Title: From —liquid crystal thermometers
1From liquid crystal thermometers
2LC thermometer
- Hold a liquid crystal thermometer card over your
hand and observe it as it warms up. Notice that
it starts out black, then becomes red, yellow,
green, blue then black once again. Liquid
crystals can be adjusted by the manufacturer to
change colors over different temperature ranges,
but 30 C to 35 C seems to be a common range. - The molecules in the liquid crystal thermometer
are made of cholesterol, and are called
cholesteric liquid crystals. The molecules are
rod-shaped. The rods form layers in the liquid
crystal, the rods in adjacent layers running in a
slightly different direction from those in the
layer above or below. From one layer to the next
the rods form a structure like the stairs of a
spiral staircase. The spiral staircase rises
through some distance before the molecules twist
around parallel to their original direction. When
this distance equals half-a-wavelength of red
light, the liquid crystal will reflect red light.
When the distance is shorter, matching half a
wavelength of blue light, the crystal will
reflect blue light. (The wavelength of light is
measured in the liquid crystal and is shorter
than the wavelength in air.) - This seemed strange to me at first. Why should
cold crystals with closely spaced layers reflect
red light and warmer more spread out layers
reflect blue light? The resolution of this
problem came when I found out that the
temperature effects not only the spacing of the
layers but the twist angle from one layer to the
next. When the liquid crystal warms up the layers
spread apart slightly, but, in addition, each
layer of rods rotates a little more relative to
the later below it. This means it takes fewer
layers and therefore a shorter distance between
layers of parallel rods. So when the temperature
increases the spacing between layers in which the
rods are parallel decreases. The color goes from
red when cold to blue when hot. - The liquid crystals are usually encapsulated,
packaged in microscopic plastic spheres. This
allows the material to be cut. they are also
thermally rugged which allows them to be
laminated to protect them from hard handling in a
high temperature laminating machine.
http//www.exo.net/pauld/activities/liquidcrystal
/liquidcrystal.html
3Liquid Crystal Sensors for Chemical Detection
4Other methods
- Spectroscopy methods (Mass spectroscopy, gas
chromatography, infrared spectroscopy) can give
precise and quantitative detection, however they
are bulky, complex to provide real-time, portable
detection. - Electrochemical sensors (such as electronic nose)
and optical sensors can be designed to detect gas
analyte fast and effectively. - Liquid crystal sensor is another option for
chemical detection which is usually based on
simple mechanisms and instrumentations.
5Outline
- Introduction of liquid crystals
- 4 type of liquid crystal sensors for chemical
detection - Type 1Nematic LC shifting for signal
amplification - Type 2Cholesteric LC sensors (color change)
- Type 3Discotic LC sensors (conductivity change)
- Type 4Lyotropic LC shifting for signal
amplification - Comparison and Conclusion
6Introduction of Liquid Crystals
- Liquid crystal phase is intermediate form between
crystalline solid and isotropic liquid. It has
some special properties - Individual molecules always have anisotropic
shape (rodlike, disk-like), dielectric constant,
reflective indices - Molecular arrangement posses some degree of
positional order or orientational order - Molecular alignment can be affected by external
fields (electric, magnetic, shear stress or
surface anchoring)
Thermotropic Liquid Crystals
7Calamatic Liquid Crystals
Nematic phase
smectic phase
cholesteric phase
- Nematic LC molecules have orientational order.
The direction can be controlled by alignment film
and external field. - Cholesteric LC pitch length can be changed by
temperature and interaction with chemicals.
8Nematic LC Sensors
Fig. 3 (A) Schematic illustration of the change
in surface roughness caused by the binding of
molecules of Av (left) or lgG (right) to ligands
hosted within a SAM of molecules supported on
gold film. (B) Scanning tunneling microscopy
image of the surface of a thin (10nm)
semitransparent, obliquely deposited (50? from
normal) gold film prepared by electron beam
evaporation onto a glass substate at 0.02 nm/s.
(C) Profile of the surface of the gold along the
black line shown in (B).
V. K. Gupta, N. L. Abbot, Langmuir, 12, 2587,
1996 V. K. Gupta, J. J. Skaife, T. B. Dubrovsky,
N. L. Abbot, Science, 279, 2077, 1998
9Nematic LC Sensors
Nematic liquid crystals can be used to amplify
and image transducer receptor-mediated binding of
proteins at surfaces. Nanometer scale
topographies on the surfaces could be overwhelmed
by the specific binding of proteins to surface
immobilized ligands, thus leading to microscopic
changes in the orientations of LCs aligned by
these surfaces.
Fig. 4. Optical images (light transmitted through
crossed polarizers) of nematic LC sandwiched
between mixed SAMs formed from BiSH and C8SH with
or without bound proteins.
V. K. Gupta, J. J. Skaife, T. B. Dubrovsky, N. L.
Abbot, Science, 279, 2077, 1998
10Nematic LC Sensors
- Selective binding of analyte and receptor
immobilized on the surface can also change
interaction (binding) between LC and surface. - The resulting optical signal can easily be
observed by the naked eye due to amplification by
the LC molecules long-range order. - Combination of surface design and receptor
selection can make this sensor applicable to
various chemicals.
R. R. Shah, N.L. Abbott, Science, 293, 1296, 2001
11Nematic LC Sensors
R. R. Shah, N.L. Abbott, Science, 293, 1296, 2001
12Nematic LC Sensors
- Because LC molecules have high mobility of
liquids, information about the binding of analyte
and receptor at surfaces propagates rapidly from
the surface into the bulk of the LC (transduction
and amplification can occur in a few seconds). - The ligands on the substrate can be tailored to
reversibly bind with the LC molecules and
analytes.
R. R. Shah, N.L. Abbott, Science, 293, 1296, 2001
13Cholesteric LC Sensors
Cholesteric LCs can selectively reflect light of
wavelengths equal to the pitch length (?Rnavep).
Organic vapors can be incorporated between the
layers of a cholesteric liquid crystal, changing
its pitch length and, therefore, its color.
A glass disk was used as substrate for
preparation of the CLC films. Its reverse side
was made black to absorb unscattered light. In
order to prolong the lifetime of liquid crystal
sensor (decrease evaporation and mechanical
drifting), the liquid crystal films can also be
immobilized in PVC and silicone rubber.
I.M. Raimundo Jr., R. Narayanaswamy, Analyst, 124
(1999) 16231627.
14Cholesteric LC Sensors
- The optical properties of the sensing phase
can be tuned by changing the composition of the
CLC mixture, altering the sensitivity and
selectivity for different organic vapors. - The lifetime of the CLC layer is not long
(lt200 mins). To overcome this drawback, the
liquid crystal films could be encapsulated in PVC
or silicone rubber, if the CLC is maintained in
small domains dispersed in the polymeric film.
Fig. 6 Effect of the solvents on the reflectance
spectra of the 0.18 CC 0.82 CN films (top)and
0.22 CC0.78 CN films (bottom).
D. A. Winterbottom, R. Narayanaswamy, I. M.
Raimundo Jr., Sensors and Actuators B, 90, 52,
2003
15Discotic Liquid Crystals
discotic liquid crystals
- Discotic LC molecules typically consist of an
aromatic core surrounded by hydrocarbon side
chains. - The center of the molecular stack is electron
rich and relatively conductive in nature, whereas
the outer layer is relatively insulating.
16Discotic LC Sensors
Gold electrode
- Charge carrier can move easily along the
columns, with relatively high mobilities, but
charge carrier motion between columns is greatly
hindered by the intervening hydrocarbon chain
region. - Molecules at the surface have many more degrees
of freedom and are able to undergo orientational
and positional fluctuations. This leads to a
considerably enhanced conductivity compared with
the bulk. - Disturbances such as the absorption of
volatiles will have a very strong effect on these
fluctuations, giving discotic liquid crystals
their sensitivity to the presence of volatiles.
Silicon Substrate
DLC film
J. Clement, N. Boden, T. D. Gibson, R. C.
Chandler, J. N. Hulbert, E. A. Ruck-Keene,
Sensors and Actuators B, 47, 37, 1998
17Discotic LC Sensors
- DR R0 is positive for all alkane hydrocarbons.
The tentative explanation is that the alkane
volatile dissolves into the alkyl side chain
region of the discotic surface, disrupts the
reorientational and positional fluctuations of
the molecules, thus increasing the surface
resistance. The longer the alkane chain length,
the greater the disruption of the fluctuations,
and the greater the measured resistance. - Other volatiles, such as benzene for instance,
decrease the surface resistance of the discotic
liquid crystal. This is presumably due to their
affinity for the aromatic core region where they
assist the transport of charge from aromatic core
to aromatic core.
J. Clement, N. Boden, T. D. Gibson, R. C.
Chandler, J. N. Hulbert, E. A. Ruck-Keene,
Sensors and Actuators B, 47, 37, 1998
18Discotic LC Sensors
The response to saturated water vapor is
negligible. This insensitivity to the presence of
water is primarily due to the hydrophobic nature
of the surface of the discotic liquid crystals.
J. Clement, N. Boden, T. D. Gibson, R. C.
Chandler, J. N. Hulbert, E. A. Ruck-Keene,
Sensors and Actuators B, 47, 37, 1998
19Lyotropic Liquid Crystals
Lyotropic liquid crystals (such as surfactants)
can form a variety of liquid crystalline phases
in solvents. This ordering is due to
hydrophobic/hydrophilic competitions.
micelle
hexagonal columnar
lamellar
Concentration increase
20Lyotropic LC Sensors
Most biologic receptors possess both hydrophilic
and hydrophobic regions and thus readily
incorporate into biphilic lyotropic liquid
crystals. When the receptor-ligand complex
forms, the uniform order is disrupted producing
an optical response.
Fig. 10 schematic representation of the
amplification mechanism with the specific ligand
bound to its receptor causing deformation of the
liquid crystal and alternation of the
transmission of polarized light.
C.J. Woolverton, G.D. Niehaus, K.J. Doane, O.D.
Lavrentovich, S.P. Schmidt, S.A. Signs, US
Patent, US 6171802, 2001.
21Lyotropic LC Sensors
The elasticity of the liquid crystal amplifies
the local distortions in the vicinity of the
receptor-ligand complex, and rapidly expands it
to an optically detectable, supramicron
scale. Lyotropic LCs offer a system that
rapidly, reliably and automatically detects
ligands, especially when present in very small
quantities. It is further envisioned that a
multiwell system, each well having a
predetermined receptor, can be used to detect
different kind of ligands individually.
Fig. 5 A profound increase in transmission of
propagating light occurs when liquid crystals
amplify the binding of antibody to ligands.
C.J. Woolverton, G.D. Niehaus, K.J. Doane, O.D.
Lavrentovich, S.P. Schmidt, S.A. Signs, US
Patent, US 6171802, 2001.
22Comparison of 4 types of LC sensors
23Comparison of 4 types of LC sensors
24Conclusions
- 4 types of liquid crystal sensors and their
working mechanisms have been introduced. - Compared to the bulky and complex spectroscopy,
these LC sensors can not only provide real-time,
portable detection at reasonable sensitivity, but
also can be easily operated and manufactured.
25Selected References
- P. G. de Gennes, J. Prost, The Physics Of Liquid
Crystals, 2 ed., Oxford Science Publication,
Oxford, 1993. - http//www.barrettresearch.ca/teaching/liquid_crys
tal/ - V. K. Gupta, J. J. Skaife, T. B. Dubrovsky, N. L.
Abbot, Science, 279, 2077, 1998. - R. R. Shah, N.L. Abbott, Science, 293, 1296,
2001. - C.J. Woolverton, G.D. Niehaus, K.J. Doane, O.D.
Lavrentovich, S.P. Schmidt, S.A. Signs, US
Patent, US 6171802, 2001. - N. Abbott, R. Shah, World Patent, WO 02/075294
A1, 2002. - D. A. Winterbottom, R. Narayanaswamy, I. M.
Raimundo Jr., Sensors and Actuators B, 90, 52,
2003. - J. Clement, N. Boden, T. D. Gibson, R. C.
Chandler, J. N. Hulbert, E. A. Ruck-Keene,
Sensors and Actuators B, 47, 37, 1998. - F.L. Dickert, A. Haunschild, P. Hofmann, J. Anal.
Chem., 350, 577 (1994). - F.J. Poziomek, T.J. Novak, R.A. Mackay, Mol.
Cryst. Liq. Cryst., 27, 175, (1973).