Laplace Transforms and Their Applications to Differential Equations
eBook - ePub

Laplace Transforms and Their Applications to Differential Equations

  1. 240 pages
  2. English
  3. ePUB (mobile friendly)
  4. Available on iOS & Android
eBook - ePub

Laplace Transforms and Their Applications to Differential Equations

About this book

This introduction to modern operational calculus offers a classic exposition of Laplace transform theory and its application to the solution of ordinary and partial differential equations. The treatment is addressed to graduate students in engineering, physics, and applied mathematics and may be used as a primary text or supplementary reading.
Chief topics include the theorems or rules of the operational calculus, evaluation of integrals and establishment of mathematical relationships, derivation of Laplace transforms of various functions, the Laplace transform for a finite interval, and other subjects. Many problems and illustrative examples appear throughout the book, which is further augmented by helpful Appendixes.

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Yes, you can access Laplace Transforms and Their Applications to Differential Equations by N.W. McLachlan in PDF and/or ePUB format, as well as other popular books in Mathematics & Differential Equations. We have over one million books available in our catalogue for you to explore.

Information

LAPLACE TRANSFORMS
AND THEIR APPLICATIONS TO DIFFERENTIAL EQUATIONS
THE LAPLACE TRANSFORM
1.11. Definition. Consider the infinite integral
image
p being a suitable parameter, either real or complex, while f(t) is a single-valued* function integrable in every positive interval of t. t is real and
images
0. This integral, but without the external p, was introduced into mathematical analysis by Laplace about the year 1779. ϕ(р), the function obtained by evaluating the integral, we define to be the p-multiplied Laplace Transform of f(t). If ϕ(p) is given, f(t) is said to be its inverse or interpretation in terms of the real variable t. When the range of integration in (1) is t = (0, + ∞), ϕ is a function of p alone. If the range is t = (h1, h2), 0
images
h1, h2, ϕ is a function of p, h1 and h2. We then write
image
the r.h.s. being defined as the p-multiplied L.T. of f(t) for the intervals t = (h1, h2). Integral (2) may be written in the form (1), for if
image
then
image
Integral (1) is a particular case of (2) with h1 = 0 and h2 → + ∞. When p is real and > 0, (1), (2) may be interpreted geometrically as the areas of the exponentially damped function p f(t) between the limits t = (0, + ∞), t = (hl, h2), respectively.
The p-multiplied Laplace transform of a function, as defined by (1), is usually identical with what Heaviside called its operational form,* and the latter nomenclature is used frequently. By way of variation, some writers refer to ϕ(p) as the image of the original function f(t). The most rational terminolo...

Table of contents

  1. Cover
  2. Title Page
  3. Copyright Page
  4. Contents
  5. Prefaces
  6. Symbols
  7. Foreword
  8. chapter
  9. Foreword to Appendices
  10. appendix
  11. Examples to be worked out (with Answers)
  12. Short List of Laplace Transforms (81)
  13. References
  14. Index