Large aggregate species in conjugated polymer solutions characterized by dynamic light scattering and in situ rheological/flow turbidity measurements Chih.

Slides:



Advertisements
Similar presentations
Viscosity of Dilute Polymer Solutions
Advertisements

Lecture 17. Light Scattering/Viscometry. What is light scattering? In the lab…
Polyelectrolyte solutions
Colloid: Electrokinetic properties
MODELLING OF CAVITATION FLOW IN A DIESEL INJECTION NOZZLE S. Martynov 1, D. Mason 2, M. Heikal 2 1 Department of Mechanical Engineering, University College.
Stress Relaxation of Comb Polymers Keith M. Kirkwood a, Dimitris Vlassopoulos b,c, and L. Gary Leal a a Department of Chemical Engineering, University.
Measurement of mobility of positive charge carriers in polyethylene J Zhao, G Chen and P L Lewin University of Southampton, Southampton, UK Positive charge.
The use of light scattering in characterizing lignin.
 M OTIVATION C ONTROL OF AGGREGATES IN POLY (3- HEXYLTHIOPHENE ) SOLUTIONS AND THIN FILMS Recent research has shown that the charge carrier mobility in.
Granular flows under the shear Hisao Hayakawa* & Kuniyasu Saitoh Dept. Phys. Kyoto Univ., JAPAN *
Dr. Mohammed M. Amro Petroleum Engineering Dept. King Saud University Effect of Scale and Corrosion Inhibitors on Well Productivity in Reservoirs Containing.
Nanoparticles Characterization: Measurement of the particles size by the PCS technique MSc. Priscyla D. Marcato Dr. Nelson Durán.
Dynamics of a Colloidal Glass During Stress-Mediated Structural Arrest (“Relaxation in Reverse”) Dynamics of a Colloidal Glass During Stress-Mediated Structural.
Computer Simulations, Scaling and the Prediction of Nucleation Rates
The Scaling of Nucleation Rates Barbara Hale Physics Department and Cloud and Aerosol Sciences Laboratory University of Missouri – Rolla Rolla, MO
James Sprittles ECS 2007 Viscous Flow Over a Chemically Patterned Surface J.E. Sprittles Y.D. Shikhmurzaev.
NEMATIC FLUCTUATIONS AS A PROBE OF THE PROPERTIES OF LIQUID CRYSTAL ELASTOMERS Martin Čopič Irena Drevenšek-Olenik Andrej Petelin Boštjan Zalar.
1 Stimuli Responsive Materials Derived from Poly(acrylamides) Greg Sorenson April 15, 2010 Mahanthappa Group University of Wisconsin - Madison.
National Science Foundation WHERE DISCOVERIES BEGIN Controlling Polymer Rheological Properties Using Long-Chain Branching PI: Ronald Larson Univ. of Mich.,
Thermo-responsive interaction between  -cyclodextrin and amphiphilic biopolymers. Here we will discuss how the cosolute  -cyclodextrin and temperature.
Photophysical Properties of CdSe/ZnS Quantum Dots Embedded in Polymer Films and Solubilized in Toluene Final Presentation Jamie Golden CHEM /30/10.
Surface and Interface Chemistry  Rheology Valentim M. B. Nunes Engineering Unit of IPT 2014.
© J D White SMS : Illuminating the photo-physics of Luminescent Conjugated Polymers– Results 1 Results & Discussion Results: observing the PL time trace’s:
Date: 2008/11/7 Complex Fluids & Molecular Rheology Laboratory, Department of Chemical Engineering, National Chung Cheng University, Chia-Yi 621, Taiwan,
A computational study of shear banding in reversible associating polymers J. Billen, J. Stegen +, A.R.C. Baljon San Diego State University + Eindhoven.
Experimental and Theoretical Investigations on Dilute MEH-PPV Solutions 謝盛昌、陳建龍、張志偉、林信宏、 華繼中 國立中正大學化學工程系 Polymer Rheology and Molecular Simulation Lab.,
Complex Fluids & Molecular Rheology Laboratory, Department of Chemical Engineering, National Chung Cheng University, Chia-Yi 621, Taiwan, R.O.C. Chi-Chung.
Critical Phenomena in Random and Complex Systems Capri September 9-12, 2014 Spin Glass Dynamics at the Mesoscale Samaresh Guchhait* and Raymond L. Orbach**
Protein oligomerization in homogenous protein solutions Crosslinker:GlutaraldehydeOHC-CH 2 -CH 2 -CH 2 -CHO Y. Wang and O. Annunziata Langmuir, 24,
Ch 24 pages Lecture 9 – Flexible macromolecules.
FIG. 5.1 Multiple scattering is viewed as a random walk of the photon in diffusing wave spectroscopy (DWS)
Structural origin of non-Newtonian rheology Computer simulations on a solution of telechelic associating polymers J. Stegen +, J. Billen°, M. Wilson °,
Study of Pentacene clustering MAE 715 Project Report By: Krishna Iyengar.
Nigel Clarke Department of Chemistry Durham University Effect of Shear Flow on Polymer-Polymer Miscibility: Theoretical Advances and Challenges With.
Title: SHAPE OPTIMIZATION OF AXISYMMETRIC CAVITATOR IN PARTIALY CAVITATING FLOW Department of Mechanical Engineering Ferdowsi University of Mashhad Presented.
Pressure Quench of flow-induced crystallization Zhe Ma, Luigi Balzano, Gerrit W M Peters Materials Technology Department of Mechanical Engineering Eindhoven.
A computational study of shear banding in reversible associating polymers J. Billen +, J. Stegen *, A.R.C. Baljon + + Department of Physics, San Diego.
Predicting Engine Exhaust Plume Spectral Radiance & Transmittance Engineering Project MANE 6980 – Spring 2010 Wilson Braz.
利用小角度X光散射、動態光散射探討二氧化矽/聚環氧乙烷 懸浮液之結構與作用力
Pursuing the initial stages of crystal growth using dynamic light scattering (DLS) and fluorescence correlation spectroscopy (FCS) Takashi Sugiyama Miyasaka.
Light Scattering (pp in Shaw and pp in Hiemenz and Rajagopalan) Introduction Rayleigh Scattering Debye Scattering, Zimm Plots Dynamic.
COLLOID: ZETA POTENTIAL
Correlation of Solid Solubility for Biological Compounds in Supercritical Carbon Dioxide: Comparative Study Using Solution Model and Other Approaches Jaw-Shin.
Efficient control of the bulk and surface rheological properties by using C8-C18 fatty acids as co-surfactants Zlatina Mitrinova,1* Zhulieta Popova,1.
Chen-Yang Liu, Roland Keunings, Christian Bailly UCL, Louvain la Neuve, Belgium Dynamics of complex fluids: 10 years on, Cambridge, October Old.
Shear and Bulk Viscosities of Hot Dense Matter Joe Kapusta University of Minnesota New Results from LHC and RHIC, INT, 25 May 2010.
Two-phase hydrodynamic model for air entrainment at moving contact line Tak Shing Chan and Jacco Snoeijer Physics of Fluids Group Faculty of Science and.
Department of Chemical Engineering, National Chung Cheng University
Berat Molekul Polimer.
Shear banding in a simulated telechelic polymeric gel J. Billen, J. Stegen +, M. Wilson, A. Rabinovitch°, A.R.C. Baljon San Diego State University + Eindhoven.
Lab.343.
Aggregation-induced enhanced emission (AIEE) Myounghee Lee
Suspended Nanomaterials
Polymer Properties Exercise 1.
Lipid Molecules near a repulsive wall
Surfactant at Oil / Water Interface – Comparison with Simulation
Numerical Study of the Wall Slip Reduction Effects for a Double Concentric Cylinder Rheometer with Slotted Rotor D. De Kee, Department of Chemical and.
From Microscopic to Mesoscopic Descriptions:
Computer simulation of cell aggregation & growth on a tissue scaffold
Dynamic Light Scattering from Light Absorbing Solutions
Indrajeet Singh, Efrosyni Themistou, Lionel Porcar, Sriram Neelamegham 
Synthesis and Solution Processing of a Hydrogen-Bonded Ladder Polymer
Physical pharmacy Lab (6) Viscosity
Jan Genzer (Department of Chemical & Biomolecular Engineering)
Solvent-Temperature Superposition Rules for Predicting the Rheology of Wormlike Micellar Fluids Rajesh Khare, Department of Chemical Engineering, Texas.
工研院 講稿 11/9/2017 NAPLES: a practical pathway toward computer simulation of complex molten materials Complex Fluids & Molecular Rheology Lab., Department.
Lipid Molecules near a repulsive wall
Surfactant at Oil / Water Interface – Comparison with Simulation
Scarlet S. Shell, Christopher D. Putnam, Richard D. Kolodner 
Counterion Condensation and Collapse of Polyelectrolyte Chains
Presentation transcript:

Large aggregate species in conjugated polymer solutions characterized by dynamic light scattering and in situ rheological/flow turbidity measurements Chih J. Lin 1, Chan Y. Kuo 1, Chi C. Hua 1, * Show A. Chen 2 1 Department of Chemical Engineering, National Chung Cheng University, Chia-Yi 621,Taiwan, R.O.C. 2 Department of Chemical Engineering, National Tsing Hua University, Hsin-Chu 300, Taiwan, R.O.C. Date: 2008/07/01 Complex Fluids & Molecular Rheology Laboratory, Department of Chemical Engineering, National Chung Cheng University, Chia-Yi 621, Taiwan, R.O.C. Speaker: Chi C. Hua (華繼中)

Imagining PLED display Spin- coating Casting Ink-jet printing Films Electro-luminescent conjugated polymer film

Aggregation Properties in MEH-PPV Solutions Thermal irreversibility in the solution Viscosity — Existence of unstable aggregation properties Hua et al, J Rheol 49, 641 (2005) Poly[2-methoxy-5-(2’-ethyl- hexyloxy)- 1,4-phenylene vinylene] (MEH-PPV) M w : 70,000-10,000 g/mol PDI: 2.5 5mg/ml

Parameter-Free Coarse-Grained Simulations Which yields the exact (generally poor) solvent qualities for MEH-PPV solutions: Toluene: 0.32 Chloroform: 0.38 cf. Theta condition: MEH-PPV monomers per Kuhn length highly collapsed chain conformation

Dynamic Light Scattering (DLS)/Photoluminescence (PL): Effects of solvent quality and concentration M/T: 1 mg/mlM/T: 3 mg/ml, no filtrationM/C: 3 mg/ml, no filtration M/T M/C

In situ rheological/flow turbidity measuring apparatus Derived specific turbidity representation equation

Specific turbidity measuring theory Kerker, M., 1969, THE SCATTERIG OF LIGHT AND OTHER ELECTROMAGNETIC RADIATION, Academic Press, Inc., San Diego. Heller, W., and W. J. Pangonis, “Theoretical Investigations on the Light Scattering of Colloidal Spheres. I. The Specific Turbidity,” J. Chem. Phys. 26, (1956) Liberatore, M. W., and A. J. McHugh, “Dynamics of shear-induced structure formation in high molecular weight aqueous solutions,” J. Non- Newton. Fluid 132, (2005) Plot figure of specific turbidity vs. Mie radius So, quantity of Mie radius can get from equation of fitting curve.

Experimental design and procedure: DLS In-situ rheological/flow turbidity measurement Use DLS to measure hydrodynamic radius before shearing. Compared Mie radius with R h by two so different theory. Under shear flow 10 min Shear rate : 60 [s -1 ] Flow rested 15 min Under shear flow 10 min Shear rate : 151~2,800 [s -1 ] Flow rested 15 min Altered shear rate Under shear flow 10 min Shear rate : 60 [s -1 ] Flow rested 15 min Under shear flow 10 min Shear rate : 151~2,800 [s -1 ] Flow rested 15 min Run2 Run1 Altered shear rate MEH-PPV/DOP Sample Main ideal is changed experiment factors of conc. and aging time, to observe the influence of two factors on aggregated properties. Conc. [mg/ml] Aging time W/o aging2 days aging Experiment factors setting The run1 is observed the behaviors while samples under various shear flow field The run2 is observed the behaviors while samples experienced high shear flow field

Specific turbidity signal at various shear rate (w/o aging) 0.02 mg/ml0.3 mg/ml1.0 mg/ml3.0 mg/ml

Summary of specific turbidity (w/o aging) At the lowest concentration, i.e., 0.02 mg/ml, the fluctuation in specific turbidity was noticed to be very large, suggesting that the aggregation state is unstable. The specific turbidity decreased with increased sample concentration. In both shearing and relaxation region, the specific turbidity of 0.3 mg/ml and 1.0 mg/ml sample solutions were lower than those before the shearing treatment.

Specific turbidity signal at various shear rate (2 days aging) 0.02 mg/ml0.3 mg/ml1.0 mg/ml3.0 mg/ml

Summary of specific turbidity (2 days aging) Under sample with 2 days aging, the qualitative trends are the same as sample w/o aging. Signal fluctuation of the 0.3 mg/ml sample solution is very large in the relaxation region. Suggesting that the aggregation state become unstable after shearing treatment.

The effect of concentration on aggregation properties W/o aging2 days ageing

Summary of the effect of concentration With or without 2 days aging, Mie radius and increased with decreased sample concentration.

The influence of aging on aggregated properties 0.02 mg/ml0.3 mg/ml 1.0 mg/ml3.0 mg/ml Shear thinning Max.

Summary of aging influence All concentration samples have the same trend, the Mie radius and increased while sample with aging. The 3.0 mg/ml sample solution shows shear-thinning behavior whether sample w/o aging or with 2 days aging.

Comparison of results from flow turbidity and DLS measurements Aging effectConc. Mie radius from specific turbidity R h from dynamic light scattering Before shearing W/o aging 0.02 mg/ml mg/ml mg/ml mg/ml Aged 2 days 0.02 mg/ml mg/ml mg/ml mg/ml Good agreement was founded between the results from both measurements. The Mie radius was differed from R h in low concentration, 0.02 mg/ml.

Conclusion The aggregation properties of MEH-PPV solution precursor solution, as they highly depend on sample concentration and sample with or w/o aging. The results obtained from in-situ rheological/flow turbidity measurements and dynamic light scattering have great consistence.