- Volumes 108-119 (2025)
-
Volumes 96-107 (2025)
-
Volume 107
Pages 1-376 (December 2025)
-
Volume 106
Pages 1-336 (November 2025)
-
Volume 105
Pages 1-356 (October 2025)
-
Volume 104
Pages 1-332 (September 2025)
-
Volume 103
Pages 1-314 (August 2025)
-
Volume 102
Pages 1-276 (July 2025)
-
Volume 101
Pages 1-166 (June 2025)
-
Volume 100
Pages 1-256 (May 2025)
-
Volume 99
Pages 1-242 (April 2025)
-
Volume 98
Pages 1-288 (March 2025)
-
Volume 97
Pages 1-256 (February 2025)
-
Volume 96
Pages 1-340 (January 2025)
-
Volume 107
-
Volumes 84-95 (2024)
-
Volume 95
Pages 1-392 (December 2024)
-
Volume 94
Pages 1-400 (November 2024)
-
Volume 93
Pages 1-376 (October 2024)
-
Volume 92
Pages 1-316 (September 2024)
-
Volume 91
Pages 1-378 (August 2024)
-
Volume 90
Pages 1-580 (July 2024)
-
Volume 89
Pages 1-278 (June 2024)
-
Volume 88
Pages 1-350 (May 2024)
-
Volume 87
Pages 1-338 (April 2024)
-
Volume 86
Pages 1-312 (March 2024)
-
Volume 85
Pages 1-334 (February 2024)
-
Volume 84
Pages 1-308 (January 2024)
-
Volume 95
-
Volumes 72-83 (2023)
-
Volume 83
Pages 1-258 (December 2023)
-
Volume 82
Pages 1-204 (November 2023)
-
Volume 81
Pages 1-188 (October 2023)
-
Volume 80
Pages 1-202 (September 2023)
-
Volume 79
Pages 1-172 (August 2023)
-
Volume 78
Pages 1-146 (July 2023)
-
Volume 77
Pages 1-152 (June 2023)
-
Volume 76
Pages 1-176 (May 2023)
-
Volume 75
Pages 1-228 (April 2023)
-
Volume 74
Pages 1-200 (March 2023)
-
Volume 73
Pages 1-138 (February 2023)
-
Volume 72
Pages 1-144 (January 2023)
-
Volume 83
-
Volumes 60-71 (2022)
-
Volume 71
Pages 1-108 (December 2022)
-
Volume 70
Pages 1-106 (November 2022)
-
Volume 69
Pages 1-122 (October 2022)
-
Volume 68
Pages 1-124 (September 2022)
-
Volume 67
Pages 1-102 (August 2022)
-
Volume 66
Pages 1-112 (July 2022)
-
Volume 65
Pages 1-138 (June 2022)
-
Volume 64
Pages 1-186 (May 2022)
-
Volume 63
Pages 1-124 (April 2022)
-
Volume 62
Pages 1-104 (March 2022)
-
Volume 61
Pages 1-120 (February 2022)
-
Volume 60
Pages 1-124 (January 2022)
-
Volume 71
- Volumes 54-59 (2021)
- Volumes 48-53 (2020)
- Volumes 42-47 (2019)
- Volumes 36-41 (2018)
- Volumes 30-35 (2017)
- Volumes 24-29 (2016)
- Volumes 18-23 (2015)
- Volumes 12-17 (2014)
- Volume 11 (2013)
- Volume 10 (2012)
- Volume 9 (2011)
- Volume 8 (2010)
- Volume 7 (2009)
- Volume 6 (2008)
- Volume 5 (2007)
- Volume 4 (2006)
- Volume 3 (2005)
- Volume 2 (2004)
- Volume 1 (2003)
• A model with shrinkage deformation is developed for desorption prediction.
• The model uniquely couples multiphase flow, heat/mass transfer, and phase change.
• The model accurately predicts hydrogel desorption kinetics and shrinkage.
Hydrogel desorption shows promise for thermal management and passive cooling engineering applications, but challenges persist in understanding particle desorption and shrinkage. A Lattice Boltzmann-based phase-field model was developed by combining experiments and mesoscopic simulations to simulate conjugate heat transfer, desorption kinetics, and shrinkage of single hydrogel particles, achieving <5% deviation from experiments. Results show that raising temperature from 343 to 353 K increases 1-h desorption mass by ∼12% of initial mass (vs. 1.3% for 313–323 K), driven by rising saturation vapor pressure and falling evaporation enthalpy. Shrinkage is more sensitive at high temperature and low humidity, with surface area reductions of ∼17% (343–353 K) and ∼13% (20–30% RH), compared to ∼5% under mild conditions. Reducing particle initial mass from 5.75 g to 0.16 g shortens the time to release 50% of the initial water from 516 min to 117 min, indicating greater efficiency for smaller particles. This work bridges the macro-pore scale gap and offers a numerical tool with design insights for passive cooling.