{"title":"关于","authors":"Tom Cain, R. Connolly","doi":"10.4324/9781315696195-11","DOIUrl":null,"url":null,"abstract":"3D-Filmstrip knows how to calculate and display solutions of the initial value problem for first and second order systems of ordinary differential equations (ODE) in one, two, or three dependent variables. Let us recall briefly what this means. We will be dealing with vector-valued functions x of a single real variable t called the “time”. Here x can take values in R, R2, or R3. The problem is to find x from a knowledge of how x0 depends on x and t (in the first order case) or a knowledge of how x00 depends on x, x0, and t (in the second order case). Thus in the first order case the ODE we are trying to solve has the form x0 = f(x, t) and in the second order case it is x00 = f(x, x0, t). In the first order case, the so-called Local Existence Theorem for First Order ODEs tells us that, provided the function f is continuously differentiable, given an “initial time” t0, and an “initial position” x0, then in some sufficiently small interval around t0, there will be a unique solution x(t) to the ODE with x(t0) = x0. There is a similar local existence theorem for second order ODEs (which in fact is an easy consequence of the first order theorem). It says that given an initial time t0, an initial position x0, and an initial velocity v0 then, in some","PeriodicalId":275564,"journal":{"name":"The Poems of Ben Jonson","volume":"15 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2021-10-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":"{\"title\":\"Ode\",\"authors\":\"Tom Cain, R. Connolly\",\"doi\":\"10.4324/9781315696195-11\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"3D-Filmstrip knows how to calculate and display solutions of the initial value problem for first and second order systems of ordinary differential equations (ODE) in one, two, or three dependent variables. Let us recall briefly what this means. We will be dealing with vector-valued functions x of a single real variable t called the “time”. Here x can take values in R, R2, or R3. The problem is to find x from a knowledge of how x0 depends on x and t (in the first order case) or a knowledge of how x00 depends on x, x0, and t (in the second order case). Thus in the first order case the ODE we are trying to solve has the form x0 = f(x, t) and in the second order case it is x00 = f(x, x0, t). In the first order case, the so-called Local Existence Theorem for First Order ODEs tells us that, provided the function f is continuously differentiable, given an “initial time” t0, and an “initial position” x0, then in some sufficiently small interval around t0, there will be a unique solution x(t) to the ODE with x(t0) = x0. There is a similar local existence theorem for second order ODEs (which in fact is an easy consequence of the first order theorem). It says that given an initial time t0, an initial position x0, and an initial velocity v0 then, in some\",\"PeriodicalId\":275564,\"journal\":{\"name\":\"The Poems of Ben Jonson\",\"volume\":\"15 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2021-10-20\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"2\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"The Poems of Ben Jonson\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.4324/9781315696195-11\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"The Poems of Ben Jonson","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.4324/9781315696195-11","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2
摘要
3D-Filmstrip知道如何计算和显示一阶和二阶常微分方程(ODE)在一个,两个或三个因变量中的初值问题的解决方案。让我们简单回顾一下这意味着什么。我们将处理一个实变量t的向量值函数,叫做时间。这里x可以取R, R2或R3中的值。问题是通过已知x0如何依赖于x和t(在一阶情况下)或已知x00如何依赖于x, x0和t(在二阶情况下)来求x。因此在一阶情况下ODE我们试图解决的形式x0 = f (x, t)和二阶情况下x00 = f (x, x0, t)在一阶的情况下,一阶常微分方程的所谓的地方存在性定理告诉我们,提供了f是连续可微的函数,给定一个初始时间“t0,和一个“初始位置”x0,然后在t0一些足够小的时间间隔,会有唯一解x (t)和x (t0) = x0 ODE。二阶ode有一个类似的局部存在定理(实际上是一阶定理的一个简单推论)。它说给定初始时间为,初始位置为,初始速度为
3D-Filmstrip knows how to calculate and display solutions of the initial value problem for first and second order systems of ordinary differential equations (ODE) in one, two, or three dependent variables. Let us recall briefly what this means. We will be dealing with vector-valued functions x of a single real variable t called the “time”. Here x can take values in R, R2, or R3. The problem is to find x from a knowledge of how x0 depends on x and t (in the first order case) or a knowledge of how x00 depends on x, x0, and t (in the second order case). Thus in the first order case the ODE we are trying to solve has the form x0 = f(x, t) and in the second order case it is x00 = f(x, x0, t). In the first order case, the so-called Local Existence Theorem for First Order ODEs tells us that, provided the function f is continuously differentiable, given an “initial time” t0, and an “initial position” x0, then in some sufficiently small interval around t0, there will be a unique solution x(t) to the ODE with x(t0) = x0. There is a similar local existence theorem for second order ODEs (which in fact is an easy consequence of the first order theorem). It says that given an initial time t0, an initial position x0, and an initial velocity v0 then, in some