By L Dresner

ISBN-10: 0750305312

ISBN-13: 9780750305310

Lie's team conception of differential equations unifies the various advert hoc equipment recognized for fixing differential equations and gives strong new how one can locate suggestions. the speculation has functions to either usual and partial differential equations and isn't constrained to linear equations. purposes of Lie's concept of normal and Partial Differential Equations offers a concise, easy creation to the applying of Lie's concept to the answer of differential equations. the writer emphasizes readability and immediacy of knowing instead of encyclopedic completeness, rigor, and generality. this permits readers to fast seize the necessities and begin making use of the the right way to locate recommendations. The ebook comprises labored examples and difficulties from quite a lot of clinical and engineering fields.

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**Extra resources for Applications of Lie’s Theory of Ordinary and Partial Differential Equations**

**Sample text**

5 focused on problems on the semiinfinite interval (0, oo ). 1) known as the Poisson-Boltzmann equation, provides an example of a problem on a finite interval in which the group is not a stretching group. g. Na+ ions) inside a solventfilled cavity with walls charged oppositely to the charge of the mobile ions. The value of v is 0, 1 or 2 according to whether the cavity is the slit between two charged planes perpendicular to the x-direction, the interior of a cylinder of which x is the radial coordinate, or the interior of a sphere of which x is the radial coordinate, respectively.

An envelope, if it exists, is thus invariant to all the groups that leave the differential equation invariant. 5 Change of Variables Lie proposed a second method of solving first-order differential equations that are invariant to a group, which involves using the group to find new variables ~(x,y) and y(x,y), in terms of which the differential equation becomes separable. 2b)

Consider a particular solution S belonging to a fixed value of a. 3. 7b) These images all lie on a single vertical line at x' = c. The image point (x', y') also lies on the curve belonging to the initial value 42 Second-Order Ordinary Differential Equations a' = (clx)Pa. Thus as x ~ oo, a' ~ oo (remember f3 < 0). This means as the point (x, y) moves out along the solution S toward x = oo, the image point (x', y') moves steadily upwards along the vertical line x' = c. 8) which completes the proof.

### Applications of Lie’s Theory of Ordinary and Partial Differential Equations by L Dresner

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