<front><div type="abstract" xml:lang="en">This paper deals with the non conservation of volume during ultrasonic breakage of ZnO particles whose density varies against size. The observed volumetric particle distributions, obtained by light scattering measurements, are transformed into mass distributions using an expression of the density variation against size based on the fractal dimension. Calculations are then performed using a discretization method given in literature. To validate calculated results, ultrasonic fragmentation of zinc dioxide nanopowder in water is performed in cell dispersion to follow the evolution of the particle size distribution against time. Furthermore, calculated results are adjusted to the experimental particle size distribution curves to determine the breakage frequency constant. This parameter varies with the energy released by the collapse of the cavitation bubbles. Most work on mechanisms of fragmentation by ultrasound is based on the electrical power consumption required for the dispersion of agglomerate. Here, the study focuses on the thermal power which is correlated to the breakage frequency constant. Finally it is found that this parameter is also function of the square root of the thermal power.</div>
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<fC01 i1="01" l="ENG"><s0>This paper deals with the non conservation of volume during ultrasonic breakage of ZnO particles whose density varies against size. The observed volumetric particle distributions, obtained by light scattering measurements, are transformed into mass distributions using an expression of the density variation against size based on the fractal dimension. Calculations are then performed using a discretization method given in literature. To validate calculated results, ultrasonic fragmentation of zinc dioxide nanopowder in water is performed in cell dispersion to follow the evolution of the particle size distribution against time. Furthermore, calculated results are adjusted to the experimental particle size distribution curves to determine the breakage frequency constant. This parameter varies with the energy released by the collapse of the cavitation bubbles. Most work on mechanisms of fragmentation by ultrasound is based on the electrical power consumption required for the dispersion of agglomerate. Here, the study focuses on the thermal power which is correlated to the breakage frequency constant. Finally it is found that this parameter is also function of the square root of the thermal power.</s0>
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<fC03 i1="04" i2="X" l="FRE"><s0>Densité</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG"><s0>Density</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA"><s0>Densidad</s0>
<s5>04</s5>
</fC03>
<fC03 i1="05" i2="X" l="FRE"><s0>Diffusion lumière</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="X" l="ENG"><s0>Light scattering</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="X" l="SPA"><s0>Difusión luz</s0>
<s5>05</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Distribution masse</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Mass distribution</s0>
<s5>06</s5>
</fC03>
<fC03 i1="07" i2="X" l="FRE"><s0>Dimension fractale</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="X" l="ENG"><s0>Fractal dimension</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="X" l="SPA"><s0>Dimensión fractal</s0>
<s5>07</s5>
</fC03>
<fC03 i1="08" i2="X" l="FRE"><s0>Méthode discrétisation</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="X" l="ENG"><s0>Discretization method</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="X" l="SPA"><s0>Método discretización</s0>
<s5>08</s5>
</fC03>
<fC03 i1="09" i2="X" l="FRE"><s0>Fragmentation</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="X" l="ENG"><s0>Fragmentation</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="X" l="SPA"><s0>Fragmentación</s0>
<s5>09</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE"><s0>Dispersion</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG"><s0>Dispersion</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA"><s0>Dispersión</s0>
<s5>10</s5>
</fC03>
<fC03 i1="11" i2="X" l="FRE"><s0>Distribution dimension particule</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="X" l="ENG"><s0>Particle size distribution</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="X" l="SPA"><s0>Distribución dimensión partícula</s0>
<s5>11</s5>
</fC03>
<fC03 i1="12" i2="X" l="FRE"><s0>Bulle cavitation</s0>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="X" l="ENG"><s0>Cavitation bubble</s0>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="X" l="SPA"><s0>Burbuja cavitación</s0>
<s5>12</s5>
</fC03>
<fC03 i1="13" i2="X" l="FRE"><s0>Ultrason</s0>
<s5>13</s5>
</fC03>
<fC03 i1="13" i2="X" l="ENG"><s0>Ultrasound</s0>
<s5>13</s5>
</fC03>
<fC03 i1="13" i2="X" l="SPA"><s0>Ultrasonido</s0>
<s5>13</s5>
</fC03>
<fC03 i1="14" i2="X" l="FRE"><s0>Consommation énergie</s0>
<s5>14</s5>
</fC03>
<fC03 i1="14" i2="X" l="ENG"><s0>Energy consumption</s0>
<s5>14</s5>
</fC03>
<fC03 i1="14" i2="X" l="SPA"><s0>Consumo energía</s0>
<s5>14</s5>
</fC03>
<fC03 i1="15" i2="X" l="FRE"><s0>Puissance thermique</s0>
<s5>15</s5>
</fC03>
<fC03 i1="15" i2="X" l="ENG"><s0>Thermal power</s0>
<s5>15</s5>
</fC03>
<fC03 i1="15" i2="X" l="SPA"><s0>Potencia térmica</s0>
<s5>15</s5>
</fC03>
<fN21><s1>129</s1>
</fN21>
<fN44 i1="01"><s1>OTO</s1>
</fN44>
<fN82><s1>OTO</s1>
</fN82>
</pA>
</standard>
</inist>
</record>

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A mass conservative approach to model the ultrasonic de-agglomeration of ZnO nanoparticle suspension in water

A mass conservative approach to model the ultrasonic de-agglomeration of ZnO nanoparticle suspension in water

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