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Samenvatting chapter 1 - Kinematics and Dynamics of Mechanisms (E048300)

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Samenvatting chapter 1 - Kinematics and Dynamics of Mechanisms (E048300)

Institution
Course

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Chapter 1 : Kinematics
of linkages and mechanism


1 .
1) Introduction

↳ Read


2)
Mobility
1 .

of Mechanisms
-




_

Y. f 4
sf π rj
~
jhas 3DOF (Xi s Y, Gil
Ii
If j
Xi .
word
body
y
>
- ex .
Connected to another a
,

hove
y. not
independentand
sone relation
. -- Cnstäit
¤ i



i


here number of constrat eq 2 NCE 2

3-
= = =




=
from the 3 card
,
only
3-NCE = 1
may
be considered independent
に NCE )

allow translation
3-NCE only
L =

indep .
word
.


O allev

-only




rotation






"T interaction has
force
2 unknown scolos
cop ..




Liz
zodwayscontactpar
allowed
in hat slipping
↳ Assume now

NCE
=
= 2
does not have to
^
be
( ↳
FCD =


slipping
;

fulfilled ?
Note : z =
3 -
c = 3 -

13 -
NCEI =
INCE =
1 = 7 ( = 2 = て = 1

=
) と = NCE



* Consider mechanism , has Connected
a which a links
by means
of p constraints



Coming
constraintsConstraints of Carpet
the
p a

, o unconnected links of mechanisms would have Im DOF



↳ Constraint
each ofClose < take
away
(3-2) DOF
↳ # DOF
left after imposition of
,
the
p contraints is Called
Mobility
&
#1 DOF
juint #2DOF
joint
MO =
3n -

(3 -



1)p -

(3 -




2(pa
#God to determine the the
= Mo =

3 m-2pr-p2 reg .
position of system ?
M20 kinematic chain cannot movs/

over constructed
=> Mox o
?
6
example
~
U an :
C=
C= =A
C <

c = 1




}
3 >
- M =
7 I#links) 3 7 2 3 1
く=^
- -


mo
= . .




2 §
E =Λ 3 => Mo = ·2
~- pe =
c =e c =^


Uㅋ
has 2 DOF)


indept
1 1 k
p2
=

Omi2DOF ?= par
~



Gird to
C
required
l
2
=




mech
.
des cribe motion
of the
le .




g
. 2 , p1

~
for e . remove roller K


6

{
n =




m = 8 =
m0 3 6 2 8 1

c
= = .
- .
-




1 MO Λ
Na = → ) =




-motion be determ word
con
by only 1

=
fu e .
α


=> in
general : set of MO Card
9.19--quo determines
positio of
mechanism


= r =

r191 , 92 .
----

quot ( Position vector

~ See some mix er+ exercise

1 3) .
Applications to Mechanisms

* linear
kinemotice
of slides


first what's the
mobility
? - n = 2
, pr
= 2
; pa
= 0





= Mo = 3 . 2 -
2 . 2 -
0 = 2
M ^


↳ 2 cod can describe the mech .
Ot sin L
α
=> α ,
ot



"
"Tacac r = I) -


aii2 + vt(t) + y(a(2 + vt eiG)


C
등옮 α

Vt CosL
> >
->
v
= =
t) - aLax + vGL -
vt] eind)


3) a2imn2
+
-

+ vim + + vt2(x)

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