Liquid Crystals
Transcript of Liquid Crystals
1
Liquid crystals• Anisotropic motion
• rotation• diffusion
• Effect on NMRmeasurables• CSA lineshapes• dipolar couplings• diffusion coefficients
Surfactants and liquid crystalsSelf-assembly in water solution
hexagonal lamellar, Lαcubicmicellarsolution
conc.surfactant
2
Motion in a lamellar phase• Rotation, translation, change of
conformation• Interactions ⊥n averaged
ndirector
4
6
DNA and phospholipid
deconvolution
Leal, Sandström, Nevsten, Topgaard, Biochim. Biophys. Acta (2008)
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Fast, anisotropic motionB0
rθ
S = 0S = 1/4
(3cos2θ-1)/2
θ / º
order parameter, S
!
"#d
=1
23cos
2$ %1 "#d,max
average
Δνdresidual dipolar coupling, RDC
Separated local field161514 12 4 25 31 13N 6-11
1615
14
12
10
8
6
4
2
9
7
5
3
1
13
11
Nν 1
(1H
-13C
) / k
Hz
SCH can be measured!
Lα, non-ionic surfactant
-1
12108642
97531 11
-2
-13 -11
-10 -8
-7 -5
-4-14
C12E5
Ferreira, Medronho, Martin, Topgaard, Phys. Chem. Chem. Phys. (2008)
ν 1(1
H-13
C) /
kHz
Effect of temperature
-1
12108642
97531 11
-2
-13 -11
-10 -8
-7 -5
-4-14
|SC
H |
T / K
δ - δ
298K
/ pp
m
Conformation• Lowest energy
• alkyl: straight• ethylene oxide:
gauche helix• Increase T:
• alkyl: more gauche• ethylene oxide:
more trans
SCH(T) maximum
Liquid ordered phaseliquid disordered liquid ordered
•Translational diffusionreduced factor 2-3•Flat SCH profile
• CP• dipolar couplings• efficient for solids
• INEPT• J-couplings• efficient for liquids
1H→13C polarization transfer
polarizationtransfer
Domain size mm-scale:isotropic
nm-scale:lamellae
µm-scale:anisotropicdomainsB0
n
θ
Influence on NMRmeasurables?CSA, RDC, D