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Schematic of the circular dielectric liquid crystal elastomer sheet sandwiched between two compliant electrodes and the nematic director d at a material point (r,β,z) in the cylindrical coordinate system
Published Online: April 17, 2025
Fig. 1 Schematic of the circular dielectric liquid crystal elastomer sheet sandwiched between two compliant electrodes and the nematic director d at a material point ( r , β , z ) in the cylindrical coordinate system More about this image found in Schematic of the circular dielectric liquid crystal elastomer sheet sandwic...
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Cone-like bending shapes and corresponding spontaneous shear strain distributions γrzs(r). γrzs(r) maintains a consistent sign: (a) the standard cone corresponds to the constant γrzs(r), (b) the convex cone corresponds to the monotonically increasing |γrzs(r)|, and (c) the concave cone corresponds to the monotonically decreasing |γrzs(r)|. E~V is a dimensionless parameter given by Eq. (32).
Published Online: April 17, 2025
Fig. 2 Cone-like bending shapes and corresponding spontaneous shear strain distributions γ r z s ( r ) . γ r z s ( r ) maintains a consistent sign: ( a ) the standard cone corresponds to the constant γ r z s ( r ) , ( b ) the convex cone correspo... More about this image found in Cone-like bending shapes and corresponding spontaneous shear strain distrib...
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Convex–concave coexisting cone bending shapes and corresponding spontaneous shear strain distributions γrzs(r). γrzs(r) maintains a consistent sign and the value of |γrzs(r)| is non-monotonic. The convex part corresponds to the interval where |γrzs(r)| is monotonically increasing, while the concave part corresponds to the interval where |γrzs(r)| is monotonically decreasing.
Published Online: April 17, 2025
Fig. 3 Convex–concave coexisting cone bending shapes and corresponding spontaneous shear strain distributions γ r z s ( r ) . γ r z s ( r ) maintains a consistent sign and the value of | γ r z s ( r ) | is non-monotonic. The convex part corres... More about this image found in Convex–concave coexisting cone bending shapes and corresponding spontaneous...
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Phase diagram of the bending shapes with constant radial principal curvatures κrr. The standard cone corresponds to the γ0s-axis where K=0. The convex cone corresponds to the first and third quadrants where γ0s/K≥0. The concave cone corresponds to the regions in the second and fourth quadrants near the vertical axis where γ0s/K≤−1. The concave cone with a trough corresponds to the regions in the second and fourth quadrants far from the vertical axis where −1<γ0s/K<0. Under a specific |E~V| given by Eq. (32), the values of K and γ0s are limited to the interior of the parallelogram.
Published Online: April 17, 2025
Fig. 4 Phase diagram of the bending shapes with constant radial principal curvatures κ r r . The standard cone corresponds to the γ 0 s -axis where K = 0 . The convex cone corresponds to the first and third quadrants where γ 0 s / K ≥ 0 . The concave con... More about this image found in Phase diagram of the bending shapes with constant radial principal curvatur...
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Phase diagram of the bending shapes with linearly varying radial principal curvatures κrr. The standard cone corresponds to the γ0s-axis where K0=0. The convex–concave coexisting cone (with its side edges bulging outward near the apex and curving inward near the base) corresponds to the first and third quadrants where γ0s/K0≥0. The convex–concave coexisting cone (with its side edges curves inward near the apex and bulges outward near the base) corresponds to the regions in the second and fourth quadrants near the vertical axis where γ0s/K0≤−1/4. The cone with one peak and one trough corresponds to the regions where −1/4<γ0s/K0<0. Under a specific |E~V| given by Eq. (32), the values of K0 and γ0s are limited to the interior of the parallelogram.
Published Online: April 17, 2025
Fig. 5 Phase diagram of the bending shapes with linearly varying radial principal curvatures κ r r . The standard cone corresponds to the γ 0 s -axis where K 0 = 0 . The convex–concave coexisting cone (with its side edges bulging outward near the apex and curving in... More about this image found in Phase diagram of the bending shapes with linearly varying radial principal ...
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Wave-like bending shapes: (a)–(c) the extremum points of the deflection w are located where the spontaneous shear strain γrzs is zero; and (d) bending shapes with multiple peaks and troughs
Published Online: April 17, 2025
Fig. 6 Wave-like bending shapes: ( a )–( c ) the extremum points of the deflection w are located where the spontaneous shear strain γ r z s is zero; and ( d ) bending shapes with multiple peaks and troughs More about this image found in Wave-like bending shapes: ( a )–( c ) the extremum points of the deflection...
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Optimal nematic director orientation alignments for (a) programming the standard cone bending shape as tall as possible, and (b) programming the convex cone, (c) concave cone, and (d) concave cone with a trough bending shapes possessing the maximum possible radial principal curvature value, under a given applied voltage
Published Online: April 17, 2025
Fig. 9 Optimal nematic director orientation alignments for ( a ) programming the standard cone bending shape as tall as possible, and ( b ) programming the convex cone, ( c ) concave cone, and ( d ) concave cone with a trough bending shapes possessing the maximum possible radial principal curvatur... More about this image found in Optimal nematic director orientation alignments for ( a ) programming the s...
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Optimal nematic director orientation alignments for programming the convex–concave coexisting cone bending shapes possessing the maximum possible radial principal curvature gradient
Published Online: April 17, 2025
Fig. 10 Optimal nematic director orientation alignments for programming the convex–concave coexisting cone bending shapes possessing the maximum possible radial principal curvature gradient More about this image found in Optimal nematic director orientation alignments for programming the convex–...
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(a) Optimal nematic director orientation alignments for programming the wave-like bending shape with n (=4) peaks and n (=4) troughs possessing the maximum possible bending amplitude. The parameter pγ is set to zero; (b) optimal nematic director orientation alignments for programming the piecewise bending shape with side edges featuring most different dual inclinations. The parameter rj is set to R/2.
Published Online: April 17, 2025
Fig. 11 ( a ) Optimal nematic director orientation alignments for programming the wave-like bending shape with n (=4) peaks and n (=4) troughs possessing the maximum possible bending amplitude. The parameter p γ is set to zero; ( b ) optimal nematic director orientation alignments for... More about this image found in ( a ) Optimal nematic director orientation alignments for programming the w...
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A plane longitudinal wave traveling in an elastic medium is scattered by a modulated medium where both real and imaginary parts of material parameters vary periodically in space and time
Published Online: April 17, 2025
Fig. 1 A plane longitudinal wave traveling in an elastic medium is scattered by a modulated medium where both real and imaginary parts of material parameters vary periodically in space and time More about this image found in A plane longitudinal wave traveling in an elastic medium is scattered by a ...
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Band dispersion and wave scattering properties of stiffness-modulated media: (a) and (b) α1=0.4, β1=0, and cm=0; (c) and (d) α1=0.4, β1=0, and cm=0.1c0; (e) and (f) α1=0.4, β1=0.4, and cm=0.1c0; (g) and (h) α1=0.4, β1=−0.4, and cm=0.1c0, where scattering results of different order modes are given for the case of the 0th-order wave incidence
Published Online: April 17, 2025
Fig. 2 Band dispersion and wave scattering properties of stiffness-modulated media: ( a ) and ( b ) α 1 = 0.4 , β 1 = 0 , and c m = 0 ; ( c ) and ( d ) α 1 = 0.4 , β 1 = 0 , and c m = 0.1 c 0 ; ( e ) and ( f ) α 1 = 0.4... More about this image found in Band dispersion and wave scattering properties of stiffness-modulated media...
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Reflection coefficients of the ±1st-order wave modes for stiffness-modulated media with different modulating amplitudes: α1=β1= 0.1 (a), 0.24 (b), and 0.4 (c)
Published Online: April 17, 2025
Fig. 3 Reflection coefficients of the ± 1 st-order wave modes for stiffness-modulated media with different modulating amplitudes: α 1 = β 1 = 0.1 ( a ), 0.24 ( b ), and 0.4 ( c ) More about this image found in Reflection coefficients of the ± 1 st-order wave modes for stiffness-...