¿Ü±¹µµ¼
´ëÇб³Àç/Àü¹®¼Àû
ÀÚ¿¬°úÇÐ ÀϹÝ
2013³â 9¿ù 9ÀÏ ÀÌÈÄ ´©Àû¼öÄ¡ÀÔ´Ï´Ù.
Á¤°¡ |
59,000¿ø |
---|
59,000¿ø
1,770P (3%Àû¸³)
ÇÒÀÎÇýÅÃ | |
---|---|
Àû¸³ÇýÅà |
|
|
|
Ãß°¡ÇýÅÃ |
|
À̺¥Æ®/±âȹÀü
¿¬°üµµ¼
»óÇ°±Ç
ÀÌ»óÇ°ÀÇ ºÐ·ù
¸ñÂ÷
A bird's eye view of liquid crystal elastomers | p. 1 |
Liquid crystals | p. 9 |
Ordering of rod and disc fluids | p. 9 |
Nematic order | p. 11 |
Free energy and phase transitions of nematics | p. 15 |
Molecular theory of nematics | p. 20 |
Distortions of nematic order | p. 22 |
Transitions driven by external fields | p. 25 |
Anisotropic viscosity and dissipation | p. 29 |
Cholesteric liquid crystals | p. 33 |
Smectic liquid crystals | p. 38 |
Polymers, elastomers and rubber elasticity | p. 47 |
Configurations of polymers | p. 48 |
Liquid crystalline polymers | p. 52 |
Shape of liquid crystalline polymers | p. 54 |
Frank elasticity of nematic polymers | p. 61 |
Classical rubber elasticity | p. 62 |
Manipulating the elastic response of rubber | p. 67 |
Finite extensibility and entanglements in elastomers | p. 70 |
Classical elasticity | p. 75 |
Deformation tensor and Cauchy-Green strain | p. 75 |
Non-linear and linear elasticity | p. 78 |
Geometry of deformations and rotations | p. 83 |
Rotations | p. 83 |
Shears and their decomposition | p. 84 |
Square roots and polar decomposition of tensors | p. 90 |
Compressibility of rubbery networks | p. 91 |
Nematic elastomers | p. 95 |
Structure and examples of nematic elastomers | p. 96 |
Stress-optical coupling | p. 99 |
Polydomain textures and alignment by stress | p. 101 |
Monodomain 'single-crystal' nematic elastomers | p. 104 |
Spontaneous shape changes | p. 106 |
Nematic photoelastomers | p. 108 |
Field-induced director rotation | p. 111 |
Applications of liquid crystalline elastomers | p. 115 |
Nematic rubber elasticity | p. 120 |
Neo-classical theory | p. 120 |
Spontaneous distortions | p. 123 |
Equilibrium shape of nematic elastomers[Dagger] | p. 129 |
Photo-mechanical effects | p. 131 |
Thermal phase transitions | p. 136 |
Effect of strain on nematic order | p. 139 |
Mechanical and nematic instabilities | p. 145 |
Mechanical Freedericks transition | p. 146 |
The elastic low road | p. 148 |
Finite extensibility and entanglements | p. 150 |
Soft elasticity | p. 154 |
Director anchoring to the bulk | p. 155 |
Director rotation without strain | p. 155 |
Coupling of rotations to pure shear | p. 158 |
Soft elasticity | p. 159 |
Soft modes of deformation | p. 160 |
Principal symmetric strains and body rotations | p. 164 |
Forms of the free energy allowing softness | p. 166 |
Optimal deformations | p. 167 |
A practical method of calculating deformations | p. 167 |
Stretching perpendicular to the director | p. 169 |
Semi-soft elasticity | p. 173 |
Example: random copolymer networks | p. 174 |
A practical geometry of semi-soft deformation | p. 175 |
Experiments on long, semi-soft strips | p. 117 |
Unconstrained elastomers in external fields | p. 178 |
Semi-soft free energy and stress | p. 179 |
Thermomechanical history and general semi-softness | p. 183 |
Thermomechanical history dependence | p. 184 |
Forms of the free energy violating softness | p. 185 |
Distortions of nematic elastomers | p. 187 |
Freedericks transitions in nematic elastomers | p. 188 |
Strain-induced microstracture: stripe domains | p. 194 |
General distortions of nematic elastomers | p. 201 |
One-dimensional quasi-convexification | p. 202 |
Full quasi-convexification | p. 205 |
Numerical and experimental studies | p. 207 |
Random disorder in nematic networks | p. 210 |
Nematic ordering with quenched disorder | p. 212 |
Characteristic domain size | p. 213 |
Polydomain-monodomain transition | p. 216 |
Cholesteric elastomers | p. 220 |
Cholesteric networks | p. 221 |
Intrinsically chiral networks | p. 221 |
Chirally imprinted networks | p. 222 |
Mechanical deformations | p. 227 |
Uniaxial transverse elongation | p. 228 |
Stretching along the pitch axis | p. 233 |
Piezoelectricity of cholesteric elastomers | p. 236 |
Imprinted cholesteric elastomers | p. 242 |
Photonics of cholesteric elastomers | p. 245 |
Photonics of liquid cholesterics | p. 246 |
Photonics of elastomers | p. 249 |
Experimental observations | p. 251 |
Lasing in cholesterics | p. 253 |
Continuum description of nematic elastomers | p. 256 |
From molecular theory to continuum elasticity | p. 257 |
Compressibility effects | p. 257 |
The limit of linear elasticity | p. 258 |
The role of nematic anisotropy | p. 260 |
Phenomenological theory for small deformations | p. 262 |
Strain-induced rotation | p. 265 |
Soft elasticity | p. 268 |
Symmetry arguments | p. 269 |
The mechanism of soft deformation | p. 271 |
Continuum representation of semi-softness | p. 273 |
Unconstrained director fluctuations | p. 276 |
Unconstrained phonons | p. 279 |
Light scattering from director fluctuations | p. 282 |
Dynamics of liquid crystal elastomers | p. 288 |
Classical rubber dynamics | p. 289 |
Rouse model and entanglements | p. 291 |
Dynamical response of entangled networks | p. 293 |
Long time stress relaxation | p. 296 |
Nematohydrodynamics of elastic solids | p. 298 |
Viscous coefficients and relaxation times | p. 300 |
Balance of forces and torques | p. 301 |
Symmetries and order parameter | p. 303 |
Response to oscillating strains | p. 304 |
Experimental observations | p. 308 |
Oscillating shear | p. 309 |
Steady stress relaxation | p. 313 |
Smectic elastomers | p. 317 |
Materials and preparation | p. 317 |
Smectic A elastomers | p. 319 |
Smectic C and ferroelectric C elastomers | p. 321 |
Physical properties of smectic elastomers | p. 322 |
Smectic-A elastomers | p. 322 |
Smectic-C elastomers | p. 326 |
A molecular model of Smectic-A rubber elasticity | p. 328 |
The geometry of affine layer deformations | p. 330 |
Response to principal deformations | p. 331 |
General deformations of a SmA elastomer | p. 339 |
Instability and CMHH microstructure | p. 340 |
Comparison with experiment | p. 342 |
Smectic-C rubber elasticity | p. 344 |
SmC soft deformations | p. 345 |
SmC deformations with microstructure | p. 348 |
Continuum description of smectic elastomers | p. 350 |
Continuum description of smectic A elastomers | p. 350 |
Relative translations in smectic networks revisited | p. 351 |
Nematic -strain, -rotation and -smectic couplings | p. 353 |
Effective smectic elasticity of elastomers | p. 355 |
Effective rubber elasticity of smectic elastomers | p. 360 |
Layer elasticity and fluctuations in smectic A elastomers | p. 364 |
Layer buckling instabilities: the CMHH effect | p. 371 |
Quenched layer disorder and the N-A phase transition | p. 374 |
Smectic C and ferroelectric C elastomers | p. 378 |
References | p. 382 |
Index | p. 393 |
Author Index | p. 400 |
Online Appendices: (www.lcelastomer.org.uk) | |
Nematic order in elastomers under strain | |
Biaxial soft elasticity | |
Stripe microstructure | |
Couple-stress and Cosserat elasticity | |
Expansion at small deformations and rotations | |
Smectic C soft elasticity | |
Table of Contents provided by Ingram. All Rights Reserved. |
Ã¥¼Ò°³
Liquid crystals are fluids with a directionality defined. Polymers are long molecules with a shape that can be changed. As a network, polymers form rubber - a soft solid that is locally liquid-like and capable of huge extension. Liquid crystal elastomers are a combination of all these curiousaspects, but with additional, revolutionary new phenomena - for example, spontaneous shape changes of several hundred percent induced by temperature change, with equally large opto-mechanical responses, shape change without energy cost ("soft elasticity"), colour change with strain, lasing andphotonics, sensitivity to molecular handedness and soft solid ferroelectricity. This book is a primer for liquid crystals, polymers, rubber, and elasticity. It then describes the theory and experiment of these remarkable materials for the first time as a monograph. Worked examples are solved so thatthe reader can become proficient in the field himself. The book is directed at physicists, chemists, material scientists, engineers and applied mathematicians at the graduate student level and beyond
ÀúÀÚ¼Ò°³
»ý³â¿ùÀÏ | - |
---|
ÇØ´çÀÛ°¡¿¡ ´ëÇÑ ¼Ò°³°¡ ¾ø½À´Ï´Ù.
ÁÖ°£·©Å·
´õº¸±â»óÇ°Á¤º¸Á¦°ø°í½Ã
À̺¥Æ® ±âȹÀü
´ëÇб³Àç/Àü¹®¼Àû ºÐ¾ß¿¡¼ ¸¹Àº ȸ¿øÀÌ ±¸¸ÅÇÑ Ã¥
ÆǸÅÀÚÁ¤º¸
»óÈ£ |
(ÁÖ)±³º¸¹®°í |
---|---|
´ëÇ¥ÀÚ¸í |
¾Èº´Çö |
»ç¾÷ÀÚµî·Ï¹øÈ£ |
102-81-11670 |
¿¬¶ôó |
1544-1900 |
ÀüÀÚ¿ìÆíÁÖ¼Ò |
callcenter@kyobobook.co.kr |
Åë½ÅÆǸž÷½Å°í¹øÈ£ |
01-0653 |
¿µ¾÷¼ÒÀçÁö |
¼¿ïƯº°½Ã Á¾·Î±¸ Á¾·Î 1(Á¾·Î1°¡,±³º¸ºôµù) |
±³È¯/ȯºÒ
¹ÝÇ°/±³È¯ ¹æ¹ý |
¡®¸¶ÀÌÆäÀÌÁö > Ãë¼Ò/¹ÝÇ°/±³È¯/ȯºÒ¡¯ ¿¡¼ ½Åû ¶Ç´Â 1:1 ¹®ÀÇ °Ô½ÃÆÇ ¹× °í°´¼¾ÅÍ(1577-2555)¿¡¼ ½Åû °¡´É |
---|---|
¹ÝÇ°/±³È¯°¡´É ±â°£ |
º¯½É ¹ÝÇ°ÀÇ °æ¿ì Ãâ°í¿Ï·á ÈÄ 6ÀÏ(¿µ¾÷ÀÏ ±âÁØ) À̳»±îÁö¸¸ °¡´É |
¹ÝÇ°/±³È¯ ºñ¿ë |
º¯½É ȤÀº ±¸¸ÅÂø¿À·Î ÀÎÇÑ ¹ÝÇ°/±³È¯Àº ¹Ý¼Û·á °í°´ ºÎ´ã |
¹ÝÇ°/±³È¯ ºÒ°¡ »çÀ¯ |
·¼ÒºñÀÚÀÇ Ã¥ÀÓ ÀÖ´Â »çÀ¯·Î »óÇ° µîÀÌ ¼Õ½Ç ¶Ç´Â ÈÑ¼ÕµÈ °æ¿ì ·¼ÒºñÀÚÀÇ »ç¿ë, Æ÷Àå °³ºÀ¿¡ ÀÇÇØ »óÇ° µîÀÇ °¡Ä¡°¡ ÇöÀúÈ÷ °¨¼ÒÇÑ °æ¿ì ·º¹Á¦°¡ °¡´ÉÇÑ »óÇ° µîÀÇ Æ÷ÀåÀ» ÈѼÕÇÑ °æ¿ì ·½Ã°£ÀÇ °æ°ú¿¡ ÀÇÇØ ÀçÆǸŰ¡ °ï¶õÇÑ Á¤µµ·Î °¡Ä¡°¡ ÇöÀúÈ÷ °¨¼ÒÇÑ °æ¿ì ·ÀüÀÚ»ó°Å·¡ µî¿¡¼ÀÇ ¼ÒºñÀÚº¸È£¿¡ °üÇÑ ¹ý·üÀÌ Á¤ÇÏ´Â ¼ÒºñÀÚ Ã»¾àöȸ Á¦ÇÑ ³»¿ë¿¡ ÇØ´çµÇ´Â °æ¿ì |
»óÇ° Ç°Àý |
°ø±Þ»ç(ÃâÆÇ»ç) Àç°í »çÁ¤¿¡ ÀÇÇØ Ç°Àý/Áö¿¬µÉ ¼ö ÀÖÀ½ |
¼ÒºñÀÚ ÇÇÇغ¸»ó |
·»óÇ°ÀÇ ºÒ·®¿¡ ÀÇÇÑ ±³È¯, A/S, ȯºÒ, Ç°Áúº¸Áõ ¹× ÇÇÇغ¸»ó µî¿¡ °üÇÑ »çÇ×Àº¼ÒºñÀÚºÐÀïÇØ°á ±âÁØ (°øÁ¤°Å·¡À§¿øȸ °í½Ã)¿¡ ÁØÇÏ¿© ó¸®µÊ ·´ë±Ý ȯºÒ ¹× ȯºÒÁö¿¬¿¡ µû¸¥ ¹è»ó±Ý Áö±Þ Á¶°Ç, ÀýÂ÷ µîÀº ÀüÀÚ»ó°Å·¡ µî¿¡¼ÀǼҺñÀÚ º¸È£¿¡ °üÇÑ ¹ý·ü¿¡ µû¶ó ó¸®ÇÔ |
(ÁÖ)ÀÎÅÍÆÄÅ©Ä¿¸Ó½º´Â ȸ¿ø´ÔµéÀÇ ¾ÈÀü°Å·¡¸¦ À§ÇØ ±¸¸Å±Ý¾×, °áÁ¦¼ö´Ü¿¡ »ó°ü¾øÀÌ (ÁÖ)ÀÎÅÍÆÄÅ©Ä¿¸Ó½º¸¦ ÅëÇÑ ¸ðµç °Å·¡¿¡ ´ëÇÏ¿©
(ÁÖ)KGÀ̴Ͻýº°¡ Á¦°øÇÏ´Â ±¸¸Å¾ÈÀü¼ºñ½º¸¦ Àû¿ëÇÏ°í ÀÖ½À´Ï´Ù.
¹è¼Û¾È³»
±³º¸¹®°í »óÇ°Àº Åùè·Î ¹è¼ÛµÇ¸ç, Ãâ°í¿Ï·á 1~2Àϳ» »óÇ°À» ¹Þ¾Æ º¸½Ç ¼ö ÀÖ½À´Ï´Ù.
Ãâ°í°¡´É ½Ã°£ÀÌ ¼·Î ´Ù¸¥ »óÇ°À» ÇÔ²² ÁÖ¹®ÇÒ °æ¿ì Ãâ°í°¡´É ½Ã°£ÀÌ °¡Àå ±ä »óÇ°À» ±âÁØÀ¸·Î ¹è¼ÛµË´Ï´Ù.
±ººÎ´ë, ±³µµ¼Ò µî ƯÁ¤±â°üÀº ¿ìü±¹ Åù踸 ¹è¼Û°¡´ÉÇÕ´Ï´Ù.
¹è¼Ûºñ´Â ¾÷ü ¹è¼Ûºñ Á¤Ã¥¿¡ µû¸¨´Ï´Ù.