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fem simulations  (Abaqus Inc)

 
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    Abaqus Inc fem simulations
    Fem Simulations, supplied by Abaqus Inc, used in various techniques. Bioz Stars score: 86/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
    https://www.bioz.com/product/fem+simulation/fem+simulations/pm42243096-240-0-5
    Average 86 stars, based on 1 article reviews
    fem simulations - by Bioz Stars, 2026-11
    86/100 stars

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    Software:

    Article Title: Semiempirical, Analytical, and Computational Predictions of Dynamic Modulus of Asphalt Concrete Mixtures
    Article Snippet: empirical pavement design protocols to compute the mechanical responses of pavement structures.. One of these pavement design protocols, the Guide for Mechanistic–Empirical Design of New and Rehabilitated Pavement Structures (the Mechanistic–Empirical Pavement Design Guide, or MEPDG) was developed in 2004 by AASHTO.. The material properties used to relate stresses and strains in the MEPDG software are Poisson’s ratio (generally assumed to be a constant value) and elastic modulus obtained from dynamic modulus master curves at a given temperature and loading frequency.

    Article Title: Self‐Oscillating Helix Showing Amplified Winding and Unwinding Motions
    Article Snippet: .. We performed the FEM simulation using commercial software ABAQUS/Standard (see for details). ..

    Article Title: Tuneable multidirectional mechanical attributes of novel sectionally nonlinearly functionally graded femur and cranial bone implants with triply periodic minimal surfaces
    Article Snippet: .. The stress and strain components in the equation are obtained from a three-dimensional FEM simulation performed by the commercial software Abaqus that employs the tetrahedral elements to mesh the structures. ..

    Adhesive:

    Article Title: Experimental testing and finite element analysis of polyurethane adhesive joints under Mode I loading and degradation conditions
    Article Snippet: .. The experimental results obtained from the tests allowed the development of an FEM simulation of the polyurethane adhesive joint using the Abaqus programme. ..

    other:

    Article Title: Rattern reduzieren durch NC- und FE-Simulation/Reducing chatter vibrations using NC and FE simulation - Vibrations in aerospace industry
    Article Snippet: FEM-Simulation in Abaqus: Die ersten sechs Eigenmoden; Deformation in Farbe und verstärkt dargestellt.



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    Thermally, chemically, and NIR‐responsive shrinking behaviors of poly(NIPAAm) helix. a) Scheme of the motion of a Vorticella ’s stalk in response to external threats (physical or chemical stimuli) from predators. b) Optical images showing the thermal‐induced shrinking of poly(NIPAAm) helix during gradual heating from 25°C to 50°C. H , p , α , and L denote axial length, pitch length, pitch angle, and total length, respectively. c) Comparison of normalized axial ( H/H 0 ) and total ( L/L 0 ) length changes of the poly(NIPAAm) helix during heating. d) Plots showing the variations in the number of turns ( n , left y ‐axis) and pitch angle ( α , right y ‐axis) of the poly(NIPAAm) helix during heating. n was calculated as H/p . e) Finite Element Method <t>(FEM)</t> <t>simulation</t> results showing the strain distribution within the poly(NIPAAm) helix during thermal shrinkage. The color map represents the maximum principal logarithmic strain (LE, Max. Principal). f) Comparison of experimental (Exp.) and finite element method (FEM) simulation results of the poly(NIPAAm) helix before heating (25°C) and after heating (50°C). The bar graphs show changes in H 50°C / H 25°C , n 50°C / n 25°C , and α 25°C – α 50°C , representing the axial length ratio, number‐of‐turns ratio, and pitch‐angle change, respectively. g) Chemically induced shrinking of the poly(NIPAAm) helix (left) and the corresponding change in H (right). A sponge containing 60 wt.% nitric acid was introduced into water at 25°C to generate localized acidic stimuli. h) NIR‐induced shrinking of the poly(NIPAAm) helix (left) and the corresponding change in H (right) under localized irradiation in a 0.01 wt.% graphene oxide aqueous solution at 25°C. i) Schematic illustration of a poly(NIPAAm) helix with a gradual variation in 2 r along its axis, where 2 r L (1.49 mm) is larger than 2 r R (1.16 mm), wrapped around a taut string. j) Time‐lapse images showing stepwise translation during periodic heating and cooling in water using a Peltier plate at 70°C for 1500 s and 5°C for 1500 s. k) Tracked positions of the left foot, right foot, and center along the string and the corresponding change in helix length calculated as the distance between the two feet.
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    Thermally, chemically, and NIR‐responsive shrinking behaviors of poly(NIPAAm) helix. a) Scheme of the motion of a Vorticella ’s stalk in response to external threats (physical or chemical stimuli) from predators. b) Optical images showing the thermal‐induced shrinking of poly(NIPAAm) helix during gradual heating from 25°C to 50°C. H , p , α , and L denote axial length, pitch length, pitch angle, and total length, respectively. c) Comparison of normalized axial ( H/H 0 ) and total ( L/L 0 ) length changes of the poly(NIPAAm) helix during heating. d) Plots showing the variations in the number of turns ( n , left y ‐axis) and pitch angle ( α , right y ‐axis) of the poly(NIPAAm) helix during heating. n was calculated as H/p . e) Finite Element Method <t>(FEM)</t> <t>simulation</t> results showing the strain distribution within the poly(NIPAAm) helix during thermal shrinkage. The color map represents the maximum principal logarithmic strain (LE, Max. Principal). f) Comparison of experimental (Exp.) and finite element method (FEM) simulation results of the poly(NIPAAm) helix before heating (25°C) and after heating (50°C). The bar graphs show changes in H 50°C / H 25°C , n 50°C / n 25°C , and α 25°C – α 50°C , representing the axial length ratio, number‐of‐turns ratio, and pitch‐angle change, respectively. g) Chemically induced shrinking of the poly(NIPAAm) helix (left) and the corresponding change in H (right). A sponge containing 60 wt.% nitric acid was introduced into water at 25°C to generate localized acidic stimuli. h) NIR‐induced shrinking of the poly(NIPAAm) helix (left) and the corresponding change in H (right) under localized irradiation in a 0.01 wt.% graphene oxide aqueous solution at 25°C. i) Schematic illustration of a poly(NIPAAm) helix with a gradual variation in 2 r along its axis, where 2 r L (1.49 mm) is larger than 2 r R (1.16 mm), wrapped around a taut string. j) Time‐lapse images showing stepwise translation during periodic heating and cooling in water using a Peltier plate at 70°C for 1500 s and 5°C for 1500 s. k) Tracked positions of the left foot, right foot, and center along the string and the corresponding change in helix length calculated as the distance between the two feet.
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    Thermally, chemically, and NIR‐responsive shrinking behaviors of poly(NIPAAm) helix. a) Scheme of the motion of a Vorticella ’s stalk in response to external threats (physical or chemical stimuli) from predators. b) Optical images showing the thermal‐induced shrinking of poly(NIPAAm) helix during gradual heating from 25°C to 50°C. H , p , α , and L denote axial length, pitch length, pitch angle, and total length, respectively. c) Comparison of normalized axial ( H/H 0 ) and total ( L/L 0 ) length changes of the poly(NIPAAm) helix during heating. d) Plots showing the variations in the number of turns ( n , left y ‐axis) and pitch angle ( α , right y ‐axis) of the poly(NIPAAm) helix during heating. n was calculated as H/p . e) Finite Element Method <t>(FEM)</t> <t>simulation</t> results showing the strain distribution within the poly(NIPAAm) helix during thermal shrinkage. The color map represents the maximum principal logarithmic strain (LE, Max. Principal). f) Comparison of experimental (Exp.) and finite element method (FEM) simulation results of the poly(NIPAAm) helix before heating (25°C) and after heating (50°C). The bar graphs show changes in H 50°C / H 25°C , n 50°C / n 25°C , and α 25°C – α 50°C , representing the axial length ratio, number‐of‐turns ratio, and pitch‐angle change, respectively. g) Chemically induced shrinking of the poly(NIPAAm) helix (left) and the corresponding change in H (right). A sponge containing 60 wt.% nitric acid was introduced into water at 25°C to generate localized acidic stimuli. h) NIR‐induced shrinking of the poly(NIPAAm) helix (left) and the corresponding change in H (right) under localized irradiation in a 0.01 wt.% graphene oxide aqueous solution at 25°C. i) Schematic illustration of a poly(NIPAAm) helix with a gradual variation in 2 r along its axis, where 2 r L (1.49 mm) is larger than 2 r R (1.16 mm), wrapped around a taut string. j) Time‐lapse images showing stepwise translation during periodic heating and cooling in water using a Peltier plate at 70°C for 1500 s and 5°C for 1500 s. k) Tracked positions of the left foot, right foot, and center along the string and the corresponding change in helix length calculated as the distance between the two feet.
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    december 2025 fem t10 simulations  (Abaqus Inc)
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    Thermally, chemically, and NIR‐responsive shrinking behaviors of poly(NIPAAm) helix. a) Scheme of the motion of a Vorticella ’s stalk in response to external threats (physical or chemical stimuli) from predators. b) Optical images showing the thermal‐induced shrinking of poly(NIPAAm) helix during gradual heating from 25°C to 50°C. H , p , α , and L denote axial length, pitch length, pitch angle, and total length, respectively. c) Comparison of normalized axial ( H/H 0 ) and total ( L/L 0 ) length changes of the poly(NIPAAm) helix during heating. d) Plots showing the variations in the number of turns ( n , left y ‐axis) and pitch angle ( α , right y ‐axis) of the poly(NIPAAm) helix during heating. n was calculated as H/p . e) Finite Element Method <t>(FEM)</t> <t>simulation</t> results showing the strain distribution within the poly(NIPAAm) helix during thermal shrinkage. The color map represents the maximum principal logarithmic strain (LE, Max. Principal). f) Comparison of experimental (Exp.) and finite element method (FEM) simulation results of the poly(NIPAAm) helix before heating (25°C) and after heating (50°C). The bar graphs show changes in H 50°C / H 25°C , n 50°C / n 25°C , and α 25°C – α 50°C , representing the axial length ratio, number‐of‐turns ratio, and pitch‐angle change, respectively. g) Chemically induced shrinking of the poly(NIPAAm) helix (left) and the corresponding change in H (right). A sponge containing 60 wt.% nitric acid was introduced into water at 25°C to generate localized acidic stimuli. h) NIR‐induced shrinking of the poly(NIPAAm) helix (left) and the corresponding change in H (right) under localized irradiation in a 0.01 wt.% graphene oxide aqueous solution at 25°C. i) Schematic illustration of a poly(NIPAAm) helix with a gradual variation in 2 r along its axis, where 2 r L (1.49 mm) is larger than 2 r R (1.16 mm), wrapped around a taut string. j) Time‐lapse images showing stepwise translation during periodic heating and cooling in water using a Peltier plate at 70°C for 1500 s and 5°C for 1500 s. k) Tracked positions of the left foot, right foot, and center along the string and the corresponding change in helix length calculated as the distance between the two feet.
    December 2025 Fem T10 Simulations, supplied by Abaqus Inc, used in various techniques. Bioz Stars score: 86/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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    Thermally, chemically, and NIR‐responsive shrinking behaviors of poly(NIPAAm) helix. a) Scheme of the motion of a Vorticella ’s stalk in response to external threats (physical or chemical stimuli) from predators. b) Optical images showing the thermal‐induced shrinking of poly(NIPAAm) helix during gradual heating from 25°C to 50°C. H , p , α , and L denote axial length, pitch length, pitch angle, and total length, respectively. c) Comparison of normalized axial ( H/H 0 ) and total ( L/L 0 ) length changes of the poly(NIPAAm) helix during heating. d) Plots showing the variations in the number of turns ( n , left y ‐axis) and pitch angle ( α , right y ‐axis) of the poly(NIPAAm) helix during heating. n was calculated as H/p . e) Finite Element Method (FEM) simulation results showing the strain distribution within the poly(NIPAAm) helix during thermal shrinkage. The color map represents the maximum principal logarithmic strain (LE, Max. Principal). f) Comparison of experimental (Exp.) and finite element method (FEM) simulation results of the poly(NIPAAm) helix before heating (25°C) and after heating (50°C). The bar graphs show changes in H 50°C / H 25°C , n 50°C / n 25°C , and α 25°C – α 50°C , representing the axial length ratio, number‐of‐turns ratio, and pitch‐angle change, respectively. g) Chemically induced shrinking of the poly(NIPAAm) helix (left) and the corresponding change in H (right). A sponge containing 60 wt.% nitric acid was introduced into water at 25°C to generate localized acidic stimuli. h) NIR‐induced shrinking of the poly(NIPAAm) helix (left) and the corresponding change in H (right) under localized irradiation in a 0.01 wt.% graphene oxide aqueous solution at 25°C. i) Schematic illustration of a poly(NIPAAm) helix with a gradual variation in 2 r along its axis, where 2 r L (1.49 mm) is larger than 2 r R (1.16 mm), wrapped around a taut string. j) Time‐lapse images showing stepwise translation during periodic heating and cooling in water using a Peltier plate at 70°C for 1500 s and 5°C for 1500 s. k) Tracked positions of the left foot, right foot, and center along the string and the corresponding change in helix length calculated as the distance between the two feet.

    Journal: Advanced Materials (Deerfield Beach, Fla.)

    Article Title: Self‐Oscillating Helix Showing Amplified Winding and Unwinding Motions

    doi: 10.1002/adma.202521736

    Figure Lengend Snippet: Thermally, chemically, and NIR‐responsive shrinking behaviors of poly(NIPAAm) helix. a) Scheme of the motion of a Vorticella ’s stalk in response to external threats (physical or chemical stimuli) from predators. b) Optical images showing the thermal‐induced shrinking of poly(NIPAAm) helix during gradual heating from 25°C to 50°C. H , p , α , and L denote axial length, pitch length, pitch angle, and total length, respectively. c) Comparison of normalized axial ( H/H 0 ) and total ( L/L 0 ) length changes of the poly(NIPAAm) helix during heating. d) Plots showing the variations in the number of turns ( n , left y ‐axis) and pitch angle ( α , right y ‐axis) of the poly(NIPAAm) helix during heating. n was calculated as H/p . e) Finite Element Method (FEM) simulation results showing the strain distribution within the poly(NIPAAm) helix during thermal shrinkage. The color map represents the maximum principal logarithmic strain (LE, Max. Principal). f) Comparison of experimental (Exp.) and finite element method (FEM) simulation results of the poly(NIPAAm) helix before heating (25°C) and after heating (50°C). The bar graphs show changes in H 50°C / H 25°C , n 50°C / n 25°C , and α 25°C – α 50°C , representing the axial length ratio, number‐of‐turns ratio, and pitch‐angle change, respectively. g) Chemically induced shrinking of the poly(NIPAAm) helix (left) and the corresponding change in H (right). A sponge containing 60 wt.% nitric acid was introduced into water at 25°C to generate localized acidic stimuli. h) NIR‐induced shrinking of the poly(NIPAAm) helix (left) and the corresponding change in H (right) under localized irradiation in a 0.01 wt.% graphene oxide aqueous solution at 25°C. i) Schematic illustration of a poly(NIPAAm) helix with a gradual variation in 2 r along its axis, where 2 r L (1.49 mm) is larger than 2 r R (1.16 mm), wrapped around a taut string. j) Time‐lapse images showing stepwise translation during periodic heating and cooling in water using a Peltier plate at 70°C for 1500 s and 5°C for 1500 s. k) Tracked positions of the left foot, right foot, and center along the string and the corresponding change in helix length calculated as the distance between the two feet.

    Article Snippet: We performed the FEM simulation using commercial software ABAQUS/Standard (see for details).

    Techniques: Comparison, Irradiation