2022
DOI: 10.1039/d2sm00304j
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Scaling mechanical instabilities in drying micellar droplets

Abstract: Drying-induced mechanical instabilities in soft matter droplets occur primarily due to the interplay of evaporative compressive stresses, leading to a stretching effect of the liquid region at the receding wet...

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Cited by 1 publication
(6 citation statements)
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“…The hydrodynamic stress (σ h ), and elastocapillary stress (σ ec ), are the consequence of outward capillary flow, that results in a coffee ring-like deposition at the droplet edge . The direction of elastocapillary stress is primarily inward, which pulls the packed bed inward to minimize its surface energy and that eventually causes cracking or wrinkling. ,, By balancing the extra surface energy associated with the new surface formation and elastic energy release on cracking, Sprakel and co-workers expressed a relation between shrinkage stress and critical shrinkage stress (σ s,c ) . Combining the well-known Griffith’s equilibrium crack propagation criterion and Routh and Russel’s stress–strain criteria for a network of identical elastic spheres, they introduced the following expression for critical shrinkage stress , : σ normals , normalc = 0.3754 true( 2 γ h true) 2 / 3 true( italicEM φ rep 2 true) 1 / 3 , where h denotes the film thickness, M is the coordination number, φ rep is the particle volume fraction at random close packing, E is the particle modulus, and γ denotes liquid–air interfacial tension.…”
Section: Resultsmentioning
confidence: 99%
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“…The hydrodynamic stress (σ h ), and elastocapillary stress (σ ec ), are the consequence of outward capillary flow, that results in a coffee ring-like deposition at the droplet edge . The direction of elastocapillary stress is primarily inward, which pulls the packed bed inward to minimize its surface energy and that eventually causes cracking or wrinkling. ,, By balancing the extra surface energy associated with the new surface formation and elastic energy release on cracking, Sprakel and co-workers expressed a relation between shrinkage stress and critical shrinkage stress (σ s,c ) . Combining the well-known Griffith’s equilibrium crack propagation criterion and Routh and Russel’s stress–strain criteria for a network of identical elastic spheres, they introduced the following expression for critical shrinkage stress , : σ normals , normalc = 0.3754 true( 2 γ h true) 2 / 3 true( italicEM φ rep 2 true) 1 / 3 , where h denotes the film thickness, M is the coordination number, φ rep is the particle volume fraction at random close packing, E is the particle modulus, and γ denotes liquid–air interfacial tension.…”
Section: Resultsmentioning
confidence: 99%
“…From droplet evaporation dynamics, it is well-established that increasing the substrate temperature causes a temperature gradient within the droplet. The portion of the drop closer to the hot substrate becomes hotter, and the apex or top of the drop, far from the substrate contact, becomes the cooler zone. ,, Now, the temperature gradient creates a surface tension gradient; therefore, a flow from higher temperature (lower surface tension) to lower temperature (higher surface tension) is generated within the droplet, known as a thermal Marangoni flow (Figure a). This inward flow works opposite to the evaporation-driven outward capillary flow field.…”
Section: Resultsmentioning
confidence: 99%
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