Title | MKD Skript |
---|---|
Course | Mehrkörperdynamik |
Institution | Karlsruher Institut für Technologie |
Pages | 85 |
File Size | 9.6 MB |
File Type | |
Total Downloads | 46 |
Total Views | 79 |
Institut für Technische Mechanik####### Teilinstitut Dynamik / Mechatronik❙❑❘■P❚▼❊❍❘❑Ö❘P❊❘❉❨◆❆▼■❑Pr♦❢✳❉r✳✲■♥❣✳❲✳❙❡❡♠❛♥♥✕❏✉❧✐✷✵✶✾✕■♥❤❛❧ts✈❡r③❡✐❝❤♥✐s✸✳✹✳✸ ▲❛❣r❛♥❣❡s❝❤❡●❧❡✐❝❤✉♥❣❡♥❜ ❡✐♥✐❝❤t❤♦❧♦♥♦♠❡♥❇✐♥❞✉♥❣❡♥ ✳✳✳✳✳✳✳✳✳✳✳✳✳✳ ✻✸ ✸✳✹✳✹ ▲❛❣r❛♥❣❡s❝❤❡●❧❡✐❝❤✉♥❣❡♥❜ ❡✐❑rä❢t❡♥♠✐t❡✐♥❡♠P♦t❡♥t✐❛❧ ✳✳✳✳✳✳✳✳✳✳✳✳✳✳ ✻✺ ✸✳...
Institut für Technische Mechanik Teilinstitut Dynamik / Mechatronik
R3
x, y, z
r, ϕ, ϑ
~v ~v
q
~v
A
q
A
q
q
B
~ p
O q1 q2 q3
B
P C
A
• ~ p
q1 q2 q3
• ~ p
~ p (q1 )
• ~ p
~ p (q1 , q2 )
• ~ p
~ p (q1 , q2 , q3 )
C
B A D
R3 ~a1 ~a2 ~a3
A
~a1 ~a2 ~a3 R3 ~v
R3
~v = v1~a1 + v2~a2 + v3~a3 ~ai v1 v2 v3 vi~ai
~v
q
A
q ~ai
~a1 ~a2 ~a3 ~ p = α1~a1 + α2~a2 + α3~a3
~v
~a1 ~a2 ~a3 A ~ p
vi
~b1 ~b2 ~b3 b~1 b~2 b~3
~ai
~v
A B
B
~ p = β1b~1 + β2 b~2 + β3b~3 R
~ p
~ p = R(c 1b~2 + s1 b~3 ) c i = cos qi si = sin qi β1 = 0 β2 = Rc 1 β3 = Rs1 . ~ai
~ p
~ai
α1
=~ p · ~a1
α2
=~ p · ~a2
= R(c 1b~2 · ~a1 + s1~b3 · ~a1 ), = R(c 1b~2 · ~a2 + s1~b3 · ~a2 ),
α3
=~ p · ~a3
= R(c 1b~2 · ~a3 + s1~b3 · ~a3 )
~b2 · ~a1 = 0, ~b2 · ~a3 = 0, ~b3 · ~a2 = 0,
α1
=
Rs1 c 2 ,
α2
=
Rc 1 ,
α3
=
Rs1 s2 .
~v
~b2 · ~a2 = 1, ~b3 · ~a1 = cos q2 = c 2 , ~b3 · ~a3 = sin q2 = s2 ,
n
q1 , . . . , qn
A
~v = v1~a1 + v2~a2 + v3~a3
A
B
n 3
A
X ∂vi ∂~v := · a~i , ∂qr ∂qr
r = 1, . . . , n
i=1
~v
A
~v
t A
3 3 X X ~v vi := · a~i = v˙i · a~i t t i=1
~v
t
i=1
A
~ p A
∂~ p ∂q1
=
∂α1 ∂α2 ∂α3 · ~a3 · ~a1 + · ~a2 + ∂q1 ∂q1 ∂q1 R · (c 1 c 2~a1 − s1~a2 + c 1 s2~a3 ),
=
R · (−s1 s2~a1 + s1 c 2~a3 ),
=
~0,
=
A
∂~ p ∂q2 A
∂~ p ∂q3 B
∂~ p ∂q1
=
∂β1 ~ ∂β2 ~ ∂β3 ~ · b1 + · b2 + · b3 ∂q1 ∂q1 ∂q1 R · (−s1 b~2 + c 1 b~3 ),
=
~0,
=
~0.
=
B
∂~ p ∂q2 B
∂~ p ∂q3
qi A
~ p t B ~ p t
=
R · [(c 1 c 2 q˙1 − s1 s2 q˙2 ) · ~a1 − s1 q˙1~a2 + (c 1 s2 q˙1 + s1 c 2 q˙2 ) · ~a3 ]
=
R · [−s1 q˙1 b~2 + c 1 q˙1 b~3 ]
A
b~i
d~ p dt
~a1
s2~b1 + c 2b~3 , ~b2 , −c 2~b1 + s2b~3
=
~a2
=
~a3
=
A
∂~ p ∂q1
=
R · [(c 1 c 2 s2 − c 1 s2 c 2 ) · ~b1 − s1b~2 + (c 1 c 2 c 2 + c 1 s2 s2 ) ·b~3 ]
=
R · [−s1~b2 + c 1~b3 ],
=
−Rs1~b1
=
~0,
=
R · [−s1 q˙2~b1 − s1 q˙1~b2 + c 1 q˙1b~3 ].
A
∂~ p ∂q2 A ∂~ p ∂q3 A
~ p t
~v1
~vN
N N X ∂~vi ∂ X ~vi = ∂qr ∂qr i=1 i=1
q1 r = 1, . . . , n.
s
~v
∂ (s · ~v) ∂qr
∂~v ∂s +s· ∂qr ∂qr
= ~v ·
∂ (~v · w) ~ = ∂qr
w ~·
∂w ~ ∂~v + ~v · ∂qr ∂qr
s
=
s(q1 , . . . , qn ),
~ p
= =
~ p(q1 , . . . , qn ), ~ p·~ p
~ p2
w ~
q1 , . . . , qn r = 1, . . . , n
r = 1, . . . , n.
a = s~ p·~ p
∂ (s · ~ p·~ p) ∂qr
∂~ p ∂~ p ∂s ·~ p+s·~ p· ·~ p·~ p+s· ∂qr ∂qr ∂qr ∂s ∂~ p ·~ p·~ p + 2s · ~ p· ∂qr ∂qr
= =
~ p2 ~ p·
∂~ p =0 ∂qr ∂~ p ∂qr
~ p
B
∂ ∂qs B
t
A
∂~v ∂qr
A
~v t
A
6=
∂ ∂qr A
6=
t
qn
B
∂~v ∂qs
B
~v t
,
r = 1, . . . , n
~v ~v
A
A
~ai
B B
~bi ~v ~v = t~a1 ~a1 = s2b~1 + c 2~b3
~v = t s2~b1 + c 2~b3 . A
B
t
A
~v t B
A
t
B
t
~v t
=
~a1
=
s2b~1 + c 2~b3 ,
=
q˙2 · (c 2~b1 − s2~b3 )
=
−q˙2~a3 ,
~v t
=
s2~b1 + c 2~b3 + tq˙2 (c 2~b1 − s2b~3 )
=
~a1 − tq˙2~a3 ,
=
− (q˙2 + t¨ q2 ) ~a3
B
~v t
A
~v t
A
6=
t
B
~v t
.
q1 , . . . , qn A
~v
n A ~v X A ∂~v ∂~v q˙r + = t ∂t ∂q r r=1 A
~ v t
∂~v ∂ ~v , = ∂qr t t ∂qr
q˙r = ~v
r = 1, . . . , n
t
qr . t
t
∂~v ∂qr
=
∂ ∂q1
=
∂ ∂qr
=
∂ ∂qr
=
∂ ∂qr
∂~v ∂qr ∂~v ∂~v ∂~v ∂~v ∂ ∂ ∂ q˙n + q˙2 + · · · + q˙1 + ∂qr ∂t ∂qr ∂qn ∂qr ∂q2 ∂q1 ∂~v ∂~v ∂~v ∂~v · q˙n + · q˙2 + · · · + · q˙1 + ∂qn ∂q2 ∂q1 ∂t ~v . t
∂~v ∂qr
q˙1 +
∂ ∂q2
∂~v ∂qr
q˙2 + · · · +
∂ ∂qn
∂~v ∂qr
q˙n +
~r ~r =
∂ ∂t
B
E
a1~e1 + a2~e2 + a3~e3 , A1~b1 + A2~b2 + A3~b3
~r =
r∼E
=
r∼B
=
a1 a2 = (a1 , a2 , a3 ) , a3 A1 A2 = (A1 , A2 , A3 ) . A3
~a
~b
a
∼
b∼
a b =b a , ~a · ~b = ∼ ∼ ∼ ∼ = (a1 , a2 , a3 ) a ∼
0 ˜a = a3 ∼ −a2
−a3 a2 0 −a1 a1 0
~c = ~a × ~b a˜∼ c∼ = ∼ b.
~a ˙ = (a˙ 1 , a˙ 2 , a˙ 3 ) . a ∼
a b ∼ ∼ t
˙ b + a b˙ =a ∼ ∼ ∼ ∼
b∼ = (b1 , b2 , b3 )
~c = ~a × ~b ˜a˙ b + a ˜ ˙b. c˙ = ∼ ∼ ∼∼ ∼
~k1
~i1 ~i2 ~i3
~k2 ~k3 ~k1 ~k2
= =
m11~i1 + m12~i2 + m13~i3 , m21~i1 + m22~i2 + m23~i3 ,
~k3
=
m31~i1 + m32~i2 + m33~i3 , mij
~ij
i
mij = ~ki · ~ij . ~ki K
~ij
m11 I m21 = m ∼ m31
m12 m22 m32
mij
m13 m23 m33
~k1 ~i1 ~ K I ~ m . i2 k2 = ∼ ~k3 ~i3
I
K
m ∼
m ¯ 11 ¯ 21 = m m ¯ 31
m ¯ 12 m ¯ 22 m ¯ 32
~km
~il
m ¯ 13 m ¯ 23 , m ¯ 33
m ¯ lm = ~il · ~km
I
K I ) . m = (K m ∼ ∼
I
I −1 K ) m = (K m ∼ ∼
P ∼ · Q| = det(P ) · det(Q ) = |P | · |Q| |P ∼ ∼ ∼ ∼
∼
∼
Q ∼
K I K ( m ) , I∼ = I m ∼ ∼
K 2 )) 1 = (det(I m ∼
K ) = 1. det(I m ∼
B
E
B
~e3 = ~b3
E
ϕ
ϕ
~b1 cos ϕ ~ = − sin ϕ b2 ~b3 0
B
cos ϕ = − sin ϕ m ∼ 0 E
det(B mE ) ∼
B
E E · (B m ) m ∼ ∼
= =
m ∼ r T r∼j = δij , ∼i
r∼j m ∼
j
m ∼
sin ϕ cos ϕ 0
sin ϕ cos ϕ 0
~e1 0 0 ~e2 . 1 ~e3
0 0 1
,
B
E
( m ) ∼
cos ϕ = sin ϕ 0
E cos2 ϕ + sin2 ϕ = 1 = det((B m ) ), ∼ 1 0 0 0 1 0 . 0 0 1
m ∼
− sin ϕ cos ϕ 0
0 0 . 1
~e3
S
S
m ∼
I
T
S m ∼
K
T m ∼
T
cos α sin α 0 = − sin α cos α 0 , 0 0 1 1 0 0 sin β , = 0 cos β 0 − sin β cos β cos γ sin γ 0 = − sin γ cos γ 0 . 0 0 1
I ~k1 ~ K T T SS I m m k2 = ∼ m ∼ ∼ ~k3
K
I
m ∼
1, 2′ , 3′′ S
~i1 ~i2 = K m I ∼ ~i3
K
~i1 ~i2 . ~i3
sin β sin γ cos γ sin β . cos β
T
α
cos α cos γ − cos β sin α sin γ cos γ sin α + cos α cos β sin γ = − cos β cos γ sin α − cos α sin γ cos α cos β cos γ − sin α sin γ sin α sin β − cos α sin β
β
I
~s1 ~s2 ~s3
=
~t1 ~t2 = ~t3 ~k1 ~ = k2 ~k3
K
• • • • • • • • • •
I m ∼
K 1 0 0
0 cos α − sin α
cos β 0 sin β
~ i1 0 sin α ~i2 , ~i3 cos α
0 − sin β ~s1 ~s2 , 1 0 ~s3 0 cos β
cos γ − sin γ 0
cos β cos γ = − sin γ cos β − sin β
sin γ cos γ 0
~t1 0 0 ~t2 . ~t3 1
cos γ sin α sin β + cos α sin γ − cos α cos γ − sin α sin β sin γ − cos β sin α
− cos α cos γ sin β + sin α sin γ cos γ sin α + cos α sin β sin γ . cos α cos β
• •
~v E
B
θ ~v
v = (x, y, z)T v∼E = ∼B
x y = z
E
mB ∼
E
E
−1
E
x mB y ∼ z
x x x T y = EmB y = y ∼ z z z
B − I∼ m ∼
B − λI∼ m ∼
x 0 y = 0 . z 0
0 x y = 0 , z 0
x, y, z
B =0 Em − λI ∼ ∼ λ
λ1 = 1
λ2,3 = e±jθ θ x, y, z λ1
v∼ ~v
θ B
A
~r
~rneu = ~r + ∆~r
B
~rneu
~r
E
~r ∆~r p~1
θ p~1
~v
p~2
~v
~r
|~ p1 | = a sin θ
a = |~r| sin α = |~v × ~r|, ~v
p~1 ~i1 = ~v × ~r |~v × ~r|
p~1 = a sin θ · ~i1 = a sin θ
~v × ~r = sin θ ~v × ~r |~v × ~r|
p~2 θ |~ p2 | = a(1 − cos θ) = 2a sin2 . 2 p~2
p~1
~v
~i2 = ~v × ~i1 = ~v × (~v × ~r) a
p~2 = 2a sin2
θ θ ~v × (~v × ~r) = 2[~v × (~v × ~r)] sin2 . 2 2 a ~rneu = ~r + ∆~r
~rneu = ~r + ∆~r = ~r + ~p1 + p~2 = ~r + sin θ(~v × ~r) + 2[~v × (~v × ~r)] sin2
θ . 2
B r, (~v × ~r)B = v∼ ˜∼
0 −v3 0 v∼ ˜ = v3 −v2 v1 v˜∼
r + sin θ r∼neu,E = ∼B
r∼neu,E
= I + sin θ ∼
r
=
∼neu,E
E
E
v˜ r + 2 sin2
∼∼B
v˜∼ +
2 2˜ v∼
sin2
B m r ∼ ∼B
B =∼ I + sin θ m ∼
2
v˜∼ + 2˜ v∼ sin2
θ 2
θ 2
v2 −v1 , 0
v˜ v˜ r
∼ ∼∼B
θ r , 2 ∼B
r1 r = r2 , ∼ r3
~v
sin θ = 2sin
E
θ θ cos 2 2
B v∼ sin m =∼ I + 2˜ ∼
Θ0
θ = cos , 2
Θ1
=
Θ2
=
Θ3
=
θ 2
I∼ cos
θ θ + v˜ sin 2 2 ∼
.
θ v1 sin , 2 θ v2 sin , 2 θ v3 sin 2
θ∼ = [Θ1 , Θ2 , Θ3 ]T
E
B ˜) m =∼ I + 2 ˜θ∼(I∼Θ0 + θ∼ ∼
˜θ
=
∼
=
3 X
Θ2k
0 −Θ3 Θ3 0 −Θ2 Θ1
0 −v3 v3 0 −v2 v1
0 Θ2 −Θ1 = v3 sin 2θ 0 −v2 sin θ2 v2 θ θ −v1 sin = v˜ · sin ∼ 2 2 0
−v3 sin θ2 0 v1 sin θ2
=
cos2
θ θ θ θ + v12 sin2 + v22 sin2 + v23 sin2 2 2 2 2
=
cos2
θ θ + ( v12 + v22 + v32 ) sin2 | {z } 2 2
k=0
v2 sin 2θ
−v1 sin θ2 0
=1,
=
3 X
1.
Θ2k = 1.
k=0
E
1 − 2Θ22 − 2Θ32
2(Θ1 Θ2 − Θ0 Θ3 ) 2(Θ1 Θ3 + Θ0 Θ2 )
B = 2(Θ2 Θ3 − Θ0 Θ1 ) m 2(Θ1 Θ2 + Θ0 Θ3 ) 1 − 2Θ12 − 2Θ32 ∼ 2(Θ1 Θ3 − Θ0 Θ2 ) 2(Θ2 Θ3 + Θ0 Θ1 ) 1 − 2Θ12 − 2Θ22
2(Θ20 + Θ12) − 1 2(Θ1 Θ2 − Θ0 Θ3 ) 2(Θ1 Θ3 + Θ0 Θ2 ) E B = 2(Θ1 Θ2 + Θ0 Θ3 ) 2(Θ20 + Θ22 ) − 1 2(Θ2 Θ3 − Θ0 Θ1 ) . m ∼ 2(Θ1 Θ3 − Θ0 Θ2 ) 2(Θ2 Θ3 + Θ0 Θ1 ) 2(Θ20 + Θ23 ) − 1 θ
~e3 T
v∼ = (0, 0, 1)
θ θ Θ0 = cos , Θ1 = 0, Θ2 = 0, Θ3 = sin . 2 2 E
E
m ∼
2Θ20 − 1 −2Θ0 Θ3 0 2 2Θ 0 − 1 0 = 2Θ0 Θ3 0 0 2(Θ20 + Θ23 ) − 1 2 cos2 θ2 − 1 −2 sin θ2 cos 2θ 0 = 2 sin θ2 cos θ2 0 2 cos2 θ2 − 1 0 0 2(cos2 θ2 + sin2 2θ ) − 1
B
θ −1 2 θ θ 2 cos sin 2 2 2 cos2
E
m ∼
B
B m ∼
=
cos θ,
=
sin θ
cos θ = sin θ 0
0 0 . 1
− sin θ cos θ 0
~ω A
~v = t
B
~v + t
A
~ω B × ~v A
B A
~ω
B
A
=
A
! ~b2 ~ · b3 ~b1 + t ~b1 , ~b2 , b~3
A
~ω B := ~b1
A
! ~b3 ~ · b1 ~b2 + t
A
! ~b1 ~ · b2 ~b3 t A
~˙b2 · ~b3 + ~b2 ~b˙ 3 · ~b1 + ~b3 ~b˙ 1 · ~b2 .
() t
= (˙ )
~ω B
~b1 × ~b1 = 0~
~b1 A
˙ ˙ ~ω B × ~b1 = ~b2 × ~b1 ~b3 ·b~1 + ~b3 × ~b1 ~b1 · ~b2 . ~b1 ~b2
~b3
~b2 × ~b1 = −~b3 , ~b3 × ~b1 = ~b2
A
˙ ˙ ~ω B × ~b1 = − ~b3 · ~b1 ~b3 + ~b1 · ~b2 b~2 . ~b1 · ~b1 = 1
~b3 · ~b1 = 0
~˙b1 · ~b1 = 0
˙ ~˙b3 · ~b1 = −~b3 · ~ b1 ,
A
˙ ˙ ˙ ~ω B × ~b1 = ~b1 · ~b1 ~b1 + ~b1 · ~b2 ~b2 + ~b1 · ~b3 ~b3 . A
A
~ω B × ~b2
A
~ω B × ~b3
~˙b1
~b 1 t
~˙b1 · ~b1 ~˙b1 · ~b2
B
˙ = ~b2 , ˙ = ~b3
E
α
B
~ ωB ~bi
~e3
~e3 ~ei ~b1 ~b2 ~b3
=
cos α ~e1 + sin α ~e2 ,
=
− sin α ~e1 + cos α ~e2 ,
=
~e3 .
E
~˙b1 · b~3
~ bi ~˙b1 ~˙b2 ~˙b3
E
=
E
() t
−α˙ sin α ~e1 + α˙ cos α ~e2 ,
=
−α˙ cos α ~e1 − α˙ sin α ~e2 ,
=
~0.
~ ωB
( ˙) =
E
0 · ~b1 + 0 · b~2 + (−α˙ sin α ~e1 + α˙ cos α ~e2 ) · (− sin α ~e1 + cos α ~e2 ) ~b3 2 α(sin ˙ α + cos2 α) ~b3 = α˙ ~b3 .
= =
A ~b
B
ϕ(t) A
~ω B = ϕ˙ ~b β~
A
~ β = t
A
B
~ω B × β~
A B ~bi
~ai ~b1 ~b2 ~b3
A
=
cos θ~a1 + sin θ~a2 ,
=
− sin θ~a1 + cos θ~a2 ,
=
~a3 .
~ ωB
=
=
i −θ˙ cos θ~a1 − θ˙ sin θ~a2 · ~a3 ~b1 + 0 · ~b2 h i + −θ˙ sin θ~a1 + θ˙ cos θ~a2 · (− sin θ~a1 + cos θ~a2 ) ~b3 h
θ˙~b3 .
~ β = −L1~b1 − L2~b3 A
A
β~ t 2~ β
t2
~b1 , ~b2 , ~b3
~a1 , ~a2 , ~a3 ~a3 , ~b3
L1 , L2
θ˙~b3 × −L1~b1 − L2~b3 = −L1 θ˙~b2 , ! ! A ~ A ~ A B A ~ β β β = +A ~ ωB × t t t t t −L1 ¨θ~b2 − L1 θ˙2~b3 × ~b2 = L1 θ˙2~b1 − θ¨~b2 .
= = =
β~
~ai ~ai
~ai ~bi
~v = v ∼ A
A B m v ∼ ∼
B
β~
~v v˙ = ∼ A
A B ˙ m v + ∼ ∼
A
B v˙ . m ∼ ∼ B
B
A
A B v ˙ m ∼ B ∼ A ˙B m v ∼ ∼
~ v t B
A
B
B
B
A
~ v t
:
~ω B × ~v :
A
A
B m ∼
A
mB ∼
A
~ v t
~ω B × ~v
−1
−1
A
A
mB ∼
−1
˙ ˙ = ∼ v∼B v m ∼ B T A ˙ B A B m = m v ∼B ∼ ∼
A
B
B
˜ω · v ∼ ∼
˜ω = ∼
B
A
B m ∼
T
0 ω ˜∼ = ω3 −ω2
A
˙B m ∼
−ω3 ω2 0 −ω 1 ω1 0
ω1 ω2
ω3
A
˙B v m ∼ ∼
B
B
~k
B
A
A B B
A
B
A
A
~ω B = ωk~ ~k
B
ω = ϑ˙
ϑ
LA ϑ
LB B
A A
A B C D
B
B A
~ ω
B
= q˙1~b,
B
~ ω
D
A C
= q˙2~c , A
C C
D
B ~ ω
D
A
D ~ = −q˙3d.
B
C
C
B
D
C
~v A
A
B
~v = t
~v + t
A
A
B
~ω B × ~v
~ω B
B
A
K ~2 + I3 ω3~k3 ~ = I1 ω1~k1 + I2 ω2k H...