VISUALISASI FENOMENA HARMONIS DAN CHAOS PADA GETARAN TERGANDENG BERBASIS KOMPUTASI NUMERIK RUNGE KUTTA

Leonora L. R. Trifina, Ali Warsito, L. A. S. Lapono, Andreas Ch. Louk
{"title":"VISUALISASI FENOMENA HARMONIS DAN CHAOS PADA GETARAN TERGANDENG BERBASIS KOMPUTASI NUMERIK RUNGE KUTTA","authors":"Leonora L. R. Trifina, Ali Warsito, L. A. S. Lapono, Andreas Ch. Louk","doi":"10.35508/fisa.v8i1.11817","DOIUrl":null,"url":null,"abstract":"Research has been carried out on the visualization of harmonic and chaos phenomenont on coupled vibration physcal case using the Runge Kutta numerical computation method with the aim of applying the first to fourth order Runge Kutta computation method to obtain  a second order differential equation solution on coupled vibration system, calculating the displacement value of objects using computation method Runge Kutta order first to fourth, obtained a graph of the displacement of objects againts time in case of coupled vibration for harmonic and chaos states at certain step width values and compare the convergence of the Runge Kutta method from first to fourth order with the special analytical method. The solution of coupled vibration equation which is classified as a second order differential equation was quite difficulted to solve analytically, so the Runge Kutta computation method was used to solve it as an alternative solution. The results of the research showed that the harmonic state of the system was obtained when the displacement graph showed the motion of each pendulum which was constant with the pendulum displacement position with respect to time in the form of a sinusoidal graph at a value of C1 = 40 N/m, C2 = 30 N/m, C = 10 N/m, C = 0 N/m and the chaotic state was represented by a graph of the displacement of the pendulum with respect to time with an irregular pattern. In this case, it was found that the fourth order Runge Kutta method converged faster than the first to third order Runge Kutta method with the best results obtained at a step width value of 0,001. The fourth order Runge Kutta method also has a smaller approximation average error value  from first to third order Runge Kutta method was  on the fourth order Runge Kutta method and the avarage error values are , and  on the Runge Kutta method of first to third order.","PeriodicalId":367071,"journal":{"name":"Jurnal Fisika : Fisika Sains dan Aplikasinya","volume":"153 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2023-04-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Jurnal Fisika : Fisika Sains dan Aplikasinya","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.35508/fisa.v8i1.11817","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

Research has been carried out on the visualization of harmonic and chaos phenomenont on coupled vibration physcal case using the Runge Kutta numerical computation method with the aim of applying the first to fourth order Runge Kutta computation method to obtain  a second order differential equation solution on coupled vibration system, calculating the displacement value of objects using computation method Runge Kutta order first to fourth, obtained a graph of the displacement of objects againts time in case of coupled vibration for harmonic and chaos states at certain step width values and compare the convergence of the Runge Kutta method from first to fourth order with the special analytical method. The solution of coupled vibration equation which is classified as a second order differential equation was quite difficulted to solve analytically, so the Runge Kutta computation method was used to solve it as an alternative solution. The results of the research showed that the harmonic state of the system was obtained when the displacement graph showed the motion of each pendulum which was constant with the pendulum displacement position with respect to time in the form of a sinusoidal graph at a value of C1 = 40 N/m, C2 = 30 N/m, C = 10 N/m, C = 0 N/m and the chaotic state was represented by a graph of the displacement of the pendulum with respect to time with an irregular pattern. In this case, it was found that the fourth order Runge Kutta method converged faster than the first to third order Runge Kutta method with the best results obtained at a step width value of 0,001. The fourth order Runge Kutta method also has a smaller approximation average error value  from first to third order Runge Kutta method was  on the fourth order Runge Kutta method and the avarage error values are , and  on the Runge Kutta method of first to third order.
可视化现象和谐和混乱基于RUNGE KUTTA的计算数字振动
利用龙格库塔数值计算方法对耦合振动物理情况下的谐波和混沌现象进行了可视化研究,目的是应用一阶至四阶龙格库塔计算方法获得耦合振动系统的二阶微分方程解,利用龙格库塔一阶至四阶计算方法计算物体的位移值,得到了在一定步宽值下谐波与混沌状态耦合振动时物体位移随时间的变化曲线图,并比较了龙格-库塔法与特殊解析法在一阶到四阶的收敛性。耦合振动方程属于二阶微分方程,其解解析求解比较困难,因此采用龙格库塔计算方法作为备选解进行求解。研究的结果表明,系统的谐波状态时得到位移图显示每个摆的运动是恒定的摆位移位置对时间的正弦图的价值C1 = 40 N / m, C2 = 30 N / m, C = 10 N / m C = 0 N / m和混乱的状态是由图表示的位移摆对时间与一个不规则的图案。在这种情况下,发现四阶Runge Kutta方法比一阶到三阶Runge Kutta方法收敛速度更快,并且在步宽为0.001时获得最佳结果。四阶龙格库塔法的近似平均误差值也较小,一阶到三阶龙格库塔法的近似平均误差值为,四阶龙格库塔法的近似平均误差值为,而对一阶到三阶龙格库塔法的近似平均误差值为。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信