W.T. van Horssen
Please Note
18 records found
1
This thesis aims to build upon the work conducted by Su et al. [1]; their paper studies the vibration of an inclined cable with an attached Tuned Mass Damper (TMD). In particular, as Su et al. assume that the cable takes the shape of a parabola in equilibrium, the goal is to find a better estimate of the equilibrium configuration of the cable. To this end, this thesis will utilise a modified version of the method used by Caswita [2]; Caswita derives the equations of motion of a cable without any attached mass by applying Lagrangian mechanics.
The results show that the equilibrium position differs meaningfully from a parabola. The ordinary differential equations that Su et al. obtain by using Galerkin’s method are also considerably different when using the alternative equilibrium position. These differences are mainly caused by the fact that the cable hangs on an incline, rather than by the addition of the TMD. ...
This thesis aims to build upon the work conducted by Su et al. [1]; their paper studies the vibration of an inclined cable with an attached Tuned Mass Damper (TMD). In particular, as Su et al. assume that the cable takes the shape of a parabola in equilibrium, the goal is to find a better estimate of the equilibrium configuration of the cable. To this end, this thesis will utilise a modified version of the method used by Caswita [2]; Caswita derives the equations of motion of a cable without any attached mass by applying Lagrangian mechanics.
The results show that the equilibrium position differs meaningfully from a parabola. The ordinary differential equations that Su et al. obtain by using Galerkin’s method are also considerably different when using the alternative equilibrium position. These differences are mainly caused by the fact that the cable hangs on an incline, rather than by the addition of the TMD.
The study focuses on investigating the primary resonance frequencies and understanding how pulsation frequencies near those resonance frequencies impact the stability of the system. Furthermore, we elaborate on special resonance cases where multiple oscillatory modes interact leading to even more complicated dynamics.
By building upon existing literature this research enhances our understanding of stability and dynamic behaviors under various flow pulsation frequencies. This study makes an important contribution to the present literature by exploring scenarios where multiple resonant modes interact, due to coinciding primary resonance frequencies, which has not been extensively discussed in the literature. Our findings suggests scepticism on the relevance of the existing solution methods and results in the literature for certain parameter values. ...
The study focuses on investigating the primary resonance frequencies and understanding how pulsation frequencies near those resonance frequencies impact the stability of the system. Furthermore, we elaborate on special resonance cases where multiple oscillatory modes interact leading to even more complicated dynamics.
By building upon existing literature this research enhances our understanding of stability and dynamic behaviors under various flow pulsation frequencies. This study makes an important contribution to the present literature by exploring scenarios where multiple resonant modes interact, due to coinciding primary resonance frequencies, which has not been extensively discussed in the literature. Our findings suggests scepticism on the relevance of the existing solution methods and results in the literature for certain parameter values.
The dimensions in the equations were removed. Applying a perturbation method yielded hierarchic partial differential equations by introducing the wave amplitude divided by the depth of the ocean as a small perturbation parameter. The analytical solution of the first order problem was found by applying separation of variables and by using a Fourier transform. For certain classes of problems it is shown in this report that it is possible to analytically solve a model for fluid-structure interaction in offshore solar farms for various initial conditions. ...
The dimensions in the equations were removed. Applying a perturbation method yielded hierarchic partial differential equations by introducing the wave amplitude divided by the depth of the ocean as a small perturbation parameter. The analytical solution of the first order problem was found by applying separation of variables and by using a Fourier transform. For certain classes of problems it is shown in this report that it is possible to analytically solve a model for fluid-structure interaction in offshore solar farms for various initial conditions.
how effective this TMD system damps. Using the multiple time scale perturbation method, the displacements of the cable and TMD system are calculated. This results in the reflected wave being damped by the TMD system, but the transmitted wave having a larger is placement than expected. The displacement of the TMD system also had unrealistic outcomes. To calculate the effectiveness of the TMD system, the energy which has been lost has to be calculated. Since the displacement of the TMD system had unrealistic outcomes, the calculation of
the energy is not realistic either. ...
how effective this TMD system damps. Using the multiple time scale perturbation method, the displacements of the cable and TMD system are calculated. This results in the reflected wave being damped by the TMD system, but the transmitted wave having a larger is placement than expected. The displacement of the TMD system also had unrealistic outcomes. To calculate the effectiveness of the TMD system, the energy which has been lost has to be calculated. Since the displacement of the TMD system had unrealistic outcomes, the calculation of
the energy is not realistic either.
To address these issues, sequentially linear analysis (SLA) was developed which exploits the fact that a linear analysis is inherently stable. By assuming a stepwise material degradation the nonlinear response of a structure can be approximated with a sequence of linear analyses. Although this approach has been proven to be effective for several case studies, the numerical performance is still a problem that has to be solved. After every linear analysis, a single element is damaged resulting in incremental damage. As a result, the system of equations only changes locally between these linear analyses. Traditional solution techniques do not exploit this property and calculate a matrix factorisation every linear analysis, resulting in high computational times per analysis step. Since SLA typically requires many linear analyses to obtain the desired structural response, this leads to unacceptable analysis times. The aim of this thesis is to improve the computational performance of SLA by developing numerical solution techniques which exploit the incremental approach of SLA. To this extend, the following methods have been developed.
A direct solution technique has been developed which is based on the Woodbury matrix identity. This identity allows for the numerically cheap computation of the inverse of a low-rank corrected matrix. In this approach, the expensive matrix factorisation does not have to be calculated every linear analysis step. Instead, the old factorisation can be reused along with some additional matrix- and vector multiplications and solving a significantly smaller linear system of equations. An optimal strategy is derived to determine at which point a new factorisation should be calculated.
An improved preconditioner for the conjugate gradient (CG) method has been developed. Instead of an incomplete factorisation, the complete factorisation is used as a preconditioner which reduces the number of required CG iterations significantly. The point at which too many CG iterations are required and a new factorisation is necessary, is determined using the same strategy as the first method. From numerical experiments it follows that both methods perform significantly better than the direct solution method, especially for large 3-dimensional problems. The best performance is achieved using the Woodbury matrix identity resulting in the solver no longer being the dominant factor in SLA. Furthermore, significantly larger problems are not solvable in time frames in which previously only smaller problems were solved. ...
To address these issues, sequentially linear analysis (SLA) was developed which exploits the fact that a linear analysis is inherently stable. By assuming a stepwise material degradation the nonlinear response of a structure can be approximated with a sequence of linear analyses. Although this approach has been proven to be effective for several case studies, the numerical performance is still a problem that has to be solved. After every linear analysis, a single element is damaged resulting in incremental damage. As a result, the system of equations only changes locally between these linear analyses. Traditional solution techniques do not exploit this property and calculate a matrix factorisation every linear analysis, resulting in high computational times per analysis step. Since SLA typically requires many linear analyses to obtain the desired structural response, this leads to unacceptable analysis times. The aim of this thesis is to improve the computational performance of SLA by developing numerical solution techniques which exploit the incremental approach of SLA. To this extend, the following methods have been developed.
A direct solution technique has been developed which is based on the Woodbury matrix identity. This identity allows for the numerically cheap computation of the inverse of a low-rank corrected matrix. In this approach, the expensive matrix factorisation does not have to be calculated every linear analysis step. Instead, the old factorisation can be reused along with some additional matrix- and vector multiplications and solving a significantly smaller linear system of equations. An optimal strategy is derived to determine at which point a new factorisation should be calculated.
An improved preconditioner for the conjugate gradient (CG) method has been developed. Instead of an incomplete factorisation, the complete factorisation is used as a preconditioner which reduces the number of required CG iterations significantly. The point at which too many CG iterations are required and a new factorisation is necessary, is determined using the same strategy as the first method. From numerical experiments it follows that both methods perform significantly better than the direct solution method, especially for large 3-dimensional problems. The best performance is achieved using the Woodbury matrix identity resulting in the solver no longer being the dominant factor in SLA. Furthermore, significantly larger problems are not solvable in time frames in which previously only smaller problems were solved.
In this project the transversal vibrations of an accelerating elevator cable system are studied, with the aim to find the resonance times, the resonance duration and the resonance amplitude. The elevator cable is modelled as an axially moving string, with length given by l(t) = l0 + 1/2 at2, with a the acceleration and t the time. The cable is sinusoidally excited at the top and fixed at the bottom. It is assumed that the axial acceleration is small compared to the transversal acceleration, that the cable mass is small compared to the car mass, and that the excitation amplitude is small compared to the length of the cable. Using these estimations, the solution for the transversal displacement u is approximated up to O(ε) with ε a small parameter. The elevator cable goes through a cascade of autoresonances: the eigenfrequencies of the cable are varying because the cable length is varying, and at several times an eigenfrequency matches the excitation frequency. These are the resonance times, and they have been found as t+ = (2/εa1l0)1/2arccos((Ωl0/χk)1/2), with t+ a measure of oscillation of t, Ω the angular excitation frequency, l0 the initial length, χk the eigenfrequency of mode k and εa1 = a. The duration of the resonances (the timescale) is shown to be O(ε-1/4) if χk≠Ωl0 and O(ε-1/6) if χk=Ωl0 (a bifurcation of the problem). The amplitude scale is thus O(ε3/4) or O(ε5/6), respectively, and solutions for the amplitude are calculated both outside and inside the resonance zone. ...
In this project the transversal vibrations of an accelerating elevator cable system are studied, with the aim to find the resonance times, the resonance duration and the resonance amplitude. The elevator cable is modelled as an axially moving string, with length given by l(t) = l0 + 1/2 at2, with a the acceleration and t the time. The cable is sinusoidally excited at the top and fixed at the bottom. It is assumed that the axial acceleration is small compared to the transversal acceleration, that the cable mass is small compared to the car mass, and that the excitation amplitude is small compared to the length of the cable. Using these estimations, the solution for the transversal displacement u is approximated up to O(ε) with ε a small parameter. The elevator cable goes through a cascade of autoresonances: the eigenfrequencies of the cable are varying because the cable length is varying, and at several times an eigenfrequency matches the excitation frequency. These are the resonance times, and they have been found as t+ = (2/εa1l0)1/2arccos((Ωl0/χk)1/2), with t+ a measure of oscillation of t, Ω the angular excitation frequency, l0 the initial length, χk the eigenfrequency of mode k and εa1 = a. The duration of the resonances (the timescale) is shown to be O(ε-1/4) if χk≠Ωl0 and O(ε-1/6) if χk=Ωl0 (a bifurcation of the problem). The amplitude scale is thus O(ε3/4) or O(ε5/6), respectively, and solutions for the amplitude are calculated both outside and inside the resonance zone.
of the time-varying masses the eigenfrequencies are analyzed, stability properties are derived, and approximations of the solutions are given. ...
of the time-varying masses the eigenfrequencies are analyzed, stability properties are derived, and approximations of the solutions are given.