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Anisotropic deformation of monodomain LCEs by a thermal phase transition from an LC to an isotropic state was rst reported by Kupfer and Finkelmann (1994) A nematic LCE prepared by the two-step process contracted by about 26% owing to the change in order parameter as a result of the change in molecular alignment of mesogens This anisotropic deformation behavior of LCEs has been a subject of extensive experimental and theoretical studies (Stenull and Lubensky, 2005; Mao et al, 2001; Warner et al, 1988) Warner and Terentjev established a relation between the nematic order parameter S and the effective backbone anisotropy of polymer chains forming the rubbery network The relation is expressed by a dimensionless ratio of the principal step lengths parallel and perpendicular to the nematic director (R8/R>) (Warner and Terentjev, 2003, 1996) In the nematic phase, this ratio is larger than unity (R8/R>E1.



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To decrypt the received ciphertext message, c, Bob computes m = cd mod n which requires the use of his secret key, (n,d)

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3) (Warner and Terentjev, 1996), but after a nematic isotropic phase transition, this ratio approaches unity as a result of the formation of a random coil of polymer chains, which makes the polymer material contract along the director axis of LCEs In the smectic A phase, the ratio R8/R> is in general smaller than unity because the polymer chains are likely to exist between the smectic layers (Cotton and Hardouin, 1997) There have been a number of efforts to develop arti cial musclelike materials (Buguin et al, 2006; Mol et al, 2005; Saikrasun et al, 2005; Stenull and Lubensky, 2005; Li et al, 2004; Naciri et al, 2003; Clarke et al, 2001; Mao et al, 2001; Thomsen et al, 2001) LCE lms with a splayed or twisted molecular alignment display a well-controlled deformation as a function of temperature (Fig 3.

As a simple example of RSA, suppose Bob chooses p=5 and q=7 (admittedly, these values are far too small to be secure) Then n=35 and z=24 Bob chooses e=5, since 5 and 24 have no common factors Finally, Bob

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12) (Mol et al, 2005) The twisted lms show a complex macroscopic deformation owing to the formation of saddlelike geometries, whereas the deformation of the splayed structure is smooth and well controlled (Mol et al, 2005) Wermter and Finkelmann (2001) reported a new type of LC coelastomers composed of LC side chains and LC main-chain polymers (Components 10a c) as network strands Thanks to the direct coupling of the LC main-chain segments to the network anisotropy, the thermoelastic response was increased remarkably with an increase of the concentration of these segments An elongation in the direction of the director by up to a factor of 4, relative to the length of the networks in an isotropic state, was observed in the nematic state (Fig 313) (Wermter and Finkelmann, 2001).

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chooses d=29, since 5*29 - 1 (ie, ed -1 ) is exactly divisible by 24 Bob makes the two values, n=35 and e=5, public and keeps the value d=29 secret Observing these two public values, suppose Alice now wants to send the letters 'l' 'o' 'v' and 'e' to Bob Interpreting each letter as a number between 1 and 26 (with 'a' being 1, and 'z' being 26), Alice and Bob perform the encryption and decryption shown in Figures 72-6 and 72-7, respectively:

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