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Coffee ring effect

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In physics, a "coffee ring" is a pattern left by a puddle of particle-laden liquid after it evaporates. The phenomenon is named for the characteristic ring-like deposit along the perimeter of a spill of coffee. It is also commonly seen after spilling red wine. The mechanism behind the formation of these and similar rings is known as the coffee ring effect or in some instances, the coffee stain effect, or simply ring stain.

Stains produced by the evaporation of coffee spills

Flow mechanism

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The coffee-ring pattern originates from the capillary flow induced by the evaporation of the drop: liquid evaporating from the edge is replenished by liquid from the interior.[1] The resulting current can carry nearly all the dispersed material to the edge. As a function of time, this process exhibits a "rush-hour" effect, that is, a rapid acceleration of the flow towards the edge at the final stage of the drying process.[2]

Evaporation induces a Marangoni flow inside a droplet. The flow, if strong, redistributes particles back to the center of the droplet. Thus, for particles to accumulate at the edges, the liquid must have a weak Marangoni flow, or something must occur to disrupt the flow.[3] For example, surfactants can be added to reduce the liquid's surface tension gradient, disrupting the induced flow. Water has a weak Marangoni flow to begin with, which is then reduced significantly by natural surfactants.[4]

Interaction of the particles suspended in a droplet with the free surface of the droplet is important in creating a coffee ring.[5] "When the drop evaporates, the free surface collapses and traps the suspended particles ... eventually all the particles are captured by the free surface and stay there for the rest of their trip towards the edge of the drop."[6] This result means that surfactants can be used to manipulate the motion of the solute particles by changing the surface tension of the drop, rather than trying to control the bulk flow inside the drop. A number of unique morphologies of the deposited particles can result. For example, an enantiopure poly (isocyanate) derivative has been shown to form ordered arrays of squashed donut structures. [7]

Suppression

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Stains produced by colloidal mixtures of polystyrene particles (diameter 1.4 μm) and cellulose fibers (diameter ~20 nm, length ~1 μm). The polystyrene concentration is fixed at 0.1 wt%, and that of cellulose is 0 (left), 0.01 (center) and 0.1 wt% (right).[2]

The coffee-ring pattern is detrimental when uniform application of a dried deposit is required, such as in printed electronics. It can be suppressed by adding elongated particles, such as cellulose fibers, to the spherical particles that cause the coffee-ring effect. The size and weight fraction of added particles may be smaller than those of the primary ones.[2]

It is also reported that controlling flow inside a droplet is a powerful way to generate a uniform film; for example, by harnessing solutal Marangoni flows occurring during evaporation.[8]

Mixtures of low boiling point and high boiling point solvents were shown to suppress the coffee ring effect, changing the shape of a deposited solute from a ring-like to a dot-like shape.[9]

Control of the substrate temperature was shown to be an effective way to suppress the coffee ring formed by droplets of water-based PEDOT:PSS solution.[10] On a heated hydrophilic or hydrophobic substrate, a thinner ring with an inner deposit forms, which is attributed to Marangoni convection.[11]

Control of the substrate wetting properties on slippery surfaces can prevent the pinning of the drop contact line, which will, therefore, suppress the coffee ring effect by reducing the number of particles deposited at the contact line. Drops on superhydrophobic or liquid impregnated surfaces are less likely to have a pinned contact line and will suppress ring formation.[12] Drops with an oil ring formed at the drop contact line have high mobility and can avoid the ring formation on hydrophobic surfaces.[13]

Alternating voltage electrowetting may suppress coffee stains without the need to add surface-active materials.[14] Reverse particle motion may also reduce the coffee-ring effect because of the capillary force near the contact line.[15] The reversal takes place when the capillary force prevails over the outward coffee-ring flow by the geometric constraints.

Determinants of size and pattern

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The lower-limit size of a coffee ring depends on the time scale competition between the liquid evaporation and the movement of suspended particles.[16] When the liquid evaporates much faster than the particle movement near a three-phase contact line, a coffee ring cannot be formed successfully. Instead, these particles will disperse uniformly on a surface upon complete liquid evaporation. For suspended particles of size 100 nm, the minimum diameter of the coffee ring structure is found to be 10 μm, or about 10 times smaller than the width of human hair. The shape of particles in the liquid is responsible for coffee ring effect.[17][18] On porous substrates, the competition among infiltration, particle motion and evaporation of the solvent governs the final deposition morphology.[19]

The pH of the solution of the drop influences the final deposit pattern.[20] The transition between these patterns is explained by considering how DLVO interactions such as the electrostatic and Van der Waals forces modify the particle deposition process.

Applications

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The coffee ring effect is utilized in convective deposition by researchers wanting to order particles on a substrate using capillary-driven assembly, replacing a stationary droplet with an advancing meniscus drawn across the substrate.[21][22][23] This process differs from dip-coating in that evaporation drives flow along the substrate as opposed to gravity.

Convective deposition can control particle orientation, resulting in the formation of crystalline monolayer films from nonspherical particles such as hemispherical,[24] dimer,[25] and dumbbell[26] shaped particles. Orientation is afforded by the system trying to reach a state of maximum packing of the particles in the thin meniscus layer over which evaporation occurs. They showed that tuning the volume fraction of particles in solution will control the specific location along the varying meniscus thickness at which assembly occurs. Particles will align with their long axis in- or out-of-plane depending on whether or not their longer dimension of the particle was equal to the thickness of the wetting layer at the meniscus location.[26] Such thickness transitions were established with spherical particles as well.[27] It was later shown that convective assembly could control particle orientation in assembling multi-layers, resulting in long-range 3D colloidal crystals from dumbbell shaped particles.[28] These finds were attractive for the self-assembled of colloidal crystal films for applications such as photonics.[28] Recent advances have increased the application of coffee-ring assembly from colloidal particles to organized patterns of inorganic crystals.[12]

References

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  1. ^ Deegan, Robert D.; Bakajin, Olgica; Dupont, Todd F.; Huber, Greg; Nagel, Sidney R.; Witten, Thomas A. (1997). "Capillary flow as the cause of ring stains from dried liquid drops". Nature. 389 (6653): 827–829. Bibcode:1997Natur.389..827D. doi:10.1038/39827. S2CID 205027233.
  2. ^ a b c Ooi, Yuto; Hanasaki, Itsuo; Mizumura, Daiki; Matsuda, Yu (2017). "Suppressing the coffee-ring effect of colloidal droplets by dispersed cellulose nanofibers". Science and Technology of Advanced Materials. 18 (1): 316–324. Bibcode:2017STAdM..18..316O. doi:10.1080/14686996.2017.1314776. PMC 5439399. PMID 28567177.
  3. ^ Hu, H; Larson, R. G. (2006). "Marangoni Effect Reverses Coffee-Ring Depositions". Journal of Physical Chemistry B. 110 (14): 7090–7094. doi:10.1021/jp0609232. PMID 16599468.
  4. ^ Savino, R.; Paterna, D.; Favaloro, N. (2002). "Buoyancy and Marangoni Effects in an Evaporating Drop". Journal of Thermophysics and Heat Transfer. 16 (4): 562–574. doi:10.2514/2.6716. ISSN 0887-8722.
  5. ^ Jafari Kang, Saeed; Vandadi, Vahid; Felske, James D.; Masoud, Hassan (2016). "Alternative mechanism for coffee-ring deposition based on active role of free surface". Physical Review E. 94 (6): 063104. arXiv:0906.3878. Bibcode:2016PhRvE..94f3104J. doi:10.1103/PhysRevE.94.063104. PMID 28085318. S2CID 10670995.
  6. ^ Coffee-ring phenomenon explained in new theory. phys.org (December 20, 2016)
  7. ^ Carroll, Gregory; Jongejan, Mahthild; Pijper, Dirk; Feringa, Ben (2010). "Spontaneous generation and patterning of chiral polymeric surface toroids" (PDF). Chemical Science. 1 (4): 469–472. doi:10.1039/c0sc00159g.
  8. ^ Gençer, Alican; Schütz, Christina; Thielemans, Wim (2017). "Influence of the Particle Concentration and Marangoni Flow on the Formation of Cellulose Nanocrystal Films". Langmuir. 33 (1): 228–234. doi:10.1021/acs.langmuir.6b03724. PMID 28034313.
  9. ^ de Gans, Berend-Jan; Schubert, Ulrich S. (2004). "Inkjet Printing of Well-Defined Polymer Dots and Arrays". Langmuir. 20 (18): 7789–7793. doi:10.1021/la049469o. ISSN 0743-7463. PMID 15323532.
  10. ^ Soltman, Dan; Subramanian, Vivek (2008). "Inkjet-Printed Line Morphologies and Temperature Control of the Coffee Ring Effect". Langmuir. 24 (5): 2224–2231. doi:10.1021/la7026847. ISSN 0743-7463. PMID 18197714.
  11. ^ Patil, Nagesh D.; Bange, Prathamesh G.; Bhardwaj, Rajneesh; Sharma, Atul (2016). "Effects of Substrate Heating and Wettability on Evaporation Dynamics and Deposition Patterns for a Sessile Water Droplet Containing Colloidal Particles". Langmuir. 32 (45): 11958–11972. arXiv:1610.06281. doi:10.1021/acs.langmuir.6b02769. PMID 27759960. S2CID 46708941.
  12. ^ a b McBride, Samantha; Dash, Susmita; Varanasi, Kripa (2018). "Evaporative Crystallization in Drops on Superhydrophobic and Liquid-Impregnated Surfaces". Langmuir. 34 (41): 12350–12358. doi:10.1021/acs.langmuir.8b00049. hdl:1721.1/129769. PMID 29609465.
  13. ^ Tan, Huanshu; Wooh, S.; Butt, H.-J.; Zhang, X.; Lohse, D. (2019). "Porous supraparticle assembly through self-lubricating evaporating colloidal ouzo drops". Nature Communications. 10 (1): 478. Bibcode:2019NatCo..10..478T. doi:10.1038/s41467-019-08385-w. PMC 6351649. PMID 30696829.
  14. ^ Eral, H.B.; Mampallil-Agustine, D.; Duits, M.H.G.; Mugele, F. (2011). "Suppressing the coffee stain effect: how to control colloidal self-assembly in evaporating drops using electrowetting". Soft Matter. 7 (10): 7090–7094. Bibcode:2011SMat....7.4954E. doi:10.1039/C1SM05183K.
  15. ^ Weon, Byung Mook; Je, Jung Ho (2010). "Capillary force repels coffee-ring effect". Physical Review E. 82 (1): 015305(R). Bibcode:2010PhRvE..82a5305W. doi:10.1103/PhysRevE.82.015305. PMID 20866682.
  16. ^ Shen, X; Ho, C. M.; Wong, T. S. (2010). "Minimal Size of Coffee Ring Structure". Journal of Physical Chemistry B. 114 (16): 5269–5274. doi:10.1021/jp912190v. PMC 2902562. PMID 20353247.
  17. ^ Yunker, P. J.; Still, T; Lohr, M. A.; Yodh, A. G. (2011). "Suppression of the coffee-ring effect by shape-dependent capillary interactions". Nature. 476 (7360): 308–311. Bibcode:2011Natur.476..308Y. doi:10.1038/nature10344. PMID 21850105. S2CID 205226009.
  18. ^ "Coffee-ring effect explained". ScienceDebate.com. Retrieved 21 August 2011.
  19. ^ Pack, Min; Hu, Han; Kim, Dong-Ook; Yang, Xin; Sun, Ying (2015). "Colloidal drop deposition on porous substrates: competition among particle motion, evaporation and infiltration". Langmuir. 31 (29): 7953–7961. doi:10.1021/acs.langmuir.5b01846. PMID 26132211.
  20. ^ Bhardwaj, R; Fang, X; Somasundaran, P; Attinger, D (2010). "Self-Assembly of Colloidal Particles from Evaporating Droplets: Role of DLVO Interactions and Proposition of a Phase Diagram". Langmuir. 26 (11): 7833–42. arXiv:1010.2564. doi:10.1021/la9047227. PMID 20337481. S2CID 4789514.
  21. ^ Prevo, Brian G.; Velev, Orlin D. (2004). "Controlled rapid deposition of structured coatings from micro-and nanoparticle suspensions". Langmuir. 20 (6): 2099–2107. doi:10.1021/la035295j. PMID 15835658.
  22. ^ Kumnorkaew, Pisist; Ee, Yik-Khoon; Tansu, Nelson; Gilchrist, James F. (2008). "Investigation of the Deposition of Microsphere Monolayers for Fabrication of Microlens Arrays". Langmuir. 24 (21): 12150–12157. doi:10.1021/la801100g. PMID 18533633.
  23. ^ Dimitrov, Antony S.; Nagayama, Kuniaki (1995). "Steady-state unidirectional convective assembling of fine particles into two-dimensional arrays". Chemical Physics Letters. 243 (5–6): 462–468. Bibcode:1995CPL...243..462D. doi:10.1016/0009-2614(95)00837-T.
  24. ^ Hosein, Ian D.; Liddell, Chekesha M. (2007-08-01). "Convectively Assembled Nonspherical Mushroom Cap-Based Colloidal Crystals". Langmuir. 23 (17): 8810–8814. doi:10.1021/la700865t. PMID 17630788.
  25. ^ Hosein, Ian D.; John, Bettina S.; Lee, Stephanie H.; Escobedo, Fernando A.; Liddell, Chekesha M. (2008-12-24). "Rotator and crystalline films viaself-assembly of short-bond-length colloidal dimers". Journal of Materials Chemistry. 19 (3): 344–349. doi:10.1039/B818613H.
  26. ^ a b Hosein, Ian D.; Liddell, Chekesha M. (2007-10-01). "Convectively Assembled Asymmetric Dimer-Based Colloidal Crystals". Langmuir. 23 (21): 10479–10485. doi:10.1021/la7007254. PMID 17629310.
  27. ^ Meng, Linli; Wei, Hong; Nagel, Anthony; Wiley, Benjamin J.; Scriven, L. E.; Norris, David J. (2006-10-01). "The Role of Thickness Transitions in Convective Assembly". Nano Letters. 6 (10): 2249–2253. Bibcode:2006NanoL...6.2249M. doi:10.1021/nl061626b. PMID 17034092.
  28. ^ a b Hosein, Ian D.; Lee, Stephanie H.; Liddell, Chekesha M. (2010-09-23). "Dimer-Based Three-Dimensional Photonic Crystals". Advanced Functional Materials. 20 (18): 3085–3091. doi:10.1002/adfm.201000134. S2CID 136970162.
 
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