Peculiar molecular dynamics behaviours in isotropic phase of some liquid crystalline systems

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    Peculiar molecular dynamicsbehaviours in isotropic phase of

    some liquid crystalline systems

    D. Filip, C. Cruz, P.J. Sebastio, A.C. Ribeiro

    T. Meyer, G.H. Mehl

    C.F.M.C. U. Lisboa

    University of Hull

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    Outline

    The systems:- low molecular weight LC organosiloxane compound

    - organosiloxane LC tetrapodes with laterally attached mesogenic groups

    - organosiloxane tetrapode with terminally attached mesogenic groups

    Purpose :

    - comparison between the peculiar molecular dynamics behaviour of the studied

    systems in isotropic phase with those of normal calamitics and other LC

    systems

    - study of the influence of the molecular characteristics on molecular

    dynamics in isotropic phase by proton NMR relaxation

    Discussion of the NMR relaxation results

    Conclusions

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    Outline

    The systems:- low molecular weight LC organosiloxane compound

    - organosiloxane LC tetrapodes with laterally attached mesogenic groups

    - organosiloxane tetrapode with terminally attached mesogenic groups

    Purpose :

    - comparison between the peculiar molecular dynamics behaviour of the studied

    systems in isotropic phase with those of normal calamitics and other LC

    systems

    - study of the influence of the molecular characteristics on molecular

    dynamics in isotropic phase by proton NMR relaxation

    Discussion of the NMR relaxation results

    Conclusions

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    Outline

    The systems:- low molecular weight LC organosiloxane compound

    - organosiloxane LC tetrapodes with laterally attached mesogenic groups

    - organosiloxane tetrapode with terminally attached mesogenic groups

    Purpose :

    - comparison between the peculiar molecular dynamics behaviour of the studied

    systems in isotropic phase with those of normal calamitics and other LC

    systems

    - study of the influence of the molecular characteristics on molecular

    dynamics in isotropic phase by proton NMR relaxation

    Discussion of the NMR relaxation results

    Conclusions

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    Outline

    The systems:- low molecular weight LC organosiloxane compound

    - organosiloxane LC tetrapodes with laterally attached mesogenic groups

    - organosiloxane tetrapode with terminally attached mesogenic groups

    Purpose :

    - comparison between the peculiar molecular dynamics behaviour of the studied

    systems in isotropic phase with those of normal calamitics and other LC

    systems

    - study of the influence of the molecular characteristics on molecular

    dynamics in isotropic phase by proton NMR relaxation

    Discussion of the NMR relaxation results

    Conclusions

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    Outline

    The systems:

    - low molecular weight LC organosiloxane compound

    - organosiloxane LC tetrapodes with laterally attached mesogenic groups

    - organosiloxane tetrapode with terminally attached mesogenic groups

    Purpose :

    - comparison between the peculiar molecular dynamics behaviour of the studied

    systems in isotropic phase with those of normal calamitics and other LC

    systems

    - study of the influence of the molecular characteristics on molecular

    dynamics in isotropic phase by proton NMR relaxation

    Discussion of the NMR relaxation results

    Conclusions

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    monomer : normal behaviour

    as usually revealed by LCs in

    isotropic phase

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    typical contribution of CM in

    nematic phase with the typical

    square root frequency dependence

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    Proton Spin Relaxation Study of Molecular

    Motions in the Lyotropic Liquid CrystallineSystem Potassium-Laurate Water,

    W.Khner, E. Rommel, F. Noack and P. Meier,

    Z. Naturforsch. 42 a, 127 (1987).

    Lyotropic LC Systems

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    Packing model in N phase Packing model in SmC phase

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    tetrapode : peculiar frequencydispersion in isotropic phase

    - square root law

    - no molecular self-diffusion

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    nematic phase :

    - square root law

    - no molecular self-diffusion

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    smectic C phase :

    - square root law

    - no molecular self-diffusion

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    tetrapode : peculiar frequency

    dispersion in isotropic phase

    - square root law

    - no molecular self-diffusion

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    nematic phase :

    - square root law

    - no molecular self-diffusion

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    Potassium laurate/6.24 % 1-decanol/68.6 % D2O

    Lyotropic LC Sytems

    318 K (Isotropic)

    303 K (Nematic calamitic)

    291 K (Nematic discotic)

    A New Formalism for the Evaluation of Order-Fluctuation Modes in Liquid Crystals from

    Field- Cycling NMR-Relaxometry Data,

    F. Grinberg, R.Kimmich, R.-O. Seitter

    and D. Pusiol, J. Magn. Reson. 135, 54 (1998)

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    tetrapode : normal behaviour

    as usually revealed by LCs inisotropic phase

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    higher contribution of CM when

    comparing with other studied LCs

    which, on the contrary showedthe dominance of SD

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    Model parameters obtained from the f its in nematic and isotropic phases of Ms

    Phase (ToC) I(130) N(100) N(90)

    Dx108(s) 0.3 - -

    Dx108(s) - 0.99 1.63

    ESD

    = 49 kJ mol-1

    Rx1010(s) 2.94 5.68 7.57

    EROT= 29 kJ mol-1

    ANx10-3(s-3/2) - 1.24 2.30

    Model parameters obtained fr om the fi ts in isotropic, nematic and smectic Cphases of Ts

    T, oC 138 134 112 104 98 78 74 70

    Phase I I N N N SmC SmC SmC

    Cmaxx10-8(Hz) 2.08 1.94 0.4 0.39 0.32 0.09 0.09 0.09

    Rx1010(s) 2.55 2.74 4.75 6.1 7.08 16.2 19.8 22.5

    EROT= 39 kJ mol-1max10

    8(s) 1.02 1.99 - - - - - -

    amax10-8( ) 1.79 0.81 - - - - - -

    ASRx10-4(s-3/2) 0.77 1.09 3.20 3.23 3.89 5.23 5.43 5.2

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    Model parameters obtained from the fi ts in isotropic and nematic

    phases of Tas

    Phase(ToC) I (60) I(52) I(49) N(35) N(32) N(27)

    Cmaxx10-6(Hz) 7.3 5.8 6.5 5.6 5.22 5.02Rx10

    9(s) 3.77 4.47 4.7 5.9 6.4 7.6

    EROT= 16 kJmol-1

    ASRx10-4(s-3/2) 6.75 7.97 8.79 13.78 14.18 17.42

    Model fi tting parameters obtained from the fi ts in isotropic, smectic A and

    smectic C phases of T-CN

    Phase(ToC) I(95) I(90) SmA(70) SmA (60) SmC(43)

    Cminx10-4(Hz) - - 8.69 7.06 7.06

    ASx10-7(s-2) - - 2.00 2.51 3.86

    Dx109(s) - - 6.47 8.16 9.98Dx10

    9(s) 6.35 7.9 - - -

    Rx1010(s) 2.92 3.77 4.84 5.98 9.0

    ESD= 7 kJ mol-1

    EROT= 19 kJ mol-1

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    Model parameters obtained from the fi ts in isotropic and nematic

    phases of Tas

    Phase(ToC) I (60) I(52) I(49) N(35) N(32) N(27)

    Cmaxx10-6(Hz) 7.3 5.8 6.5 5.6 5.22 5.02Rx10

    9(s) 3.77 4.47 4.7 5.9 6.4 7.6

    EROT= 16 kJmol-1

    ASRx10-4(s-3/2) 6.75 7.97 8.79 13.78 14.18 17.42

    Model fi tting parameters obtained from the fi ts in isotropic, smectic A and

    smectic C phases of T-CN

    Phase(ToC) I(95) I(90) SmA(70) SmA (60) SmC(43)

    Cminx10-4(Hz) - - 8.69 7.06 7.06

    ASx10-7(s-2) - - 2.00 2.51 3.86

    Dx109(s) - - 6.47 8.16 9.98Dx10

    9(s) 6.35 7.9 - - -

    Rx1010(s) 2.92 3.77 4.84 5.98 9.0

    ESD= 7 kJ mol-1

    EROT= 19 kJ mol-1

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    Isotropic Polymeric Systems

    ex. melts and solutions of poly(dimethyl

    siloxane)

    Anomalous Segment Diffusion in Polymersand NMR Relaxation Spectroscopy,

    H. W. Weber and R. Kimmich, Macromolecules,

    26, 2597 (1993).

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    Conclusions :

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    1. Low molecular weight organosiloxane compound

    3. Organosiloxane tetrapodes with shorter flexible spacers and laterally attached mesogens

    isotropic phase : - frequency dispersion

    - similar behaviour as in LC phase

    - molecular self-diffusion very much restricted possible due the

    arm interdigitation characteristic for low generation dendrimers

    - same square root frequency dependence law, like in nematic phase :

    these slow movements possible to be explained by the existence ofaggregates formed of interdigitated molecules

    2. Organosiloxane tetrapodewith long flexible spacersand terminally attached mesogens

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    4. The same type of peculiar behaviours were found also for some lyotropic LCs.

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    Conclusions :

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    1. Low molecular weight organosiloxane compound

    3. Organosiloxane tetrapodes with shorter flexible spacers and laterally attached mesogens

    isotropic phase : - frequency dispersion

    - similar behaviour as in LC phase

    - molecular self-diffusion very much restricted possible due the

    arm interdigitation characteristic for low generation dendrimers

    - same square root frequency dependence law, like in nematic phase :

    these slow movements possible to be explained by the existence ofaggregates formed of interdigitated molecules

    2. Organosiloxane tetrapodewith long flexible spacersand terminally attached mesogens

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    4. The same type of peculiar behaviours were found also for some lyotropic LCs.

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    Conclusions :

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    1. Low molecular weight organosiloxane compound

    3. Organosiloxane tetrapodes with shorter flexible spacers and laterally attached mesogens

    isotropic phase : - frequency dispersion

    - similar behaviour as in LC phase

    - molecular self-diffusion very much restricted possible due the

    arm interdigitation characteristic for low generation dendrimers

    - same square root frequency dependence law, like in nematic phase :

    these slow movements possible to be explained by the existence ofaggregates formed of interdigitated molecules

    2. Organosiloxane tetrapodewith long flexible spacersand terminally attached mesogens

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    4. The same type of peculiar behaviours were found also for some lyotropic LCs.

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    Conclusions :

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    1. Low molecular weight organosiloxane compound

    3. Organosiloxane tetrapodes with shorter flexible spacers and laterally attached mesogens

    isotropic phase : - frequency dispersion

    - similar behaviour as in LC phase

    - molecular self-diffusion very much restricted possible due the

    arm interdigitation characteristic for low generation dendrimers

    - same square root frequency dependence law, like in nematic phase :

    these slow movements possible to be explained by the existence ofaggregates formed of interdigitated molecules

    2. Organosiloxane tetrapode with long flexible spacers and terminally attached mesogens

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    4. The same type of peculiar behaviours were found also for some lyotropic LCs.

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    Conclusions :

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    1. Low molecular weight organosiloxane compound

    3. Organosiloxane tetrapodes with shorter flexible spacers and laterally attached mesogens

    isotropic phase : - frequency dispersion

    - similar behaviour as in LC phase

    - molecular self-diffusion very much restricted possible due the

    arm interdigitation characteristic for low generation dendrimers

    - same square root frequency dependence law, like in nematic phase :

    these slow movements possible to be explained by the existence ofaggregates formed of interdigitated molecules

    2. Organosiloxane tetrapode with long flexible spacers and terminally attached mesogens

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    4. The same type of peculiar behaviours were found also for some lyotropic LCs.

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    Conclusions :

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    1. Low molecular weight organosiloxane compound

    3. Organosiloxane tetrapodes with shorter flexible spacers and laterally attached mesogens

    isotropic phase : - frequency dispersion

    - similar behaviour as in LC phase

    - molecular self-diffusion very much restricted possible due the

    arm interdigitation characteristic for low generation dendrimers

    - same square root frequency dependence law, like in nematic phase :

    these slow movements possible to be explained by the existence ofaggregates formed of interdigitated molecules

    2. Organosiloxane tetrapodewith long flexible spacersand terminally attached mesogens

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    4. The same type of peculiar behaviours were found also for some lyotropic LCs.

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    Conclusions :

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    1. Low molecular weight organosiloxane compound

    3. Organosiloxane tetrapodes with shorter flexible spacers and laterally attached mesogens

    isotropic phase : - frequency dispersion

    - similar behaviour as in LC phase

    - molecular self-diffusion very much restricted possible due the

    arm interdigitation characteristic for low generation dendrimers

    - same square root frequency dependence law, like in nematic phase :

    these slow movements possible to be explained by the existence ofaggregates formed of interdigitated molecules

    2. Organosiloxane tetrapodewith long flexible spacersand terminally attached mesogens

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    4. The same type of peculiar behaviours were found also for some lyotropic LCs.

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    Conclusions :

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    1. Low molecular weight organosiloxane compound

    3. Organosiloxane tetrapodes with shorter flexible spacers and laterally attached mesogens

    isotropic phase : - frequency dispersion

    - similar behaviour as in LC phase

    - molecular self-diffusion very much restricted possible due the

    arm interdigitation characteristic for low generation dendrimers

    - same square root frequency dependence law, like in nematic phase :

    these slow movements possible to be explained by the existence ofaggregates formed of interdigitated molecules

    2. Organosiloxane tetrapodewith long flexible spacersand terminally attached mesogens

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    4. The same type of peculiar behaviours were found also for some lyotropic LCs.

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    Conclusions :

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    1. Low molecular weight organosiloxane compound

    3. Organosiloxane tetrapodes with shorter flexible spacers and laterally attached mesogens

    isotropic phase : - frequency dispersion

    - similar behaviour as in LC phase

    - molecular self-diffusion very much restricted possible due the

    arm interdigitation characteristic for low generation dendrimers

    - same square root frequency dependence law, like in nematic phase :

    these slow movements possible to be explained by the existence ofaggregates formed of interdigitated molecules

    2. Organosiloxane tetrapodewith long flexible spacersand terminally attached mesogens

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    4. The same type of peculiar behaviours were found also for some lyotropic LCs.

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    Conclusions :

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    1. Low molecular weight organosiloxane compound

    3. Organosiloxane tetrapodes with shorter flexible spacers and laterally attached mesogens

    isotropic phase : - frequency dispersion

    - similar behaviour as in LC phase

    - molecular self-diffusion very much restricted possible due the

    arm interdigitation characteristic for low generation dendrimers

    - same square root frequency dependence law, like in nematic phase :

    these slow movements possible to be explained by the existence ofaggregates formed of interdigitated molecules

    2. Organosiloxane tetrapodewith long flexible spacersand terminally attached mesogens

    isotropic phase : - typical relaxation mechanisms (SD, ROT)

    - no frequency dispersion

    4. The same type of peculiar behaviours were found also for some lyotropic LCs.

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    Acknowledgements

    The authors acknowledge the financial support of EU network onSuper Molecular Liquid Crystal Dendrimers (RTN-LCDD)HPRN-

    CT-2000-00016 and also for a fellowship, thank P. Kouwer for X-ray

    measurements on aligned samples and most helpful discussions, thank

    Dr. G. Feio for the experimental help with the Bruker MSL

    spectrometer, thank to D. Sousa and J. Cascais for fast field cyclingNMR technical developments and support, thank to C. Costa for

    preparation of the samples and X-ray diffraction facilities technical

    support.