2004-10-258CB Layers at Different Temperature 1 “Formation of Liquid Crystalline Phases from a Langmuir Monolayer” By K.A. Suresh and A. Bhattacharyya.

Slides:



Advertisements
Similar presentations
Metamorphic Rocks. Metamorphic Rock Formation: As the Earth moves, all types of rock can be pushed deep into the Earth. These rocks are exposed to extreme.
Advertisements

C6 Liquid Crystals.
Soft bend elastic constant and transition to a modulated nematic phase Alenka Mertelj, 1 Martin Čopič, 1,* Geoffrey R. Luckhurst 2, R. P. Tuffin 3, and.
Nanocamp June 27, 2012Chris Marin. What is a liquid?  All liquids:  have a definite volume  conform to the shape of container  are not compressible.
Dynamics and Structure of Smectic Liquid Crystal Multilayers at the Air/Water Interface P.Basnet * L.Zou * J.Wang * V.Beleva * A.Bernoff † J.Alexander.
Collecting Latex from a Rubber Tree Natural rubber production begins with the collection of latex, a milky white substance produced by the cells of several.
DCMST May 23 rd, 2008 Liquid Crystals Gavin Lawes Wayne State University.
Time Dependence of Liquid Crystal Orientational Memory Effect at a Polymer Surface Frederick Davey, Joel Pendery, Sameh Ferjani Principal Investigator:
Wetting of Liquid Crystal Surfaces and Induced Smectic Layering at the Nematic-Liquid Interface* Masafumi Fukuto, 1 Oleg Gang, 2 Kyle J. Alvine, 3 Benjamin.
L IQUID C RYSTALS P AUL D UPIANO M ANDEEP S INGH.
Author: Tim Verbovšek Mentor: doc. dr. Primož Ziherl.
ADSORPTION. Surface Activity of Solutes Solute, c  oo Solutes that decrease surface tension are called “surfactants”  Solute, c.
Introduction We applied a new, simplified model of the dynamics of molecular layers to derive the line tension of 8CB multilayers from the relaxation of.
1 Example of PDLC architectural window. 2 Polymer Dispersed Liquid Crystal (PDLC)
Hole Dynamics in Polymer Langmuir Films Lu Zou +, James C. Alexander *, Andrew J. Bernoff &, J. Adin Mann, Jr. #, Elizabeth K. Mann + + Department of Physics,
Phase Difference = Phase Difference = 0.05.
Hole Dynamics in Polymer Langmuir Films Lu Zou +, James C. Alexander *, Andrew J. Bernoff &, J. Adin Mann, Jr. #, Elizabeth K. Mann + + Department of Physics,
Liquid Crystals.
I. Brief introduction Several questions to ask in this course: 1. What is the objective of the course - “introduction to crystal structure and diffraction.
VISUALISATION OF DOMAINS IN 2D MOLECULAR SYSTEMS BY BREWSTER ANGLE MICROSCOPE J. Cirák.
Science Update Programme Liquid Crystals and Their Applications
Side Chain Liquid Crystalline Polymers Polymers with mesogens attached as side chains can exhibit liquid crystalline properties. The extent to which.
Contents of the Lecture
Liquid Crystals: Structure, Properties and Applications
New frontiers in anisotropic fluid–particle composites by Susanne Klein, Peter Raynes, and Roy Sambles Philosophical Transactions A Volume 371(1988):
1.1 The World of Liquid Crystal Department of Chemistry Yonsei University Moon-Gun Choi.
Polar Planar vs. Polar Vertical Reverse Tilt Domain Walls Charles Rosenblatt, Case Western Reserve University, DMR Left: Polarized photomicrograph.
Interfacial Characteristics of Semi fluorinated Polymers Dvora Perahia (Clemson University) DMR Thin layers of semifluorinated and fluorinated.
Two models for the description of light The corpuscular theory of light stating that light can be regarded as a stream of particles of discrete energy.
My Book These images are grouped. You may find it easier to ungroup and work with them.
Molecular structure of calamitic LCs rigid ring systemsterminal groups bridging groups (+linking groups) terminal groups (+linking groups) phenyl biphenyl.
Liquid Crystals at Nanopatterned Surfaces. AFM Contact Nanolithography AFM used as a probe of the surface topography.
May 24, 2005 Advanced Liquid Crystal Technologies, Inc. 1 Liquid Crystalline Elastomers as Artificial Muscles P.E. Cladis Advanced Liquid Crystal Tech.
Complex Fluids Group University of São Paulo, Brazil LYO-BANANA MESOPHASES COMPOSED BY A MIXTURE OF APOLAR SOLVENTS AND BENT- SHAPED MOLECULES O. G. Martins.
Liquid Crystal Materials. Lyotropics Thermotropics amphiphilic molecules, polar and non-polar parts form liquid crystal phases over certain concentration.
LIQUID CRYSTALS Introduction Introduction LC mesophases LCs in the bulk and in confined geometries optical properties of LCs fluctuations and light scattering.
How are Liquid Crystals like Superconductors? Charles Rosenblatt, Case Western Reserve University, DMR Many seemingly different phase transitions.
Liquid crystals : The fourth state of matter Thierry Chuard, LLB, Universität Bern.
Images for reflection. Que
Image from
Liquid Crystals Thermotropic (temperature dependent)
Soft Condensed Matter Physics.
Waves.
MVGR College of Engineering
2D Phase Transition in Monolayer Germanium Selenide
Liquid Crystal Properties of Aggregated Dyes
4EOBBA/2RP/nSBZ Networks Results/Observations Synthetic Methodologies
Liquid Crystals The Fourth State of Matter? Dr. Vance Williams
Literature seminar Yuna Kim
Laser- and Electric-Field-Induced Nucleation in Supersaturated Solutions and Supercooled Melts Bruce A. Garetz, Department of Chemical & Biological Sciences,
Can Liquid Crystals / Polymers
Liquid-Crystalline Collapse of Pulmonary Surfactant Monolayers
Coralie Alonso, Alan Waring, Joseph A. Zasadzinski  Biophysical Journal 
The Microscope.
Juan M. Vanegas, Maria F. Contreras, Roland Faller, Marjorie L. Longo 
Biodegradable Melt processable liquid crystalline polyesters
Another Example: Aluminum chloride, Al2Cl6, can be made by the reaction of aluminum with chlorine according to the following equation:                        2.
Competition Between Mesogens in Pyridone-based Supramolecular Calamitic, Banana and Discotic Liquid Crystals.   Kurt N. Wiegel, Department of Chemistry,
Metamorphic Rocks.
Yuna Kim thermotropic liquid crystals where one compound exhibits both calamitic and discotic mesomorphism with the change of molecular shape.
Angew. Chem. Int. Ed. 2014, Early view
Phase Separation Kinetics of Polymer Dispersed Liquid Crystals (PDLC) on a Chemically Heterogeneous Substrate Polarized optical micrograph of the formation.
Physical and Chemical Changes
IRG-2: MAPLE of Polymer Films for Morphology Control (DMR ) Craig Arnold, Lynn Loo, Rodney Priestley, Princeton University Substrate (Si) crystal.
Photoresponsive chiral dopant
Yasuo Norikane,a Yuki Hiraib and Masaru Yoshida
Fig. 1 1T-TaS2 single crystals with reduced thickness.
Large-screen Television Vision Technology
Liquid Crystal Formation in Supercoiled DNA Solutions
Introduction Although the LC mixtures composed of nematic or cholesteric liquid crystals (LCs) and azobenzene compounds have been comprehensively studied,
Presentation transcript:

CB Layers at Different Temperature 1 “Formation of Liquid Crystalline Phases from a Langmuir Monolayer” By K.A. Suresh and A. Bhattacharyya Langmuir 1997, 13,

CB Layers at Different Temperature 2 Phase Transition of 8CB in Bulk (3D) Crystal 20.5 o C Smectic A 33.3 o C Nematic 41.5 o C Isotropic Temperature

CB Layers at Different Temperature 3 Typical Isotherm at 25 o C (T < 28 o C)

CB Layers at Different Temperature 4 Isotherm at 30 o C (28 o C < T < 36 o C)

CB Layers at Different Temperature 5 Isotherm at 40 o C (36 o C < T < 36 o C)

CB Layers at Different Temperature 6 Images under Fluorescence Microscope 25 o C 30 o C Area/Molecule = 10 A 2 1~40 um

CB Layers at Different Temperature 7 Images under Reflection Microscope 25 o C30 o C~28 o C Area/Molecule = 10 A 2 Thickness = Nλ/(2n)

CB Layers at Different Temperature 8 Images under Polarized Microscope 30 o C, 10 A 2 A/M  Nematic Phase Schlieren Textures Boojum-like Textures

CB Layers at Different Temperature 9