journal article·2019-06-18

Nanoparticle Diffusion within Dilute and Semidilute Xanthan Solutions

Kavindya K. Senanayake, Ashis Mukhopadhyay

Langmuir· Volume 35· Issue 24
Publisher page

Abstract

We measured the translation diffusion coefficient (D) of nanoparticles within dilute and semidilute solutions of a semiflexible polymer, xanthan. Our results showed that for particle diameters (d) of 5 and 10 nm, the obstruction theory can explain the concentration (c) dependence of D in the dilute regime. Diffusion in semidilute solutions is better explained by additionally considering the modified Darcy flow with the hydrodynamic screening length varying according to κ ≈ c–0.76. The depletion effect is operative for larger particles (d = 30 nm) within semidilute solutions. We used a scaling relation for the depletion layer thickness δ ≈ ξν, where ξ is the static correlation length and the exponent ν ≈ 0.42 that can explain our data. This is in contrast with a flat surface, where the exponent is expected to be 1. Our results showed that in the situation, when the polymer network relaxation is much slower compared to the diffusive time-scale of particles, no single theory is capable to describe the concentration and size dependence of particle mobility.
Source: openalex_inverted_index · Quality: baseline

Research context

OpenAlex topics: Electrostatics and Colloid Interactions · Surfactants and Colloidal Systems · Material Dynamics and Properties

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

Department of Physics, Wayne State University, Detroit, Michigan 48201, United States

References (41)

Show source-provided references
1. 10.1021/acs.macromol.6b0047110.1021/acs.macromol.6b00471 ↗
2. 10.1002/9781119290971.ch310.1002/9781119290971.ch3 ↗
3. 10.1039/C6SM01543C10.1039/C6SM01543C ↗
4. 10.1016/j.ijbiomac.2013.12.01710.1016/j.ijbiomac.2013.12.017 ↗
5. 10.1103/PhysRevE.69.02180410.1103/PhysRevE.69.021804 ↗
6. 2001
7. 10.1016/0144-8617(86)90023-810.1016/0144-8617(86)90023-8 ↗
8. 10.1021/ma00211a01810.1021/ma00211a018 ↗
9. 10.1021/la053325810.1021/la0533258 ↗
10. 10.1002/app.3109310.1002/app.31093 ↗
11. 10.1021/ma201583q10.1021/ma201583q ↗
12. 10.1103/PhysRevE.78.05180410.1103/PhysRevE.78.051804 ↗
13. 10.1021/ma501670u10.1021/ma501670u ↗
14. 10.1021/acs.macromol.8b0191710.1021/acs.macromol.8b01917 ↗
15. 10.1021/ma501499510.1021/ma5014995 ↗
17. 10.1021/ma00110a02110.1021/ma00110a021 ↗
18. 10.1063/1.183489510.1063/1.1834895 ↗
19. 10.1063/1.45401610.1063/1.454016 ↗
20. de Gennes P.-G. · 1979
21. 10.1007/s10189005001110.1007/s101890050011 ↗
22. 10.1021/ma301237r10.1021/ma301237r ↗
23. 10.1021/acs.langmuir.7b0341810.1021/acs.langmuir.7b03418 ↗
24. 10.1021/acs.jpclett.5b0262410.1021/acs.jpclett.5b02624 ↗
25. 10.1021/jp502467u10.1021/jp502467u ↗
26. 10.1021/acs.macromol.5b0153010.1021/acs.macromol.5b01530 ↗
27. 10.1016/S0079-6700(99)00016-710.1016/S0079-6700(99)00016-7 ↗
28. 10.1016/S0006-3495(96)79467-510.1016/S0006-3495(96)79467-5 ↗
29. 10.1016/S0966-7822(97)00012-910.1016/S0966-7822(97)00012-9 ↗
30. 10.1209/epl/i2006-10200-010.1209/epl/i2006-10200-0 ↗
31. 10.1063/1.216120410.1063/1.2161204 ↗
32. 10.1063/1.45066510.1063/1.450665 ↗
33. 10.1021/ma00132a02310.1021/ma00132a023 ↗
34. 10.1002/pol.1982.18020090110.1002/pol.1982.180200901 ↗
35. 10.1007/BF0212031310.1007/BF02120313 ↗
36. 10.1021/j150670a02610.1021/j150670a026 ↗
37. 10.1103/PhysRevE.64.04050110.1103/PhysRevE.64.040501 ↗
38. 10.1103/PhysRevLett.53.83410.1103/PhysRevLett.53.834 ↗
39. 10.1063/1.47949810.1063/1.479498 ↗
40. 10.1063/1.366486310.1063/1.3664863 ↗
41. 10.1021/ma501150q10.1021/ma501150q ↗