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Understanding liquid crystal

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Title: Understanding liquid crystal


1
Understanding liquid crystal
  • PHY0411A
  • Jiang Han
  • Fong King Sing

2
Contents
  • Introduction
  • Different phase
  • Physical properties
  • Application

3
States of matter
  • Solid
  • Definite shape
  • Particles are packed closely together to form
    crystal structure
  • Particles cannot move freely, only vibration is
    possible

4
States of matter
  • Liquid
  • No definite shape but definite volume
  • Particles can vibrate, move about, and slide past
    each other

5
Phase change of matter
  • Normal matter
  • Temp?
  • Single phase change
  • crystalline solid ? isotropic liquid
  • Some organic molecules
  • Temp?
  • Multiple phase change
  • crystalline solid ?mesophase(s) ? isotropic
    liquid

6
Liquid Crystals
  • Some organic molecules were found to exhibit one
    or more mesophases
  • Such mesophases were classified into two types
  • Disordered Crystal Mesophases
  • Ordered Fluid Mesophases ? Liquid Crystal

7
Liquid Crystals
  • In ordered fluid mesophases, matters have
    properties between those of a conventional
    liquid, and those of a solid crystal. For
    instance, a liquid crystal can flow like a
    liquid, but have the molecules in the liquid
    arranged and/or oriented in a crystal-like way

8
Classification of LC phase
  • Liquid crystals can be divided into two types
    according to how they are formed
  • Lyotropic LCs
  • exhibit phase transitions as a function of
    concentration of the mesogen in a solvent as well
    as temperature
  • Thermotropic LCs
  • exhibit a phase transition into the LC phase as
    temperature is changed
  • We will only discuss thermotropic LCs in this
    presentation

9
Phases of Thermotropic LCs
  • Nematic phases
  • Smectic phases
  • Chiral phases

10
Nematic phase
  • Molecules have no positional order, but they have
    long-range orientational order
  • Molecules flow and their center of mass positions
    are randomly distributed as in a liquid, but they
    all point in the same direction

11
Smectic phase
  • At temperatures below the nematic phase, the
    liquid crystal material may gain an amount of
    positional order it transforms into smectic
    phase
  • In such phase, molecules still form a fluid, but
    prefer to lie on average in layers
  • Within each layer the liquid crystal is
    essentially a 2-dimensional nematic liquid crystal

Smectic A
Smectic C
12
Smectic phase
  • There are over 10 types of smectic phase, we name
    it Smectic A, B, CThe most common ones are A and
    C
  • When the nematic-like director in each layer is
    parallel to the layer normal the material is
    Smectic A
  • If this director tilts away from the layer normal
    the Smectic C phase is formed

Smectic A
Smectic C
13
Smectic phase
  • The positional ordering may be described in terms
    of the density of the centers of mass of the
    molecules, where z is the coordinate parallel
    to the layer normal, the average density of the
    fluid is ?0 , d is the distance between layers
    and is the order parameter.

14
Strength of the smectic order
  • ? measures the strength of the smectic order
  • When ?0 there is no layering and the material
    is nematic
  • If ?gt0 then some amount of sinusoidal layering
    exists and the material is smectic

15
Physical Properties of LC
  • To understand a material
  • Electronic response
  • Dielectric permittivity
  • Refractive index
  • Mechanical response
  • Elastic constant

16
Physical Properties of LC
  • Director of a LC
  • Liquid crystal are composed of rod-like molecules
  • Long axes are aligned to one another
  • Represent the direction of preferred orientation
    of molecules

17
Physical Properties of LC
  • Order parameter
  • In long range, liquid crystals have no position
    order, but still have orientation order
  • Molecules share the same director, but
    distribution of angle can be different

18
Physical Properties of LC
  • Order parameter
  • Define an order parameter to quantify the
    orientational order
  • Typical value 0.30.9
  • Reduce to 0 at liquid crystal-liquid phase
    transition

19
Physical Properties of LC
  • Elastic continuum theory
  • The material is treated as a continuum
  • Ignore molecular details
  • Useful in studies of their mechanical properties,
    eg. response to twist, bend ...
  • Assume order parameter is constant

20
Electric Properties
  • Electric displacement
  • Energy density depends on
  • Larger e , larger induce dipole
  • Difference in e give reason for rotation of LC

LC director n
21
Electric Properties
  • Consider non-polar compound
  • Torque is provided
  • Useful in LCD

E
??(?-??) gt 0
?gt??
?gt ??
??(?-??) lt 0
E
?lt??
?lt ??
22
Electric Properties
  • Typical relation of dielectric constant on
    temperature
  • Decrease with temperature
  • Recall order parameter

4-n-pentyl-4'-cianobiphenyl
23
Optical Properties
  • Review
  • If EM wave Poynting vector in
    z-directionVector in x-direction
  • Refractive index depends on permittivity
  • It is easier to polarize materials along their
    anisotropy axis
  • Dielectric displacement can be nonparallel to
    electric field , i.e. polarization also

24
Optical Properties
  • Nematic phase
  • Uniaxial LC has two refractive indices
  • Ordinary refractive index
  • Electric vector vibrates perpendicular to the
    optical axis
  • Extraordinary refractive index
  • Electric vector vibrates parallel to the optical
    axis
  • Practically,
  • Positive birefringence effect

LC director n
25
Optical Properties
  • Chiral nematic phase
  • The optical axis of chiral nematic is the helix
    axis
  • Circular orientated liquid crystal
  • Light exhibits circular polarization

26
Mechanical Properties
  • A liquid crystal experiences 3 distortions
  • Response to the distortion is described by 3
    elastic constant, K11, K22, K33

27
Mechanical Properties
  • Splay
  • Mathematical description

28
Mechanical Properties
  • Twist
  • Mathematical description

29
Mechanical Properties
  • Bend
  • Mathematical description

30
On the surface
  • Liquid crystals may have different surface
    alignment
  • Energy is needed to move the director from its
    easy axis
  • The magnitude depends on the anchoring angle

31
  • What so important about the above parameters
  • Determine the free energy of liquid crystal
  • Useful in application

32
Energy of liquid crystal
  • Free energy density

Energy due to external field (E, M, EM field)
Energy due to distortion
Coupling energy of LC to the surface
33
Energy of liquid crystal
  • We have the equation for free energy
  • In principle, we can minimize it to calculate the
    equilibrium state of the liquid crystal (static)

34
Application of LCs
  • Liquid Crystal Display (LCD)
  • Thermometers
  • Some LCs change its color at different
    temperature, used in aquarium and pool
  • Liquid crystal sheets are often used in industry
    to look for hot spots

35
Liquid Crystal Display (LCD)
  • Widely used display technology nowadays
  • Calculators
  • Digital clock, watches
  • Laptop computers
  • PDAs
  • Mobile phones
  • TVs
  • etc

36
Four facts that make LCD works
  • Light can be polarized
  • Liquid crystals can transmit and change polarized
    light
  • The structure of liquid crystals can be changed
    by electric current
  • There are transparent substances that can conduct
    electricity

37
Twisted nematic field effect
  • First discovered in 1970

38
Principle of LCD
39
Summary
  • Liquid crystal is a mesophase
  • Different phases of liquid crystal
  • Highly anisotropic, its response to physical
    processes depend on orientation
  • Special optical property
  • Various application

40
END
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