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Published **1966**
by American Elsevier in New York .

Written in English

- Differential equations, Partial.,
- Wave-motion, Theory of.,
- Gas dynamics.,
- Plasticity.

**Edition Notes**

Other titles | Method of characteristics., Characteristics. |

Statement | [by] Michael B. Abbott. |

Classifications | |
---|---|

LC Classifications | QA374 .A2 1966a |

The Physical Object | |

Pagination | ix, 243 p. |

Number of Pages | 243 |

ID Numbers | |

Open Library | OL5984061M |

LC Control Number | 66013527 |

Introduction and Objectives. First‐Order Hyperbolic Equations. Second‐Order Hyperbolic Equations. Applications to Financial Engineering. Systems of Equations. Propagation of Discontinuities. Summary and Conclusions. An introduction to the method of characteristics | M. B Abbott | download | B–OK. Download books for free. Find books. An introduction to the method of characteristics by Michael B. Abbott. Introduction These are notes and worked examples from Abbott's book. This is a good introduction to the method of characteristics. Download Problem Solutions (Part 1 of 1). An Introduction to the Method of Characteristics. By M. B. ABBOTT. Thames and Hudson, pp. £4. 4s. - Volume 27 Issue 2 - C. HunterAuthor: C. Hunter.

The method of matched asymptotic expansions is used to obtain the large-time asymptotic structure of the solution to this problem which exhibits the formation of an expansion wave. “Method of Characteristics” • Basic principle of Methods of Characteristics-- If supersonic flow properties are known at two points in a flow field, -- There is one and only one set of properties compatible* with these at a third point, -- Determined by the intersection of characteristics, or mach waves, from the two original Size: 5MB. This set of equations is known as the set of characteristic equations for (). Once we have found the characteristic curves for (), our plan is to construct a solution of () by forming a surface S as a union of these characteristic curves. Introduction to the method. A ﬁrst order quasilinear equation in 2D is of the form a(x,y,u) u. x + b(x,y,u) u. y = c(x,y,u); () in 3D is of the form a(x,y,z,u) u. x + b(x,y,z,u) u. y + c(x,y,z,u) u. z = d(x,y,z,u). () One can easily generalize this to higher dimensions.

Introduction. The Differential Equations of the Characteristics. Applications. Alternative Form of the Compatibility Equations. Properties of the Characteristic Lines. Weak Discontinuities. The Equations of the Planar Isoentropic Flow in the Hodograph Plane. Weakly Perturbed Two-Dimensional Flow. Mach Lines. The Flow Near a Curved Wall. Flow. Summary This chapter contains sections titled: Introduction and Objectives First‐Order Hyperbolic Equations Second‐Order Hyperbolic Equations Applications to Financial Engineering Systems of . Since ξ=x−at, the solution of the PDE (1a) is simply given by u(x,t)=F(x−at) (5) Indeed, if F has a C1 continuity, it can be easily veriﬁed that u(x,t)=F(x−at)satisﬁes the PDE and the initial condition. The reduction of a PDE to an ODE along its characteristics is called the method of characteristics. Method of characteristics: a special case. I Consider a ﬂrst-order linear homogeneous PDE of the form. a(x;y)ux +b(x;y)uy = 0: In order to solve it, one tries to ﬂnd parametric curves. x = x(s); y = y(s) along which u(x;y) remains Size: 48KB.

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