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Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

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Page 1: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Chapter 2: Liquid CrystalsStates between crystalline and

isotropic liquid

Page 2: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Liquid Crystals, 1805-1922. Before discovery of LC, Lehmann designed a microscope that could be used to monitor phase transition process.

Page 3: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

1888 by Prof. Reinitzer, a botanist, University of Prague, Germany

Page 4: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

C11H23O CO2H

C S N I

84.5o 128o 139.5o

Phase Transition first defined by Georges Freidel in 1922

Page 5: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 6: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

The ordering parameterS=1/2<3cos2-1>

S=0, isotropicS=1, OrderedNematic, S=0.5-0.6

Page 7: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 8: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Classification of Smectic Liquid Crystals

A type: molecular alignment perpendicular to the surface of the layer, but lack of order within the layer.

B type: molecular alignment perpendicular to the surface of the layer, having order within the layer.

C type: having a tilted angle between molecular alignment and the surface of the layer.

Page 9: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Smectic B Liquid Crystals

Page 10: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Smectic C Liquid Crystals

Page 11: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Smectic A Liquid Crystals

Page 12: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

More Detailed Classification of Smectic Phases

Page 13: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Nematic Liquid Crystals

Page 14: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Cholesteric Phase Liquid Crystals

Page 15: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Polymeric Liquid Crystal

Page 16: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Advantages of Nematic Phase and Cholesteric Phase LC

For Display Propose

Low ViscosityFast Response Time

Page 17: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Discotic Liquid Crystals

Page 18: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 19: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Response to Electric and Magnetic Fields

Page 20: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

External Electric Field and Dielectric Properties of LC molecules

Page 21: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Dielectric Constant

L = C = q/V

Page 22: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Flow of ions in the presence of electric field

Internal Field Strength E = E0 – E’

Page 23: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

S = 0 1 > S > 0

Alignment of LC molecules in Electric Field

Page 24: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Dielectric Anisotropy and Permanent Dipole Moment

Page 25: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Dielectric Anisotropy and Induced Dipole Moment

easily polarized

Molecular axis

induced is large is large

induced is small

is small

+ -r//

+

-

r

dielectric constant along the direction perpendicular to the molecular axis

dielectric constant along the direction parallel to the molecular axis

Page 26: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Light is a high frequency electromagnetic wave and will only

polarize electron cloud.

In general, = > 0 or

Positive> 0 (10 to 20) Negative < 0 (-1 to -2)

For high electrical resistance materials, n is proportional

to 1/2

n = n n > 0 in general

n is a very important parameter for a LC device. Larger the n value, thinner the LC device and faster the response time

Page 27: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

O

S C N

C5H11

= +33

C - N - I76 98

O

O C7H15

C

N

C5H11 = - 4.0

C - N - I45 101

Examples

Page 28: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Magnetic Susceptibility and Anisotropy

Page 29: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Most of the organic molecules have closed-shell structure which is diamagnetic. In particular, the aromatic component will lead to a ring current that against the external magnetic field. Therefore the magnetic susceptibility is negative

//

large

small

Page 30: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 31: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Light as Electromagnetic Wave

Plane Polarized light can be resolved into Ex and Ey

Page 32: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 33: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 34: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Birefringence

Page 35: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Ordinary light travels in the crystal with the same speed v in all direction. The refractive index n0=c/v in all direction are identical.

Extraordinary light travels in the crystal with a speed v that varies with direction.The refractive index n0=c/v also varies with different direction

Page 36: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Generation of polarized light by crystal birefringence

Page 37: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Interaction of Electromagnetic Wave with LC Molecules

Page 38: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

E field

Induced dipole by electromagnetic wave

Propagation of the light is hindered by the molecule

Speed of the light is slowed down

= C ///

//

Page 39: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

E field

Induced dipole by electromagnetic wave

Propagation of the light parallel to the molecular axis

Change of the speed is relatively small

// = C// /

//

Page 40: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Circular Birefringence

Page 41: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 42: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 43: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Reflection of Circular Polarized Light

Page 44: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Devices for Liquid Crystal Display

Page 45: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Designs of LC cell

Electronic DriveAM: active matrix; TFT: thin film transistor; MIM: metal-insulator-metal

Page 46: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Alignment of LC molecules in a Display Device

Page 47: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 48: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Dynamic Scattering Mode LCD Device

Page 49: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Twisted Nematic (TN) Device 1971 by Schadt

Page 50: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Optical Response of a Twisted Nematic (TN) Device

Applied voltages and optical response

Page 51: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Super Twisted Nematic (STN) LC Device 1984 by Scheffer

By addition of appropriate amounts of chiral reagent

Twisted by 180-270 o

N:Number of row for scanningVs: turn on voltageVns:turn off voltage

Page 52: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Sharp change in the voltage-transmittance curve

Page 53: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Electrically Controlled Birefringence (ECB) Device (DAP type)

Page 54: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 55: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Black and White RF-STN Device

Page 56: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 57: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Optical response of Nematic LC in a Phase-ChangeGuest-Host Type Device (by G. Heilmeier)

Page 58: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Phase Change (PC) in a Guest Host (GH) LC Device

Page 59: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

In-Plane Switching (IPS) type LC Device

Page 60: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Polymer Dispersed Liquid Crystal (PDLC) Device

Page 61: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Polymeric Nematic LC Materials

Page 62: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Active Matrix LCD

Page 63: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Structure of a typical LC Display

Page 64: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 65: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Hybrid Aligned Nematic (HAN) type

Fast response time,Upto ms scale.

Page 66: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Full color reflective display

Page 67: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

References(1) Liquid Crystals, P. J. Collings, Princeton(2) Introduction to liquid crystals, P. J. Collings and M. Hird, Taylor and Francis(3) Flat Panel Displays, J. A. Connor, RSC.

Page 68: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Structure of rigid rod like liquid crystal molecules

Core group: usually aromatic or alicyclic; to make the structure linear and rigidLinker: maintaining the linearity and polarizability anisotropic.Terminal Chain: usually aliphatic chain, linear but soft so that the melting point could be reduced. Without significant destroy the LC phase. Note that sometimes one terminal unit is replaced by a polar group to provide a more stable nematic phase.Side group: to control the lateral interaction and thereore enhance the chance for nematic. Note that large side groups will weaken the lateral interaction

Page 69: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Linker A, B -(CH=N)-; -(N=N)--(N=NO)-; -(O-C=O)-

Terminal Group X, YNon-polar flexible groups

-R, -OR, -O2CRPolar rigid group

-CN, -CO2H, -NO2, -F, -NCS

Core Group

Common components for LC molecules

Side Branch-F, -Cl, -CN, -CH3

Page 70: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Character of LC molecules

(1) Rod like or Discotic(2) Empirical Length/Diameter parameter for LC phase

4 (Flory theory predicted critical L/D ratio = 6.4; Onsager theory predicted critical L/D ratio = 3.5)

(3) Having polar or highly polarizable moiety(4) Large enough rigidity to maintain the rod or discotic l

ike structure upon heating(5) Chemically stable.(6) Phase transition temperature is determined by H an

d S. At TCN or TNI, Go = Ho –TSo= 0. Therefore TCN= Ho

CN/SoCN and TNI= Ho

NI/SoNI

Page 71: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

n

L/D > 4 Ti > Tm (nematic)

L

D

No. of Phenyl ring L/D Ti Tm2 2 773 3 2134 3.9 3205 4.8 445 3886 5.5 565 438

Page 72: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

When the length of the molecules increases, van der Waal’s interactions that lead to thermal stability of the nematic phase increases. When L/D goes over the critical value, nematic phase appears.

In the above examples, the critical L/D is around 4. When L/D = 1, 2, or 3, no LC phase was observed.

Page 73: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

O

O

O

O

n DL

n L/D Ti Tm

1 3.8 1322 5.1 254 1763 6.4 464 220

Nematic phase could not be observed until L/D >4

Flexible linker

6-10 o67 o

Page 74: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

6-10 o67 o

This type of linker group is more flexible. Entropy gain is more effective in isotropic liquid state. Therefore SN-I is relatively large, leading to a low Ti. In the presence case, even for the LC molecules having the L/D upto 5.1, the Ti is only 254 oC

Page 75: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Other Options for the core group.

Page 76: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Thermal Stability:

Low TC-N; high TN-I

larger T = TN-I - TC-N , higher the stability of the LC state

In general, shorter the LC molecule, lower the phase transition temperature it has.For LC molecule contains more polarizable aromatic cores, or longer the body, Vander Waals interactions between LC molecules will increase. This will lead to higher thermal stability.

Crystal Nematic LC Isotropic LiquidTC-N

TN-I

T

Page 77: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

(1) Nematogenic: structures that lead to nematic phase as the only LC phase

(2) Smectogenic: smectic phase is the only mesophase exhibited

(3) Calamitic: Both nematic and smectic phases would exhibited.

Page 78: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Smectic Phase

Smectic LC phase: Lamellar close packing structure are favored by a symmetrical molecular structure; Wholly aromatic core-alicyclic core each with two terminals alkyl/alkoxyl chains compatible with the core ten to pack well into a layer-like structures and generates smectic phase.

Long alkyl/alkoxyl chain would lead to strong lateral interactions that favors lamellar packing smectic phase formation.

RO

OHR

O

HO

R = C5H11 TCN = 88; TNI=126.5

R = C8H17O TCS = 101; TSN = 108; TNI=147

R = C10H21O TCS = 97; TSN = 122; TNI=142

Page 79: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Terminal groups for smectic phase

(1) Salts from RCO2H/RNH2

(2) Terminal groups contain -CO2R, -CH=CHCOR, -CONH2, -OCF3, -Ph, -NHCOCH3, -OCOCH3

N CH

C8H17O X

Page 80: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

N CH

MeO XShort chain

Terminal group for nematic

Page 81: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

For Smectic Phase

NHCOCH3 > Br > Cl > F > NMe2 > RO > H > NO2 > OMe

For nematic Phase

NHCOCH3 > OMe > NO2 > RO > Br~ Cl > NMe2 > Me >F > H

-CN,-NO2 -MeO are nematogen: poor smectic/good nematic-NHCOCH3, halogen, -NR2, good smectic/nematic

Page 82: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Nematic Phase.

(1) Due to its fast response time, the nematic LC phase is technologically the most important of the many different types of LC phase

(2) The smectic phases are lamellar in structure and more ordered than the nematic phase.

(3) The smectic phases are favored by an symmetrical molecular structure.

(4) Any breaking of the symmetry or where the core is long relative to the overall molecular length tends to destabilized the smectic formation and facilitate the nematic phase formation.

Page 83: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

(1) At least two rings are required to enable the generation of LC phase.

(2) The nematic phase tends to be the phase exhibited when the conditions for the lamellar packing (smectic) cannot be met.

(3) Molecular features for nematic phase: (a) breaking of the symmetry or (b) short terminal chain.

Page 84: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 85: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

C N TiTm Ti

24 35

130 239

84 127

68 130

71 (52)

204

95

3.5

34

Page 86: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

NC R

H

H

NC H

H

R

No LC phase

Stereochemistry of alicyclic systems

Page 87: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

CNC5H11

CNC5H11

CNC5H11

CNC5H11

C N ITm Ti

48

24

31

62

61

35

55

100

Change in the core structure of one phenyl ring for a range of non-aromatic rings only leads to increasing Tm and Ti, indicating that packing effect is more important than the polarizability effect for nematic phase. The ring functions in a space-filling manner, preventing the molecule form tumbling and maintaining the orientational ordering.

Page 88: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 89: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Heteroatomeffects

The heteroatoms enhances the polarity and higher melting point are seen. Nematic phase transition temperature is low than the melting point. The large sulfur atom further disrupts the nematic packing. The flexible sulfur containing ring gains more entropy from N to I and therefore lead to lower TNI.

Page 90: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

UnsymmetricalTNI = 19 oC

Flat moleculeTNI = 55 oC

Symmetrical but rings are perpendicularTNI = 28 oC

MM2 space-filling models

Page 91: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

The TCN and TNI orders: dicyclooctane > cyclohexane > phenyl

Page 92: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

MM2 calculation

Linearstructure

Bent structure

Page 93: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Extending the number of the rings

Page 94: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Linking group:

Linking groups are used to extend the length and polarizability anisotropy of the molecular core in order to enhance the LC phase stability by more than any increase in melting point, producing wider LC phase ranges.

(A) Linking group should maintain the linearity of the molecule.

(CH2)nR R

R = N CH

OCH3

where

n Tm Ti

0 266 >390

1 - -

2 171 3123 - -

4 156 2705 - -

Page 95: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Odd number of CH2: Bent

Even number of CH2: Linear

Page 96: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

(b) Linker groups that connect aromatic core units with the conjugation extended over the longer molecules. This could enhance the polarizability anisotropy.

Page 97: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Other common linker groups

O

O

O O

O

e.g.

C5H11

O CN

O

C5H11

CN

Tm Ti

48

30

79

51

Amide linker cannot be used due to the strong hydrogen bond interactions that lead to high melting temperature

Page 98: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Terminal Flexible Long Chain:

The function of the terminal flexible long chain is to suppress the melting point without serious destroying the LC phase.

Page 99: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 100: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 101: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 102: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Lateral Substitution

Lateral substitution is important in both nematic/smectic systems. However, because of the particular disruption to the lamellar packing, necessary for smectic phases, lateral substitution nearly always reduces smectic phase stability more than nematic phase stability except when the lateral substitutions lead to a strong dipole-dipole interaction.

Page 103: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 104: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 105: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 106: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

CO2HC8H17O

X Not quite linear for some substituents

Page 107: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid
Page 108: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Electronic effects arising from the lateral groups

Page 109: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

CO2HRO

R = Me or Et

Doesn't show LC properties

RO

O

OH

OR or R'

O

HO

LC

Mixing of two Components may generate a LC phase

Page 110: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Mixture of two Components

N C4H9

RO

MBBA R = MeEBBA R = Et

A mixture of MBBA (60%) and EBBA (40%) would lead to LC at room temperature

Page 111: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Cl

H

CH3(CH2)12CO2

H

Left

Right

Temperature Dependent Rotation of the Cholesteric Phase

Page 112: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Main Chain Liquid Crystal Polymer

mesogenic unit flexible linker

Side Chain Liquid Crystal Polymer

Polymer Backbone

Polymer Backbone

Terminally attached

Laterally attached

Page 113: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Combined Liquid Crystal Polymer

Page 114: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Lyotropic Liquid Crystal Polymers

Fairly rigid rod like polymers; but soluble in certain solvents to form a LC phase

NHHN

O O

Kelver

HN

O

PBA

Page 115: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Dissolve and LC formation

Fiber formation to give high tensile strength fibers

Common Components for Lyotropic Liquid Crystals

N

ON

O N

SN

S

Page 116: Chapter 2: Liquid Crystals States between crystalline and isotropic liquid

Examples

N

SN

S nPoly(p-phenylenebenzobisthiazole) PBT

Soluble in PPA or H2SO2 and could be fabricated as high tensile strength polymeric wires

N

ON

O n