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Mathematical Methods for Physicists: A concise introduction - Site Map

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APPENDIX 1 PRELIMINARIES<br />

Di€erentiation of integrals<br />

(1) Inde®nite integrals: We ®rst consider di€erentiation of inde®nite integrals. If<br />

f …x;† is an integrable function of x and is a variable parameter, and if<br />

Z<br />

f …x;†dx ˆ G…x;†;<br />

…A1:11†<br />

then we have<br />

@G…x;†=@x ˆ f …x;†:<br />

…A1:12†<br />

Furthermore, if f …x;† is such that<br />

then we obtain<br />

@<br />

@x<br />

@ 2 G…x;†<br />

@x@<br />

<br />

@G…x;†<br />

@<br />

ˆ @<br />

@<br />

ˆ @2 G…x;†<br />

@@x ;<br />

<br />

@G…x;†<br />

@x<br />

ˆ<br />

@f …x;†<br />

@<br />

and integrating gives<br />

Z @f …x;†<br />

@<br />

dx ˆ @G…x;† ; …A1:13†<br />

@<br />

which is valid provided @f …x;†=@ is continuous in x as well as .<br />

(2) De®nite integrals: We now extend the above procedure to de®nite integrals:<br />

I…† ˆ<br />

Z b<br />

a<br />

f …x;†dx;<br />

…A1:14†<br />

where f …x;† is an integrable function of x in the interval a x b, anda and b<br />

are in general continuous and di€erentiable (at least once) functions of . We now<br />

have a relation similar to Eq. (A1.11):<br />

I…† ˆ<br />

Z b<br />

a<br />

f …x;†dx ˆ G…b;†G…a;†<br />

…A1:15†<br />

and, from Eq. (A1.13),<br />

Z b<br />

a<br />

@f …x;†<br />

@<br />

Di€erentiating (A1.15) totally<br />

dI…†<br />

d<br />

ˆ @G…b;†<br />

@b<br />

dx ˆ @G…b;†<br />

@<br />

db<br />

d ‡ @G…b;†<br />

@<br />

534<br />

@G…a;† : …A1:16†<br />

@<br />

@G…a;†<br />

@a<br />

da<br />

d @G…a;† :<br />

@

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