Thi-Hoa Nguyen, Bruno A. Roccia, Dominik Schillinger, Cristian G. Gebhardt
{"title":"无剪切和无扭转杆非线性动力学的节点和等几何公式研究","authors":"Thi-Hoa Nguyen, Bruno A. Roccia, Dominik Schillinger, Cristian G. Gebhardt","doi":"10.1002/nme.70104","DOIUrl":null,"url":null,"abstract":"<div>\n \n <p>In this work, we compare the nodal and isogeometric spatial discretization schemes for the nonlinear formulation of shear- and torsion-free rods introduced in Gebhardt and Romero (see Reference no. 31). We investigate the resulting discrete solution space, the accuracy, and the computational cost of these spatial discretization schemes. To fulfill the required <span></span><math>\n <semantics>\n <mrow>\n <msup>\n <mrow>\n <mi>C</mi>\n </mrow>\n <mrow>\n <mn>1</mn>\n </mrow>\n </msup>\n </mrow>\n <annotation>$$ {C}^1 $$</annotation>\n </semantics></math> continuity of the rod formulation, the nodal scheme discretizes the rod in terms of its nodal positions and directors using cubic Hermite splines. Isogeometric discretizations naturally fulfill this with smooth spline basis functions and discretize the rod only in terms of the positions of the control points (see Nguyen et al. in Reference no. 41), which leads to a discrete solution in multiple copies of the Euclidean space <span></span><math>\n <semantics>\n <mrow>\n <msup>\n <mrow>\n <mi>ℝ</mi>\n </mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msup>\n </mrow>\n <annotation>$$ {\\mathbb{R}}^3 $$</annotation>\n </semantics></math>. They enable the employment of basis functions of one degree lower, that is, quadratic <span></span><math>\n <semantics>\n <mrow>\n <msup>\n <mrow>\n <mi>C</mi>\n </mrow>\n <mrow>\n <mn>1</mn>\n </mrow>\n </msup>\n </mrow>\n <annotation>$$ {C}^1 $$</annotation>\n </semantics></math> splines, and possibly reduce the number of degrees of freedom (dofs). When using the nodal scheme, since the defined director field is in the unit sphere <span></span><math>\n <semantics>\n <mrow>\n <msup>\n <mrow>\n <mi>S</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msup>\n </mrow>\n <annotation>$$ {S}^2 $$</annotation>\n </semantics></math>, preserving this for the nodal director variable field requires an additional constraint of unit nodal directors. This leads to a discrete solution in multiple copies of the manifold <span></span><math>\n <semantics>\n <mrow>\n <msup>\n <mrow>\n <mi>ℝ</mi>\n </mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msup>\n <mo>×</mo>\n <msup>\n <mrow>\n <mi>S</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msup>\n </mrow>\n <annotation>$$ {\\mathbb{R}}^3\\times {S}^2 $$</annotation>\n </semantics></math>; however, it results in zero nodal axial stress values. Allowing arbitrary length for the nodal directors, that is a nodal director field in <span></span><math>\n <semantics>\n <mrow>\n <msup>\n <mrow>\n <mi>ℝ</mi>\n </mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msup>\n </mrow>\n <annotation>$$ {\\mathbb{R}}^3 $$</annotation>\n </semantics></math> instead of <span></span><math>\n <semantics>\n <mrow>\n <msup>\n <mrow>\n <mi>S</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msup>\n </mrow>\n <annotation>$$ {S}^2 $$</annotation>\n </semantics></math> as within discrete rod elements, eliminates the constrained nodal axial stresses and leads to a discrete solution in multiple copies of <span></span><math>\n <semantics>\n <mrow>\n <msup>\n <mrow>\n <mi>ℝ</mi>\n </mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msup>\n </mrow>\n <annotation>$$ {\\mathbb{R}}^3 $$</annotation>\n </semantics></math>. To enforce the unit nodal director constraint, we discuss two approaches using the Lagrange multiplier and penalty methods. We compare the resulting semi-discrete formulations and the computational cost of these discretization variants. We numerically demonstrate our findings via examples of a planar roll-up, a catenary, and a mooring line.</p>\n </div>","PeriodicalId":13699,"journal":{"name":"International Journal for Numerical Methods in Engineering","volume":"126 16","pages":""},"PeriodicalIF":2.9000,"publicationDate":"2025-08-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A Study on Nodal and Isogeometric Formulations for Nonlinear Dynamics of Shear- and Torsion-Free Rods\",\"authors\":\"Thi-Hoa Nguyen, Bruno A. Roccia, Dominik Schillinger, Cristian G. Gebhardt\",\"doi\":\"10.1002/nme.70104\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div>\\n \\n <p>In this work, we compare the nodal and isogeometric spatial discretization schemes for the nonlinear formulation of shear- and torsion-free rods introduced in Gebhardt and Romero (see Reference no. 31). We investigate the resulting discrete solution space, the accuracy, and the computational cost of these spatial discretization schemes. To fulfill the required <span></span><math>\\n <semantics>\\n <mrow>\\n <msup>\\n <mrow>\\n <mi>C</mi>\\n </mrow>\\n <mrow>\\n <mn>1</mn>\\n </mrow>\\n </msup>\\n </mrow>\\n <annotation>$$ {C}^1 $$</annotation>\\n </semantics></math> continuity of the rod formulation, the nodal scheme discretizes the rod in terms of its nodal positions and directors using cubic Hermite splines. Isogeometric discretizations naturally fulfill this with smooth spline basis functions and discretize the rod only in terms of the positions of the control points (see Nguyen et al. in Reference no. 41), which leads to a discrete solution in multiple copies of the Euclidean space <span></span><math>\\n <semantics>\\n <mrow>\\n <msup>\\n <mrow>\\n <mi>ℝ</mi>\\n </mrow>\\n <mrow>\\n <mn>3</mn>\\n </mrow>\\n </msup>\\n </mrow>\\n <annotation>$$ {\\\\mathbb{R}}^3 $$</annotation>\\n </semantics></math>. They enable the employment of basis functions of one degree lower, that is, quadratic <span></span><math>\\n <semantics>\\n <mrow>\\n <msup>\\n <mrow>\\n <mi>C</mi>\\n </mrow>\\n <mrow>\\n <mn>1</mn>\\n </mrow>\\n </msup>\\n </mrow>\\n <annotation>$$ {C}^1 $$</annotation>\\n </semantics></math> splines, and possibly reduce the number of degrees of freedom (dofs). When using the nodal scheme, since the defined director field is in the unit sphere <span></span><math>\\n <semantics>\\n <mrow>\\n <msup>\\n <mrow>\\n <mi>S</mi>\\n </mrow>\\n <mrow>\\n <mn>2</mn>\\n </mrow>\\n </msup>\\n </mrow>\\n <annotation>$$ {S}^2 $$</annotation>\\n </semantics></math>, preserving this for the nodal director variable field requires an additional constraint of unit nodal directors. This leads to a discrete solution in multiple copies of the manifold <span></span><math>\\n <semantics>\\n <mrow>\\n <msup>\\n <mrow>\\n <mi>ℝ</mi>\\n </mrow>\\n <mrow>\\n <mn>3</mn>\\n </mrow>\\n </msup>\\n <mo>×</mo>\\n <msup>\\n <mrow>\\n <mi>S</mi>\\n </mrow>\\n <mrow>\\n <mn>2</mn>\\n </mrow>\\n </msup>\\n </mrow>\\n <annotation>$$ {\\\\mathbb{R}}^3\\\\times {S}^2 $$</annotation>\\n </semantics></math>; however, it results in zero nodal axial stress values. Allowing arbitrary length for the nodal directors, that is a nodal director field in <span></span><math>\\n <semantics>\\n <mrow>\\n <msup>\\n <mrow>\\n <mi>ℝ</mi>\\n </mrow>\\n <mrow>\\n <mn>3</mn>\\n </mrow>\\n </msup>\\n </mrow>\\n <annotation>$$ {\\\\mathbb{R}}^3 $$</annotation>\\n </semantics></math> instead of <span></span><math>\\n <semantics>\\n <mrow>\\n <msup>\\n <mrow>\\n <mi>S</mi>\\n </mrow>\\n <mrow>\\n <mn>2</mn>\\n </mrow>\\n </msup>\\n </mrow>\\n <annotation>$$ {S}^2 $$</annotation>\\n </semantics></math> as within discrete rod elements, eliminates the constrained nodal axial stresses and leads to a discrete solution in multiple copies of <span></span><math>\\n <semantics>\\n <mrow>\\n <msup>\\n <mrow>\\n <mi>ℝ</mi>\\n </mrow>\\n <mrow>\\n <mn>3</mn>\\n </mrow>\\n </msup>\\n </mrow>\\n <annotation>$$ {\\\\mathbb{R}}^3 $$</annotation>\\n </semantics></math>. To enforce the unit nodal director constraint, we discuss two approaches using the Lagrange multiplier and penalty methods. We compare the resulting semi-discrete formulations and the computational cost of these discretization variants. We numerically demonstrate our findings via examples of a planar roll-up, a catenary, and a mooring line.</p>\\n </div>\",\"PeriodicalId\":13699,\"journal\":{\"name\":\"International Journal for Numerical Methods in Engineering\",\"volume\":\"126 16\",\"pages\":\"\"},\"PeriodicalIF\":2.9000,\"publicationDate\":\"2025-08-19\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"International Journal for Numerical Methods in Engineering\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1002/nme.70104\",\"RegionNum\":3,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"ENGINEERING, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Journal for Numerical Methods in Engineering","FirstCategoryId":"5","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/nme.70104","RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ENGINEERING, MULTIDISCIPLINARY","Score":null,"Total":0}
A Study on Nodal and Isogeometric Formulations for Nonlinear Dynamics of Shear- and Torsion-Free Rods
In this work, we compare the nodal and isogeometric spatial discretization schemes for the nonlinear formulation of shear- and torsion-free rods introduced in Gebhardt and Romero (see Reference no. 31). We investigate the resulting discrete solution space, the accuracy, and the computational cost of these spatial discretization schemes. To fulfill the required continuity of the rod formulation, the nodal scheme discretizes the rod in terms of its nodal positions and directors using cubic Hermite splines. Isogeometric discretizations naturally fulfill this with smooth spline basis functions and discretize the rod only in terms of the positions of the control points (see Nguyen et al. in Reference no. 41), which leads to a discrete solution in multiple copies of the Euclidean space . They enable the employment of basis functions of one degree lower, that is, quadratic splines, and possibly reduce the number of degrees of freedom (dofs). When using the nodal scheme, since the defined director field is in the unit sphere , preserving this for the nodal director variable field requires an additional constraint of unit nodal directors. This leads to a discrete solution in multiple copies of the manifold ; however, it results in zero nodal axial stress values. Allowing arbitrary length for the nodal directors, that is a nodal director field in instead of as within discrete rod elements, eliminates the constrained nodal axial stresses and leads to a discrete solution in multiple copies of . To enforce the unit nodal director constraint, we discuss two approaches using the Lagrange multiplier and penalty methods. We compare the resulting semi-discrete formulations and the computational cost of these discretization variants. We numerically demonstrate our findings via examples of a planar roll-up, a catenary, and a mooring line.
期刊介绍:
The International Journal for Numerical Methods in Engineering publishes original papers describing significant, novel developments in numerical methods that are applicable to engineering problems.
The Journal is known for welcoming contributions in a wide range of areas in computational engineering, including computational issues in model reduction, uncertainty quantification, verification and validation, inverse analysis and stochastic methods, optimisation, element technology, solution techniques and parallel computing, damage and fracture, mechanics at micro and nano-scales, low-speed fluid dynamics, fluid-structure interaction, electromagnetics, coupled diffusion phenomena, and error estimation and mesh generation. It is emphasized that this is by no means an exhaustive list, and particularly papers on multi-scale, multi-physics or multi-disciplinary problems, and on new, emerging topics are welcome.