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Anisotropic and isotropic electroconvection

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Anisotropic and isotropic electroconvection. Collaborators: L. ... planar, a 0, a 0 anisotropic. homeotropic, a 0, a 0 ... obliqueness! e1- e3= 1.34 ... – PowerPoint PPT presentation

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Title: Anisotropic and isotropic electroconvection


1
Anisotropic and isotropic electroconvection
Collaborators L.Kramer, W.Pesch (Univ.
Bayreuth/Germany and
N.Eber (Inst. Solid State Phys./Hungary)
H
I. (anis.)
III. (isotr.)
II. (interm.)
OR (low f)
y
x
NR (high f)


planar
homeotropic
homeotropic
2
ELECTROHYDRODYNAMICS OF NEMATICS
STANDARD
- free energy density - balance of torques -
equation of motion - incompressibility - equation
of electrostatics -charge conservation
MODEL



(SM)
3
Material parameters
Boundary conditions planar or homeotropic
Relevant alignment sign of ?a and ?a ? 8
combinations
  • planar, ?a lt 0, ?a gt 0
    anisotropic
  • homeotropic, ?a lt 0, ?a gt 0 intermediate
  • homeotropic, ?a gt 0, ?a lt 0 isotropic
  • IV. planar, ?a lt 0, ?a lt 0
    non-standard

SM
4
I. planar, ?a lt 0, ?a gt 0
anisotropic
Ginzburg-Landau description works
MBBA - 0.13
5
At threshold, increasing f (planar, ?a gt 0, ? a lt
0)
OR
NR
n
TW (non-stand.)
DR
6
II. homeotropic, ?a lt 0, ?a gt 0
7
H drives between semi-isotropic and anisotropic
  • soft lt-gt patterning mode
  • direct transition to STC
  • AR-s
  • chevron formation
  • defect glide
  • 2 LP-s

NR
OR
8
Homeotropic alignment (standard, semi-isotropic)
(A.Rossberg, L.Kramer)
OR
NR
theor.
exp.
9
III. Homeotropic, ?a gt 0, ?a lt 0 ( truly
isotropic)
Direct transition to isotropic EC
10
Direct transition to EC -gt SM
11
Swift-Hohenberg eq.
(W.Pesch, L.Kramer, B.Dressel)
At onset
exp.
theo.
f
nonlinear regime hard squares
soft squares

not reproduced
12
(No Transcript)
13
(No Transcript)
14
(No Transcript)
15
IV. planar, ?a lt 0, ?a lt 0 no standard
pattern (conductive)
16
  • PR or oblique
  • nz 0, no shadowgraph
  • ny (?) oscillates
  • Uc d, f
  • - qc is d indep.

Experimental
Dielectric mode! (LK)
17
I and II- conductive III and IV - dielectric
18
1. Dielectric mode for MBBA (planar, ?a lt 0, ?a
gt 0)
2. Dielectric mode for MBBA (planar, ?a lt 0, ?a
lt 0) - no pattern
Flexoelectricity
19
Flexoelectricity
Effect on the roll angle, only for d.c. (only in
conductive)
20
3. Dielectric mode for MBBA (planar, ?a lt 0, ?a
lt 0) flexoelectricity
e1- e3 1.34 e1 e3 -7.84
finite threshold!
obliqueness!
21
4. Dielectric mode for MBBA (planar, ?a lt 0, ?a
lt 0) flexoelectricity
e1- e3 2.68 e1 e3 -7.84
(A.Krekhov, W.Pesch)
22
planar, ?a lt 0, ?a lt 0 no standard pattern
(conductive)
  • dielectric mode at low f
  • SM flexoelectricity
  • why is DM more sensitive to flexo, than CM?
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