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Mathematical Methods for Physicists: A concise introduction - Site Map

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LAPLACE TRANSFORMS OF ELEMENTARY FUNCTIONS<br />

Solution:<br />

We have to check whether or not<br />

<br />

lim<br />

x!1 ebx x 3 x 3<br />

ˆ lim<br />

x!1 e bx<br />

exists. Now if b > 0, then L'Hospital's rule gives<br />

<br />

lim<br />

x!1 ebx x 3 ˆ lim<br />

x!1<br />

x 3<br />

There<strong>for</strong>e x 3 is of exponential order as x !1.<br />

3x 2 6x 6<br />

ˆ lim ˆ lim<br />

bx<br />

e x!1 bx<br />

be x!1 b 2 ˆ lim<br />

bx<br />

e x!1 b 3 ˆ 0:<br />

bx<br />

e<br />

Laplace trans<strong>for</strong>ms of some elementary functions<br />

Using the de®nition (9.1) we now obtain the trans<strong>for</strong>ms of polynomials, exponential<br />

and trigonometric functions.<br />

(1) f …x† ˆ1 <strong>for</strong> x > 0.<br />

By de®nition, we have<br />

L‰1Š ˆ<br />

Z 1<br />

(2) f …x† ˆx n , where n is a positive integer.<br />

By de®nition, we have<br />

0<br />

e px dx ˆ 1<br />

p ; p > 0:<br />

Using integration by parts:<br />

Z<br />

L‰x n Šˆ<br />

Z 1<br />

0<br />

Z<br />

uv 0 dx ˆ uv <br />

e px x n dx:<br />

vu 0 dx<br />

with<br />

u ˆ x n ; dv ˆ v 0 dx ˆ e px dx ˆ…1=p†d…e px †; v ˆ…1=p†e px ;<br />

we obtain<br />

Z 1<br />

0<br />

<br />

e px x n dx ˆ xn e px<br />

p<br />

1<br />

0<br />

‡ n p<br />

Z 1<br />

0<br />

e px x n1 dx:<br />

For p > 0 and n > 0, the ®rst term on the right hand side of the above equation is<br />

zero, and so we have<br />

Z 1<br />

0<br />

e px x n dx ˆ n<br />

p<br />

375<br />

Z 1<br />

0<br />

e px x n1 dx

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