{"title":"计算线性时不变系统对周期输入信号的闭合响应的一种新方法","authors":"Ahmad Safaai-Jazi","doi":"10.1049/cds2.12142","DOIUrl":null,"url":null,"abstract":"<p>A new method for finding closed-form time-domain solutions of linear time-invariant (LTI) systems with arbitrary periodic input signals is presented. These solutions, unlike those obtained based on the conventional Fourier-phasor method, have a finite number of terms in one period. To implement the proposed method, the following steps are carried out: (1) For a given system, represented by a transfer function, an impulse response, a block diagram etc., the governing differential equation relating the output of the system, <math>\n <semantics>\n <mrow>\n <mi>y</mi>\n <mrow>\n <mo>(</mo>\n <mi>t</mi>\n <mo>)</mo>\n </mrow>\n </mrow>\n <annotation> $y(t)$</annotation>\n </semantics></math>, to its input, <math>\n <semantics>\n <mrow>\n <mi>x</mi>\n <mrow>\n <mo>(</mo>\n <mi>t</mi>\n <mo>)</mo>\n </mrow>\n </mrow>\n <annotation> $x(t)$</annotation>\n </semantics></math>, is obtained. (2) An auxiliary differential equation is formed by simply replacing <math>\n <semantics>\n <mrow>\n <mi>y</mi>\n <mrow>\n <mo>(</mo>\n <mi>t</mi>\n <mo>)</mo>\n </mrow>\n </mrow>\n <annotation> $y(t)$</annotation>\n </semantics></math> with <math>\n <semantics>\n <mrow>\n <mover>\n <mi>y</mi>\n <mo>‾</mo>\n </mover>\n <mrow>\n <mo>(</mo>\n <mi>t</mi>\n <mo>)</mo>\n </mrow>\n </mrow>\n <annotation> $\\overline{y}(t)$</annotation>\n </semantics></math> and equating the input side to<math>\n <semantics>\n <mrow>\n <mi>x</mi>\n <mrow>\n <mo>(</mo>\n <mi>t</mi>\n <mo>)</mo>\n </mrow>\n </mrow>\n <annotation> $x(t)$</annotation>\n </semantics></math> alone. The auxiliary differential equation is solved for each time segment of the input signal in one period, leaving the constant coefficients associated with the homogeneous solutions as unknowns. For an <i>n</i>th-order system with an input signal consisting of <i>q</i> segments in one period, there are <math>\n <semantics>\n <mrow>\n <mi>n</mi>\n <mo>×</mo>\n <mi>q</mi>\n </mrow>\n <annotation> $n\\times q$</annotation>\n </semantics></math> such unknown coefficients. (3) Continuity of <math>\n <semantics>\n <mrow>\n <mover>\n <mi>y</mi>\n <mo>‾</mo>\n </mover>\n <mrow>\n <mo>(</mo>\n <mi>t</mi>\n <mo>)</mo>\n </mrow>\n </mrow>\n <annotation> $\\overline{y}(t)$</annotation>\n </semantics></math> and its derivatives, <math>\n <semantics>\n <mrow>\n <msup>\n <mi>d</mi>\n <mi>k</mi>\n </msup>\n <mover>\n <mi>y</mi>\n <mo>‾</mo>\n </mover>\n <mrow>\n <mo>(</mo>\n <mi>t</mi>\n <mo>)</mo>\n </mrow>\n <mo>/</mo>\n <mi>d</mi>\n <msup>\n <mi>t</mi>\n <mi>k</mi>\n </msup>\n <mo>,</mo>\n </mrow>\n <annotation> ${d}^{k}\\overline{y}(t)/d{t}^{k},$</annotation>\n </semantics></math> <math>\n <semantics>\n <mrow>\n <mi>k</mi>\n <mo>=</mo>\n <mn>1</mn>\n <mo>,</mo>\n <mo>⋅</mo>\n <mo>⋅</mo>\n <mo>⋅</mo>\n <mo>,</mo>\n <mi>n</mi>\n <mo>−</mo>\n <mn>1</mn>\n <mo>,</mo>\n </mrow>\n <annotation> $k=1,\\cdot \\cdot \\cdot ,n-1,$</annotation>\n </semantics></math> at the connection points of successive segments and the periodicity conditions for the beginning and end points of the period are implemented. (4) The outcome of step 3 is a system of <math>\n <semantics>\n <mrow>\n <mi>n</mi>\n <mo>×</mo>\n <mi>q</mi>\n </mrow>\n <annotation> $n\\times q$</annotation>\n </semantics></math> equations in terms of <math>\n <semantics>\n <mrow>\n <mi>n</mi>\n <mo>×</mo>\n <mi>q</mi>\n </mrow>\n <annotation> $n\\times q$</annotation>\n </semantics></math> unknown coefficients described in step 2. Solving this system of equations, the solution for <math>\n <semantics>\n <mrow>\n <mover>\n <mi>y</mi>\n <mo>‾</mo>\n </mover>\n <mrow>\n <mo>(</mo>\n <mi>t</mi>\n <mo>)</mo>\n </mrow>\n </mrow>\n <annotation> $\\overline{y}(t)$</annotation>\n </semantics></math> in one period is obtained. (5) Finally, using the linearity and differentiation properties of the system and the coefficients of the input side of the differential equation of the system, the total response, <math>\n <semantics>\n <mrow>\n <mi>y</mi>\n <mrow>\n <mo>(</mo>\n <mi>t</mi>\n <mo>)</mo>\n </mrow>\n </mrow>\n <annotation> $y(t)$</annotation>\n </semantics></math>, in one period is constructed in terms of <math>\n <semantics>\n <mrow>\n <mover>\n <mi>y</mi>\n <mo>‾</mo>\n </mover>\n <mrow>\n <mo>(</mo>\n <mi>t</mi>\n <mo>)</mo>\n </mrow>\n </mrow>\n <annotation> $\\overline{y}(t)$</annotation>\n </semantics></math> and its derivatives. For stable LTI systems, the proposed method can be used without any limitations.</p>","PeriodicalId":50386,"journal":{"name":"Iet Circuits Devices & Systems","volume":"17 2","pages":"88-94"},"PeriodicalIF":1.0000,"publicationDate":"2023-01-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1049/cds2.12142","citationCount":"0","resultStr":"{\"title\":\"A new method for calculation of closed-form response of linear time-invariant systems to periodic input signals\",\"authors\":\"Ahmad Safaai-Jazi\",\"doi\":\"10.1049/cds2.12142\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>A new method for finding closed-form time-domain solutions of linear time-invariant (LTI) systems with arbitrary periodic input signals is presented. These solutions, unlike those obtained based on the conventional Fourier-phasor method, have a finite number of terms in one period. To implement the proposed method, the following steps are carried out: (1) For a given system, represented by a transfer function, an impulse response, a block diagram etc., the governing differential equation relating the output of the system, <math>\\n <semantics>\\n <mrow>\\n <mi>y</mi>\\n <mrow>\\n <mo>(</mo>\\n <mi>t</mi>\\n <mo>)</mo>\\n </mrow>\\n </mrow>\\n <annotation> $y(t)$</annotation>\\n </semantics></math>, to its input, <math>\\n <semantics>\\n <mrow>\\n <mi>x</mi>\\n <mrow>\\n <mo>(</mo>\\n <mi>t</mi>\\n <mo>)</mo>\\n </mrow>\\n </mrow>\\n <annotation> $x(t)$</annotation>\\n </semantics></math>, is obtained. (2) An auxiliary differential equation is formed by simply replacing <math>\\n <semantics>\\n <mrow>\\n <mi>y</mi>\\n <mrow>\\n <mo>(</mo>\\n <mi>t</mi>\\n <mo>)</mo>\\n </mrow>\\n </mrow>\\n <annotation> $y(t)$</annotation>\\n </semantics></math> with <math>\\n <semantics>\\n <mrow>\\n <mover>\\n <mi>y</mi>\\n <mo>‾</mo>\\n </mover>\\n <mrow>\\n <mo>(</mo>\\n <mi>t</mi>\\n <mo>)</mo>\\n </mrow>\\n </mrow>\\n <annotation> $\\\\overline{y}(t)$</annotation>\\n </semantics></math> and equating the input side to<math>\\n <semantics>\\n <mrow>\\n <mi>x</mi>\\n <mrow>\\n <mo>(</mo>\\n <mi>t</mi>\\n <mo>)</mo>\\n </mrow>\\n </mrow>\\n <annotation> $x(t)$</annotation>\\n </semantics></math> alone. The auxiliary differential equation is solved for each time segment of the input signal in one period, leaving the constant coefficients associated with the homogeneous solutions as unknowns. For an <i>n</i>th-order system with an input signal consisting of <i>q</i> segments in one period, there are <math>\\n <semantics>\\n <mrow>\\n <mi>n</mi>\\n <mo>×</mo>\\n <mi>q</mi>\\n </mrow>\\n <annotation> $n\\\\times q$</annotation>\\n </semantics></math> such unknown coefficients. (3) Continuity of <math>\\n <semantics>\\n <mrow>\\n <mover>\\n <mi>y</mi>\\n <mo>‾</mo>\\n </mover>\\n <mrow>\\n <mo>(</mo>\\n <mi>t</mi>\\n <mo>)</mo>\\n </mrow>\\n </mrow>\\n <annotation> $\\\\overline{y}(t)$</annotation>\\n </semantics></math> and its derivatives, <math>\\n <semantics>\\n <mrow>\\n <msup>\\n <mi>d</mi>\\n <mi>k</mi>\\n </msup>\\n <mover>\\n <mi>y</mi>\\n <mo>‾</mo>\\n </mover>\\n <mrow>\\n <mo>(</mo>\\n <mi>t</mi>\\n <mo>)</mo>\\n </mrow>\\n <mo>/</mo>\\n <mi>d</mi>\\n <msup>\\n <mi>t</mi>\\n <mi>k</mi>\\n </msup>\\n <mo>,</mo>\\n </mrow>\\n <annotation> ${d}^{k}\\\\overline{y}(t)/d{t}^{k},$</annotation>\\n </semantics></math> <math>\\n <semantics>\\n <mrow>\\n <mi>k</mi>\\n <mo>=</mo>\\n <mn>1</mn>\\n <mo>,</mo>\\n <mo>⋅</mo>\\n <mo>⋅</mo>\\n <mo>⋅</mo>\\n <mo>,</mo>\\n <mi>n</mi>\\n <mo>−</mo>\\n <mn>1</mn>\\n <mo>,</mo>\\n </mrow>\\n <annotation> $k=1,\\\\cdot \\\\cdot \\\\cdot ,n-1,$</annotation>\\n </semantics></math> at the connection points of successive segments and the periodicity conditions for the beginning and end points of the period are implemented. (4) The outcome of step 3 is a system of <math>\\n <semantics>\\n <mrow>\\n <mi>n</mi>\\n <mo>×</mo>\\n <mi>q</mi>\\n </mrow>\\n <annotation> $n\\\\times q$</annotation>\\n </semantics></math> equations in terms of <math>\\n <semantics>\\n <mrow>\\n <mi>n</mi>\\n <mo>×</mo>\\n <mi>q</mi>\\n </mrow>\\n <annotation> $n\\\\times q$</annotation>\\n </semantics></math> unknown coefficients described in step 2. Solving this system of equations, the solution for <math>\\n <semantics>\\n <mrow>\\n <mover>\\n <mi>y</mi>\\n <mo>‾</mo>\\n </mover>\\n <mrow>\\n <mo>(</mo>\\n <mi>t</mi>\\n <mo>)</mo>\\n </mrow>\\n </mrow>\\n <annotation> $\\\\overline{y}(t)$</annotation>\\n </semantics></math> in one period is obtained. (5) Finally, using the linearity and differentiation properties of the system and the coefficients of the input side of the differential equation of the system, the total response, <math>\\n <semantics>\\n <mrow>\\n <mi>y</mi>\\n <mrow>\\n <mo>(</mo>\\n <mi>t</mi>\\n <mo>)</mo>\\n </mrow>\\n </mrow>\\n <annotation> $y(t)$</annotation>\\n </semantics></math>, in one period is constructed in terms of <math>\\n <semantics>\\n <mrow>\\n <mover>\\n <mi>y</mi>\\n <mo>‾</mo>\\n </mover>\\n <mrow>\\n <mo>(</mo>\\n <mi>t</mi>\\n <mo>)</mo>\\n </mrow>\\n </mrow>\\n <annotation> $\\\\overline{y}(t)$</annotation>\\n </semantics></math> and its derivatives. For stable LTI systems, the proposed method can be used without any limitations.</p>\",\"PeriodicalId\":50386,\"journal\":{\"name\":\"Iet Circuits Devices & Systems\",\"volume\":\"17 2\",\"pages\":\"88-94\"},\"PeriodicalIF\":1.0000,\"publicationDate\":\"2023-01-04\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://onlinelibrary.wiley.com/doi/epdf/10.1049/cds2.12142\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Iet Circuits Devices & Systems\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1049/cds2.12142\",\"RegionNum\":4,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q4\",\"JCRName\":\"ENGINEERING, ELECTRICAL & ELECTRONIC\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Iet Circuits Devices & Systems","FirstCategoryId":"5","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1049/cds2.12142","RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
引用次数: 0
摘要
提出了一种求解具有任意周期输入信号的线性时不变(LTI)系统时域闭合解的新方法。与基于传统傅立叶相量方法获得的解不同,这些解在一个周期内具有有限数量的项。为了实现所提出的方法,执行了以下步骤:(1)对于由传递函数、脉冲响应、框图等表示的给定系统,与系统输出相关的控制微分方程,y(t)$y(t,x(t)$x(t。(2) 一个辅助微分方程是通过简单地用y代替y(t)$y(t)$而形成的‾(t)$\覆盖{y}(t)$并将输入侧等同于x(t)仅$x(t)$。在一个周期内为输入信号的每个时间段求解辅助微分方程,留下与齐次解相关的常数系数作为未知数。对于输入信号在一个周期内由q个分段组成的n阶系统,存在n×q$n×q$这样的未知系数。(3) y‾(t)$\overline{y}(t)$及其导数的连续性,d k y‾(t)/dtk,${d}^{k}\覆盖线{y}(t)/d{t}^{k},$k=1,‧‧‧,n−1,$k=1,\cdot\cdot\cbot,n-1,$在连续段的连接点处,并且实现了周期的起点和终点的周期性条件。(4) 步骤3的结果是根据n×q$n\times q$未知的n×q$n\times q$方程组步骤2中描述的系数。求解该方程组,得到了y‾(t)$\overline{y}(t)$在一个周期内的解。
A new method for calculation of closed-form response of linear time-invariant systems to periodic input signals
A new method for finding closed-form time-domain solutions of linear time-invariant (LTI) systems with arbitrary periodic input signals is presented. These solutions, unlike those obtained based on the conventional Fourier-phasor method, have a finite number of terms in one period. To implement the proposed method, the following steps are carried out: (1) For a given system, represented by a transfer function, an impulse response, a block diagram etc., the governing differential equation relating the output of the system, , to its input, , is obtained. (2) An auxiliary differential equation is formed by simply replacing with and equating the input side to alone. The auxiliary differential equation is solved for each time segment of the input signal in one period, leaving the constant coefficients associated with the homogeneous solutions as unknowns. For an nth-order system with an input signal consisting of q segments in one period, there are such unknown coefficients. (3) Continuity of and its derivatives, at the connection points of successive segments and the periodicity conditions for the beginning and end points of the period are implemented. (4) The outcome of step 3 is a system of equations in terms of unknown coefficients described in step 2. Solving this system of equations, the solution for in one period is obtained. (5) Finally, using the linearity and differentiation properties of the system and the coefficients of the input side of the differential equation of the system, the total response, , in one period is constructed in terms of and its derivatives. For stable LTI systems, the proposed method can be used without any limitations.
期刊介绍:
IET Circuits, Devices & Systems covers the following topics:
Circuit theory and design, circuit analysis and simulation, computer aided design
Filters (analogue and switched capacitor)
Circuit implementations, cells and architectures for integration including VLSI
Testability, fault tolerant design, minimisation of circuits and CAD for VLSI
Novel or improved electronic devices for both traditional and emerging technologies including nanoelectronics and MEMs
Device and process characterisation, device parameter extraction schemes
Mathematics of circuits and systems theory
Test and measurement techniques involving electronic circuits, circuits for industrial applications, sensors and transducers