Seminars

Ph.D. Viva-Voce Ms. Surita Basu Supervisor ( Prof Jayati Sarkar)

DateTuesday, 21 September 2021
Time4:00 PM
VenueThrough M S Team Link

STUDYOFMINIATURIZATIONOFSURFACEPATTERNSANDSELF-ORGANIZATIONOF CARBONACEOUSNANOPARTICLESON SOFT THIN FILMS AND THEIRAPPLICATIONS 

Date           :        21st September 2021
Venue       :        Online
Time          :        4.00 PM

MS TEAMS LINK: https://teams.microsoft.com/l/meetup-join/19%3ameeting_ZTFhYzhjMGMtNDUwZi00NTEzLThiNjUtMzNkNTdiNjljNzZh%40thread.v2/0?context=%7b%22Tid%22%3a%22624d5c4b-45c5-4122-8cd0-44f0f84e945d%22%2c%22Oid%22%3a%222dba7fce-4ddb-4d24-ac09-5d4ebf4b3553%22%7d

 

Abstract:-

Thin films are of paramount interest in daily customary life. Patterns formed in thin films are of more advanced importance. These micro and nano patterns on solid and liquid film is not only  used  in  microelectronics  but  has  emerged  as  an  winner  in  other  recent  developments such as in fabrication of lab-on-chip devices for biomedical purposes, coating and adhesives as  functional  and  self-cleaning  material,  various  scaffolds  for  tissue  engineering,  and  many more.  The  budding  application  of  these  patterns  in  thin  film  have  led  to  the  replacement  of hard,  exuberant  and  costly  forms  of  lithography  techniques  giving  way  to  low  cost  “self-organization”    and  “self-assembly”  technique. Self-organization  requires  external  energy source  and  therefore  is  dissipative  and  non-equilibrium  but  self-assembly  is  a  spontaneous equilibrium   process.   A   thin   film   in   a   confined   region   due   to competition   between intermolecular forces and surface tension becomes unstable and patterns arise on the surface of thin  liquid  films  due  to  the  competitive  nature  between  the  excess  intermolecular interactions  and  interfacial  tension. Another  kind  of  pattern  formation  is  observed  at  thesurface of a soft elastic film when the film is brought in close proximity of a contactor. The interaction forces between the film and the contactor destabilizes the film surface, while the stored  elastic  energy  tries  to  restore  the  film  to  original  configuration.  These  antagonistic forces   give   rise   to   instabilities   in   the   surface   and   thus   results   in   meso/nano   scaled morphological  surface  feature.Miniaturization  of  patterns  is  a  new  addition  to  this  flock  of studies.  The process of making miniaturizationof these patterns formed due to self-assembly is  of  much  interest  due  to  its  ability  to  create  small  size  and  portability,  low  sample  size, volume  and  cost  reductionThe formation  of  miniaturized  surface  morphologies  over  a  soft thin  elastic  film  of  micron  range  thickness  (h),  when  cast  on  various  patterned  substrates created from: naturally available intrinsically rough water lily leaves, commercially available sinusoidally  patterned  compact  disks  and  cubic  boxes  created  by  electron  beam  lithography were investigated   experimentally.The   evolving   surface   patterns   formed   had   varying structures  of  columns  to  labyrinth  to  cavities  during  the  adhesion  and  debonding  cycle,

irrespective of which the engendered dominant wavelength (λ) remained at a miniscule length scale and is depended solely on its RMS roughness.It was observed experimentally that the length  scales  of  the  patterns  formed  decreased  linearly  with  increase  in  substrate  amplitude and regardless of the substrate pattern geometry used depended solely on its RMS roughness such that λ⁄h=2.96-18.2*(RMS/h).The study indicates the redundancy in creating very costly regular geometrical patterned substrates for miniaturization and instead advocates the use of intrinsically rough natural surface replicasto be used as patterned substrates for cost-effective fabrication  of  miniaturized  surface  patterns  at  such  soft  interfaces.The  spontaneous  self-assembly of the carbon nano-particles-graphene and carbon nanotube intensify over the self-assembledpatternsformed  on  the  thin  polymeric  film.  The  dewetting  dynamics  of  the underlying filminfluences  the  formation  of  unique  self-assembled  graphene  patterns  at  the interface  between  graphene  and  a  thin  polystyrene  film  by  various  approaches-graphene-polymer composite thin film, polymer thin film with graphene nanoparticles as a bilayer and graphene  nanoparticles  drop-cast  over  the  array  of  dewetted  holes  on  polymeric  thin-film. When  a  minute  amount  of  graphene  dispersed  in  a  solvent  is  added  on  PS  and spin-coated into a thin film, the concentration gradient caused by centrifugal force leads to a Marangoni flow that in conjunction with the dewetting of the underlying PS at the edges lead to a series of  very  interesting,  striking  and  self-assembled  morphologies  of  graphene.At  the  particle enriched  zone  near  the  center,  the  graphene-particles  exhibit  morphologies  ranging  from folds,  wrinkles,  flakes,  onion-rings  to  blob  structures  depending  on  the  aspect  ratio. The increase in graphene nanoparticle concentration and the annealing temperature in this regime leads  to  formation  of  clusters. The  graphene-particles  thrown  to  the  periphery  are  found  to march back towards the central portion leading to the unique formation of very ordered nano-scale scratches on the PS substrate. The nano-particles that end up into the confined rims in the  intermediate  region  get  twisted  into  nano-ribbons  and  dendrimers.The  increase  in concentration  of  graphene  nanoparticles  and  temperature  leads  to  formation  of  fingering morphologies  in  this  region.  The  increase  in  the  temperature  near  the  dewetting  regime caused  the  polymer  in  presence  of  high  concentration  of  graphene  nanoparticles  to  form  a floral  pattern on  the  surface  of  the  film.The  polystyrene-graphene  nanoparticles  composite when  spin-coated  together  to  form  a  thin  film  over  a  substrate,  it  was  observed  that  these nanoparticles  self-assemble  in  a  Voronoi  tessellation  of  ribbon-like  structure  along  with  the suppression  of  dewetting  of  thin  polystyrene  film  at  this  stage.  The  graphene  nanoparticles dispersed  in  solvent  were  casted  over  the  instability  based  dewetting  patterns  formed  on  the surface  of  the  thin  polystyrene  film  causing  the  graphene  nanoparticles  to  arrange  in  a

polygonal  array  of  dots  prompted  by  the  dynamics  and  morphology  of  dewetting.  The reversals  of  the  dewetted  patterns  were  observed  in  this  process  because  of  the  solvent evaporation and Marangoni flow. Moreover, without the aid of any high-end instrumentation or  process,  different  origami  structures  were formed  by  the  presence  of  different  forces  and the underlying dewetting dynamics.The instability of a polymeric thin film, when cast either as  a  mobile  underlying  support-layer  of  a  bilayer  assembly,  as  a  mixture,  or  as  a  template, affects the self-assembly and arrangement of carbon nanotube (CNT) nanoparticles dispersed over/with  it.  The  interplay  of  the  different  forces,  like  centrifugal,  dewetting,  Marangoni, electrostatic,  assist  the  mobile  nanoparticles  in  arranging  themselves  into  circular  ring-like structures.  The  congruence  of  the  length-scales  of  the  self-assembled  circular  ring  and  the dewetted  length-scales  of  the  thin  polystyrene  film  reveals  that  the  influence  of  dewetting dynamics is majorly responsible for the incipience of ring formations.The nanoparticles not involved  in  circular-ring-self-assembly  formation  are  driven  by  Marangoni  force  (effective due to difference in surface tension values because of nanoparticle concentration difference) and  engender  nano-scratches  over  the  polymeric  surface.  The  bending  of  the  carbon nanotubes  is  an  energetically  favoured  self-organization  process  controlled  by  the  shape formation  energy.Finally, surface  corrugations  such  as  columns,  labyrinths  and  cavities evolved  spontaneously  due  to  instability  on  thesurfaces  of  a  thin  soft  elastic  PDMS  film  in adhesive contact with a contactor along with the oleophilic nature of the film help in selective adsorption  of  the  oil  from  the  oil-water  mixture  into  the  intervening  surface  spaces. The increase  in  RMS  surfaceroughness  brought  about  either  by  increase  in  adsorbent  weight  or by  formation  of  a  columnar  structure  (instead  of  cavities  or  labyrinths)  was  found  to  have  a significant  incremental  effect  on  the  true  surface  area  creation  by  formation  of  increased number  of  oil  adsorption  sites:  leading  to  higher  oil  penetration  and  thus,  higher  oil adsorption.  For  0.3wt%  of  adsorbent,  adsorption  was  found  to  be  maximum  for  columnar structures at 23%, followed by cavities at 15% and minimum with labyrinth at around 12%. The ratio (dp/dd) of the substrate pore size dimension (dp) to the surface oil droplet dimension (dd) in crude oil, motor oil, diesel and petrol were found to be progressively lower and hence the maximum adsorption and penetration in the columnar patterns was recognized in case of crude oil. Additionally, the circular rings of CNTs formed throughout the PS surface, can be used to identify trace amounts of oil from an oil-water mixture by selective adsorption. This thesis contributes  on  creating spontaneous patterns  on  soft  thin  film  embedded  with/without carbonaceous nanoparticles via different approaches with enhanced surface properties

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