LAPLACE
TRANSFORMS
CHAPTER 2
, Laplace transforms are not only
easy
to manipulate
SPECIAL FUNCTIONS they also allow us to deal with discontinuous functions
-
{ Unit Step function } I Heaviside function )
0 too
UH )
{
Htt ) a
-
= -
,
t > O
fit ) Htt ) =
B
t
Ht ) t > O
,
I ;
Hit as
aa
=
? is
-
gg#¥t¥÷
soda
inn "
.
: "
activates at a
HHHH al
{ He
-
i
-
,
: tfaa at
me
Consider Htt -
at -
Htt -
b ) where oaaab
activates then
deactivates
at
}
{ I Ibb to
Hit at Htt )
tatM←t
-
-
-
b =
fail )
IIb
at
Htt as Htt b '
-
{ hots to
- - -
-
t
, Examples
fit
{
It ) =
Et<
i<t< 2
1
0
t Z 2
Express ftt ) In terms of the Heaviside function :
fly =
fit ) [ Hlt -
a) -
HH -
b ) ]
=
t [ Hlt -
o ) -
HH -
i )] + 12 .
⇒ [ HCH ) -
Hlt -2 ) ]
=
THH ) -
t Hlt -
i ) + ZHH -
i ) -
ZH ( t 2) . -
THH -
l ) + THH -
2)
THH ) zlt
HIT
i ) I ) I t 2) H It 2)
=
-
- -
+ - -
=
. .
=
¥waut it in this farm ... we 'll see
why
letter
TRANSFORMS
CHAPTER 2
, Laplace transforms are not only
easy
to manipulate
SPECIAL FUNCTIONS they also allow us to deal with discontinuous functions
-
{ Unit Step function } I Heaviside function )
0 too
UH )
{
Htt ) a
-
= -
,
t > O
fit ) Htt ) =
B
t
Ht ) t > O
,
I ;
Hit as
aa
=
? is
-
gg#¥t¥÷
soda
inn "
.
: "
activates at a
HHHH al
{ He
-
i
-
,
: tfaa at
me
Consider Htt -
at -
Htt -
b ) where oaaab
activates then
deactivates
at
}
{ I Ibb to
Hit at Htt )
tatM←t
-
-
-
b =
fail )
IIb
at
Htt as Htt b '
-
{ hots to
- - -
-
t
, Examples
fit
{
It ) =
Et<
i<t< 2
1
0
t Z 2
Express ftt ) In terms of the Heaviside function :
fly =
fit ) [ Hlt -
a) -
HH -
b ) ]
=
t [ Hlt -
o ) -
HH -
i )] + 12 .
⇒ [ HCH ) -
Hlt -2 ) ]
=
THH ) -
t Hlt -
i ) + ZHH -
i ) -
ZH ( t 2) . -
THH -
l ) + THH -
2)
THH ) zlt
HIT
i ) I ) I t 2) H It 2)
=
-
- -
+ - -
=
. .
=
¥waut it in this farm ... we 'll see
why
letter