engeeniring math1 note
Post on 13-Sep-2015
234 views
DESCRIPTION
engeeniring Math1 NoteTRANSCRIPT
-
2 2 - 36 -
2.9 (method of undetermined coefficients) , , , , ,
( )xr
(1) ( )xrbyyay =++ (A) (basic rule) (1) 2.1 , , (1) .
( )xrpy py
(B) (modification rule) (1) ,
py
py x ( ) . 2x
(C) (sum rule) 2.1 , .
( )xrpy
2.1
( )xr py xx Ceke
kx ( ) 0111,1,0 KxKxKxKn nnnnn ++++= "" xMxK
xkxk
sincos
sincos
+
( )xMxKexkexke x
x
x
sincossincos
+
-
2 2 - 37 -
1 (A) 284 xyy =+ i2404 22 ===+ xBxAyh 2sin2cos +=
0122 KxKxKyp ++= 122 KxKyp +=
22Kyp =
( ) 201222 8424 xKxKxKKyy pp =+++=+ 4 042048 0212 =+== KKKK 102 012 === KKK
122sin2cos 2 ++=+= xxBxAyyy ph
2 (B) xeyyy =+ 23 ( )( ) 2,1021232 ===+ xxh ececy 221 +=
xp Cxey = xxp CxeCey += xxx
p CxeCeCey ++=
( ) xxxxxxppp eCxeCxeCeCxeCeyyy =+++=+ 23223 1=C
xxxph xeececyyy +=+= 221
3 (B) ( ) ( ) 10,10,2 ===++ yyeyyy x ( ) 10112 22 ==+=++
( ) xh exccy += 21
xp eCxy = 2 xxp eCxCxey = 22
xxxxp eCxCxeCxeCey += 2222
( ) xxxxxxxppp eeCxeCxCxeeCxCxeCeyyy =+++=++ 222 22422
-
2 2
- 38 -
2112 == CC
( ) xxph exexccyyy ++=+= 221 21 ( ) 10 1 == cy
( ) xxxx exxeexccecy ++= 2212 21
( ) 010 212 === cccy xxx exexey
=+= 121
21 22
4 (C) ( ) ( ) 1.600,2.00,4sin554cos4025.152 5.0 ==+=++ yyxxeyyy x ( ) ii 212104152 22 ==+=++=++ ( )xBxAey xh 2sin2cos += xMxKCey xp 4sin4cos5.0 ++= xMxKCey xp 4cos44sin45.0 5.0 +=
xMxKCey xp 4sin164cos1625.0 5.0 =
( ) ( )
xxexKMxKMCexMxKCexKxMCe
xMxKCeyyy
x
x
x
x
xppp
4sin554cos4025.14sin8114cos11825.64sin54cos554sin84cos8
4sin164cos1625.052
5.0
5.0
5.0
5.0
5.0
+=
++=
+++
++
=++
2.025.125.6 == CC 40118 = KM 0=K 55811 = KM 5=M
( ) xexBxAeyyy xxph 4sin52.02sin2cos 5.0 +++=+=
( ) 02.02.00 ==+= AAyxexBey xx 4sin52.02sin 5.0 ++=
xBexBey xx 02cos22sin ++= xe x 4cos201. 5.0 +( ) 201.60201.020 ==++= BBy
xexey xx 4sin52.02sin20 5.0 ++=
-
2 2
- 39 -
2.11 : , - (1) m 0=++ kyycy ( )trkyycym =++ , : (input), (driving force) ( )tr : (output), (response) ( )ty (2) tFkyycym cos0=++ ( )0,00 >> F (3) ( ) tbtatyp sincos += ( ) tbtatyp cossin +=
( ) tbtatyp sincos 22 = (2)
( ){ } ( ){ } tFtbmkcatcbamktkbtkatactbc
tbmtamkycymy ppp
cossincossincossincos
sincos
022
22
=+++=
++
+
=++
(4) ( ) ( ) 020
2
=+
=+
bmkcaFcbamk
Cramer rule
( )( ) 2222
20
2
2
20
0cmk
mkF
mkccmk
mkcF
a
+
=
=
-
2 2
- 40 -
( ) 222202
2
02
0
cmkcF
mkccmk
cFmk
b
+=
=
2.5 ( )00 >=mk
(5) ( )( ) 222220222
00
cm
mFa
+
= , ( ) 22222020
cm
cFb
+=
(2) (6) ( ) ( ) ( )tytyty ph += 1. . 0=c
mk=2 02
(3) (5)
(7) ( ) ( ) tk
Ft
mkm
Ftm
Ftyp
cos
1
cos
1
cos2
0
02
0
022
0
0
=
=
=
2.5 (4*) (p.88) (8) ( ) ( ) ( ) tm FtCty coscos 220 00 +=
(natural frequency)
20
2
-
2 2
- 41 -
(7) py
(9) kFa 00 = 2
0
1
1
=
(resonance) 0 =
(resonance factor) 57 , (2)
tmFy
mky 00 cos=+
(10) tmFyy 00
20 cos =+
tBtAyh 00 sincos +=
( )tbtatyp 00 sincos +=
( )tbtattbtayp 000000 cossinsincos +++=
( )tbtattbtatbtayp
02
002
0
00000000
sincos
cossincossin
+
++=
( )( )
tmFtbta
tbtat
tbtattbtayy pp
00
0000
02
002
0
02
002
000002
0
coscos2sin2
sincos
sincoscos2sin2
=+=
++
++=+
0
0
2,0
mFba ==
(11) ttmFyp 0
0
0 sin2
= 58
-
2 2
- 42 -
0
) ( ) ( ) 00,00 == yy ( ) ( ) tm FtBtAty cossincos 220 000 ++= ( ) ( ) ( )220 0220 0 00 ==+= m
FAm
FAy
( ) ( ) tm FtBtAty sincossin 220 00000 += ( ) 000 0 === BBy
(12) ( ) ( )( ) ( 00220 0 coscos = ttmFty )
BABABABABABA
sinsincoscos)cos(sinsincoscos)cos(
=+
+=
BABABA sinsin2)cos()cos( =+
22abBbaAbBA
aBA
=
+==+
=
2sin
2sin2coscos abbaba +=
( ) ( )
+
= ttm
Fty2
sin2
sin2 00220
0
59
-
2 2
- 43 -
2.
0>c
( ) ( ) ( )tth ececty + += 21 024
02
2
>
=>=mmkc
mc
t ( ) ( )h etccty += 21 ( ) ( )tBtAety th ** sincos += ( )042
42
22* >=
=
mc
mk
mcmk
ph yyy += (transient solution)
py (steady-state solution)
( )
py
(3) (13) ( ) ( ) = tCtyp cos*
( ) ( )( ) ( )( )( ){ } ( ) ( ) 2222202 02222202
20
222222
02
2220
2220
220
2
222220
2
0
2
222220
2
220022*
cm
F
cm
F
cm
cFmF
cm
cF
cm
mFbaC
+=
+=
+
+=
++
+
=+=
( )220tan
==
mc
ab
( ) 0* =
ddC , ,
0)(2 22202
=+ cm
2
2
2
2
2
22
02
22
22
2 mcmk
mcmk
mc
=
== (14) (16)
1,1 == km , () 60
-
5 - 44 -
5 Laplace (3) 1 : () 2 : 3 : sine cosine
5.1 Laplace, , ,
( )f t : t 0 ( ) ( )F s e f t dtst= 0 ( )F s : Laplace(Laplace transform) ( )f t ( )f (1) ( ) =sF ( ) ( ) = 0 dttfef st Laplace(Laplace transformation) ( )f t ( )F s (inverse transform) , ( )f t ( )F s ( )1 F =( )f t ( )1 F
-
5 - 47 -
Laplace 5.1
5.1 , .
5.1 Laplace ( )f t ( )f ( )f t ( )f ( )f t ( )f
( )( )
( )( )( ) 22
221
221
2232
222
22
sin1216
cos111positive
5
sinh10!,2,1,0
4
cosh9!23
sin812
cos7111
+
+
+=
+
+
+
+
ast
ase
asast
sa
at
asaat
sn
nt
assat
st
st
st
sst
s
at
a
a
n
n
5.9 .
(1), (2), (3) (4) . (4) . 1 0 . n = 0 1! = . n
( ) ( )t e t dt s e t s n e t dt n s e t dtn st n st n st n st+ +
+
= =
+ =
+ 1 10 10
0 0
1 1 1 1 n ( ) ( )t n s ns
ns
nn n
+
+ +=
+=
+11 2
1 1! !
(4) (5) ( ) n + =1 n! (, n ) .
-
5 - 57 -
5.3 Unit Step, Delta Functions
: sL ( s) -
3 : Y(s) Y(s) y(t)
- (Heaviside ) u ( t-a) - ( 110, 111)
u ( t-a)= { 0 t
-
5 - 58 -
f ( t-a)u( t-a)=L-1{e-asF(s)} (3*)
e-asF(s)= e-as
0e - s f ()d=
0e - s (+ a)f ()d
+a= t = t-a, d=dt, =0 t=a
e-asF(s)=
ae- stf ( t-a)dt=
0e- stf ( t-a)u( t-a)dt
( )
L{u ( t-a)}=
0e- stu ( t-a)dt
=a
0e- st0dt+
ae- st1dt=- 1s e
- st |
a= e
-as
s (s> 0)
a = 0 ,
L{u ( t)}= 1s
( u(t-a) = 1u(t-a), y(t)=1 )
1. 1 ,
f ( t)= { 2 (0< t< )0 (< t< 2)sin t ( t> 2) , F(s)=?f ( t) =2u ( t)-2u ( t-)+u ( t-2)sin t
=2u ( t)-2u ( t-)+u ( t-2)sin ( t-2)
F(s)= 2s -2e - s
s +e -2s
s 2+1
-
5 - 59 -
2. 1 ,
F(s)= 2s 2
- 2e-2s
s 2- 4e
-2s
s +se -s
s 2+1
L-1( 1s 2
)= t, L-1( e-2s
s 2)=( t-2)u ( t-2)
L-1( e-2s
s )=u ( t-2), L-1(e-s s
s 2+1)= cos ( t-)u ( t-)
f ( t) =2t-2( t-2) u ( t-2)-4 u ( t-2)+ cos ( t-) u ( t-)=2t-2t u ( t-2)- cos t u ( t-)
f ( t)= { 2t (0< t< t)0 (2< t< )- cos t ( t> ) , Dirac
- ( ) * * * hard landing*
- f(t) a ta+k (impulse) * a ta+k f(t) * : k ( zero)
(5) f k ( t-a)= { 1/k ata+k0 otherwise ( 117), I k
(6) I k=
0f k(t-a)dt=
a+ k
a
1k dt=1
-
5 - 60 -
- f k(t-a)
f k ( t-a)=1k [u( t-a)-u( t-a-k)]
- f k(t-a)
L{f k ( t-a)}=1ks [e
-as-e -(a+k) s]= e-as 1-e- ks
ks
- Dirac Delta
( t-a)= limk0
f k(t-a)= { t=a0 ta ,
0( t-a)dt=1
- Dirac Delta
L{( t-a)}= limk0
e-as 1-e- ks
ks = e-as ( )
L{( t)}=1
4 - y''+3y'+2y= r( t), y(0)=0, y'(0)=0, r( t)=( t-1),
s 2Y+3sY+2Y= e- s, Y=F(s)e- s
F(s)= 1(s+2)(s+1) =1
s+1 -1
s+2
f ( t)=L-1(F(s))= e- t-e-2t
y( t)=L-1(F(s) e- s )= f ( t-1)u ( t-1)
y ( t)={ 0 (0t< 1)e-( t-1)-e-2( t-1) ( t> 1)
-
5 - 61 -
5.4 Differentation and Integration( )
F(s)
F(s)=L(f)=
0e- stf ( t) dt
F(s) s
F'(s)= dFds =-
0e- stt f ( t) dt
L{ t f ( t) }=-F '(s) or L-1{F '(s)}= t f ( t)
1
L{ f ( t)t }=
sF( s)ds, L-1{
sF( s)ds }= f ( t)t
()
sF( s)ds=
s [
0e - s
tf ( t)dt ] ds
=
0 [
sf ( t) e - s
td s ] dt=
0f ( t) [
se - s
td s ] dt
se - s
td s=- 1t [e- s t]s = 1t e
- s t
sF( s)ds=
0e - st f ( t)t dt
-
5 - 62 -
Ex 2. F(s)= ln (1+ 2
s 2 ), f ( t)=?,
G(s) =F'( s)= 11+2/s 2
(-2) 2
s 3=- 2
2
s(s 2+2)=- 2s +
2ss 2+2
g( t)=L-1{G(s)}=-2+2cost
g( t)=L-1{G(s)}=L-1{F '(s)}=- tf ( t)
f ( t)= 2t (1- cost)
(7) L(t y ')=- dds [sY(s)-y(0)]=-Y(s) - sdY(s)ds
(8) L(t y '')=- dds [ s2Y(s)- sy(0)-y'(0)]=-2sY(s) - s 2 dY(s)ds +y(0)
5.5 (Convolution)
L-1{F(s)}= f( t), L-1{G(s)}=g( t) , H(s)=F(s) G(s) f( t) g( t) , h( t)= (f*g)( t) , f g (convolution) .
- ( convolution )h( t)= (f*g)( t) = f( t)*g( t)
= t
0f(t-)g()d =
t
0f()g( t-)d
-
5 - 63 -
1. H(s)= 1(s 2+1)2
h( t)=?,
H( s)= 1(s 2+1)2
= 1s 2+1
1s 2+1
=F( s)G(s),
f ( t)=g( t)= sin t
h( t)= f ( t)*g( t)=t
0sin ()sin ( t-)d
sin ()sin ( t-)= 12 [- cos t+ cos (2- t)],
h( t)= 12
t
0[- cos t+ cos (2- t)]d=- 12 tcos t+
12 sin t
2. H(s)= 1s 3
h( t)=?
H(s)= 1s 1s 2
=F(s)G(s)
f( t)=1, g( t)= t ,
h( t)= f ( t)*g( t)=t
01( t-)d= [ t- 12 2] t0 = t
2
2
3. H(s)= 1s 2(s-a )
h( t)=?,
H(s)== 1s 2
1s-a =F(s)G(s)
, f ( t)= t, g( t)= eat
h( t)= f ( t)*g( t)=t
0e a( t-)d= eat
t
0e -ad= 1
a 2(eat-at-1)
- ( t)
t
0( t-) f()d = f( t) *f= f* = f
, 1*f f ( t) ( (0)=),
-
5 - 64 -
(2) y''+ay'+by= r( t)
, (s 2+as+b)Y( s)= (s+a)y(0)+y'(0)+R( s) (3) Y(s)= [ (s+a)y(0)+y'(0)]Q(s)+R(s)Q (s), Q( s)= 1
s 2+as+b
y(0) = y'(0) = 0 , Y(s)=R( s)Q(s)
y( t) ,
(4) y( t) = r(t)*q( t) = t
0r() q( t-) d =
t
0q() r ( t-) d
4. 5.3 4
y''+3y'+2y= r( t), y(0)=0, y'(0)=0
r( t)=
0, 0< t< 11, 1< t< 20, 2< t
,
Q( s) = 1s 2+3s+2
= 1(s+1)(s+2) = 1
s+1 -1
s+2
q( t)=e- t-e-2t
t < 1 , r( t) = 0 y( t) = r(t)*q( t) = 0*q( t) = 0
1 < t < 2 , r( t) = 1
y( t) = r(t)*q( t) = t
0r() q( t-) d =
1
0r() q ( t-) d +
t
1r() q ( t-) d
-
5 - 65 -
= 0 + t
11 q ( t-) d
= t
1(e-( t-)-e-2( t-)) d
= [e-( t-)- 12 e-2( t-)]= t
=1
= ( (1- 12 ) - (e-( t-1) - 12 e-2( t-1))= 12 - e
-( t-1) + 12 e-2( t-1)
2 < t ,
y( t) = r(t)*q( t) = t
0r() q( t-) d
= 1
0r() q ( t-) d +
2
1r() q ( t-) d+
t
2r() q ( t-) d
= 0 + 2
11 q ( t-) d + 0
= 2
1(e-( t-)-e-2( t-)) d
= [e-( t-)- 12 e-2( t-)]= 2
=1
= ( (e-( t-2) - 12 e-2( t-2)) - (e-( t-1) - 12 e-2( t-1)))= e-( t-2) - e-( t-1) - 12 [e
-2( t-2)) - e-2( t-1))]
5.
y( t) = t+t
0y() sin ( t-)d
1 : y( t)= t+y * sin t 2 :
Y(s) = 1s 2
+Y(s) 1s 2+1
Y(s)= s2+1s 4
= 1s 2
+ 1s 4
3 :
y(t) = t+ 16 t3
-
5 - 66 -
5.6 (Partial Fraction),
-
Y(s)= F(s)G(s)
G(s)
Case I. : G(s)= s-a ( )
Ex 1. y''+y'-6y=1, y(0)=0, y'(0)=1
s 2Y-sy(0)-y'(0)+sY-y(0)-6Y= 1s
(s 2+s-6)Y=1+ 1s
Y( s)= s+1s( s-2)( s+3) =A 1s +
A 2s-2 +
A 3s+3
A 1, A 2, A 3=?
s+1=A 1( s-2)(s+3)+A 2s(s+3)+A 3s(s-2)
s=0 1=A 1(-2)(3), A 1=-1/6
s=2 3=A 225, A 2=3/10
s=-3 -2=A 3(-3) (-5), A3=-2/15
y(t) =- 16 +310 e
2t- 215 e-3t
Case II. : G(s) = (s-a)m ( )
e.g.) G( s)= ( s-a) 3 A 1(s-a) + A 2
(s-a) 2 +
A 3(s-a) 3
-
5 - 67 -
Ex 2. y''-3y'+2y=4t, y(0)=1, y'(0)=-1
s 2Y-sy(0)-y'(0)-3sY+3y(0)+2Y= 4s 2
(s 2-3 s+2)Y= 4s 2
+s-4= 4-s3-4s 2
s 2
Y= 4+ s3-4s 2
s 2(s-1) ( s-2)=
A 1s 2
+A 2s +
A 3s-1 +
A 4s-2
A 1, A 2, A 3, A 4=?
4+ s 3-4s 2=A 1(s-1) ( s-2)+A 2s( s-1) ( s-2)+A 3s 2(s-2)+A 4s 2(s-1)
s=1 1=+A 3(1) (-1), A 3=-1
s=2 -4=+A 441, A 4=-1
s=0 4=A 1(-1) (-2), A 1=2
3s 2-8s=A 1(2s-3)+A 2(s-1) ( s-2)+ s(k( s))
s=0 0=A 1(-3)+A 2(-1) (-2)=-6+2A 2, A 2=3
y(t) =2t+3-e 2t-e t
Case III. : G(s)= ( s-a)(a- a) () ( a=+ i, a=- i )
e.g.) As+B(s-a) (s- a)
or As+B(s-)2+2
-
5 - 68 -
Ex 3. y''+2y'+2y= r( t), y(0)=1, y'(0)=-5 , r( t)=10 sin 2t [1-u( t-)] = 10 sin 2t -10 u( t-)sin 2( t-)
,
[s 2Y(s)-sy(0)-y'(0)]+2[Y( s)-y(0)]+2Y (s)=10 2s 2+4
(1-e-s )
(s 2+2s+2)Y(s) = sy(0)+y'(0)+2y(0)+10 2s 2+4
(1-e-s )
= s-5+2+10 2s 2+4
(1-e-s)
= s-3+ 20s 2+4
- 20e-s
s 2+4
Y( s) = s-3s 2+2s+2
+ 20( s 2+4)( s 2+2s+2)
- 20e-s
(s 2+4)( s 2+2s+2)
L-1{ s-3s 2+2s+2 }=L-1{ (s+1)-4(s+1)2+1 } =L-1{ ss+1 } s s+1- 4L-1{ 1s+1 } s s+1
=e- t cost - 4e- tsint
L-1{ 20(s 2+4)(s 2+2s+2) }= As+Bs 2+4 + Cs+Ds 2+2s+2
(As+B)(s 2+2s+2) = (Cs+D)( s 2+4)
s 3, s 2, s 1, s 0 A=-2, B=-2, C=2, D=6
L-1{ 20(s 2+4)(s 2+2s+2) } =L-1{ -2s-2s 2+4 + 2s+6s 2+2s+2 }
=-2L-1{ ss 2+4 }-L-1{ 2s 2+4 }+L-1{ 2(s+1)+4(s+1)2+1 }
=-2 cos2t- sin2t+L-1{2 ss 2+1 +4 1s 2+1 } s s+1=-2 cos2t-sin2t+e- t(2cos t+4sin t)
-
5 - 69 -
-L-1{ 20e-s
(s 2+4)(s 2+2s+2) } = -[-2 cos2( t-)- sin2( t-) +e-( t-) (2cos ( t-)+4sin ( t-)) ] u( t-)
= -[-2 cos2t- sin2t+e-( t-)(-2 cos t-4 sin t)]
= [2cos2t + sin2t + e-( t-)(2 cos t+4 sin t)] u( t-)
y( t) = + + = [e- t cost - 4e- tsint]+[-2 cos2t- sin2t+e- t (2cos t+4sin t)]
+[2cos2t + sin2t + e-( t-)(2 cos t+4 sin t)] u( t-)
= -2 cos2t - sin2t + 3e- tcost
+ [2cos2t + sin2t + e-( t-)(2 cos t+4 sin t)] u( t-)
,
y( t)= { -2 cos2t - sin2t + 3e- tcost , 0< t<
e- t [ (3+2e )cos t+4e sint] , < t
Case IV. : G(s) = [ (s-a)(a- a)] 2 ()
e.g.) As+B[ (s-a) (s- a)] 2
+ As+B(s-a) (s- a)
Ex 3. y''+w 0y = Ksinw 0t, y(0)=0, y'(0)=0
s 2Y(s) + w20Y(s) =Kw 0
s 2+w20
Y( s) = Kw 0(s 2+w20)
2 = Kw 0
w 0s 2+w20
w 0
s 2+w20 = Kw 0
F( s)G( s)
-
5 - 70 -
f( t)= sinw 0t , g( t)= sinw 0t,
y( t)= Kw 0f( t) * g( t) = Kw 0
t
0sinw 0 sinw 0(t-) d
= Kw 0t
0
12 [ cos {w 0-w 0 (t-)}- cos {w 0+w 0 (t-)}]d
= K2w 0 [t
0cos (2w 0 -w 0t) d-
t
0cosw 0t d]
= K2w 0 [ 12w 0 ( sinw 0t+ sinw 0t ) - t cosw 0t ]= K
2w20( sinw 0t - w 0t cosw 0t)