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S-FUNCTIONS WITH COMPLICATED ARGUMENTS 109
otherwise. lt dt s ( t ) f ( t )= { i") (5.23)
Remember, by definition, anything that behaves like a 6-function inside an integral is a &function, so S ( - t ) = i3(t). This implies the &function is an even function.
5.3.2 S(at)
Now consider another simple variation 6(at), where a is any positive constant. Again, start with a sifting integral in the form
With a variable change oft' = at, this becomes
so that
otherwise l-'+ dt f(t>&(at)= { L(0)" (5.26)
Notice again, this is just the definition of the function 6 ( t )multiplied by the constant l/a, so
This derivation was made assuming a positive a. The same manipulations can be performed with a negative a, and combined with the previous result, to obtain the more general expression
6(ax) = 6(n)/lal. (5.28)
Notice that our first example, 6 ( t ) = 8 ( - t ) , can be derived from Equation 5.28 by setting a = - 1.
5. 3. 3 S(tZ - 2)
As a bit more complicated argument for the Dirac &function, consider 6(t2 - a L ).
to imply two &functions. To test this theory, place the function in the sifting integral
lr+dt f ( t ) 6 ( t 2- a2). (5.29)
110 THE DIRAC 6-FUNCTION
There can be contributions to this integral only at the zeros of the argument of the 6-function. Assuming that the integral range includes both these zeros, i.e.,
+a+€ dt f ( t ) 6 ( t 2- a2), (5.30) fa-€
NOWt2 - a2 = (t - a)(t + a), which near the two zeros can be approximated by
(t + a)(-2a) (5.31) ( t - a ) ( + k )
t --t -a t2 - a2 = (t - a)(t + a ) = t ---f +a.
about both t = -a and t = +a and keeping terms up to the first order. The Taylor series expansion of t2 - a2 around an arbitrary point to is, to first order, given by
to). (5.32) It=t', In the limit as E -+ 0, Integral 5.30 then becomes -a+€ +a+€
Using the result from the previous section, 6(at) = 6(t)/lal, gives
2a
2a 2a 6(t2 - a2) = - S ( t - a) + -6(t + a),
as shown in Figure 5.12.
6(x2 - a2) 03 00
area = 1/2a
area - = 1/2a
The Plot of S(x2 - a 2 )
**Figure 5. 12**