Download - Mechanisms Ppt
![Page 1: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/1.jpg)
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can
ChapterChapter
1&
2
MEEN 4110 – Mechanisms Design
Fall - 2010
Lecture 02
KINEMATICS FUNDAMENTALS
![Page 2: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/2.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.1 NUMBER SYSTHESIS
The term number synthesis has been coined to mean the determination of the number and order of links and joints necessary to produce motion of a particular DOF. Order in this context refers to the number of nodes perlink, i.e., binary, ternary, quaternary, etc.
The value of number synthesis is to allow the exhaustive determination of all possible combinations of links which will yield any chosen DOF.
This then equips the designer with a definitive catalog of potential linkages to solve a variety of motion control problems.
![Page 3: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/3.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.1 NUMBER SYSTHESIS
Hypothesis: If all joints are full joints, an odd number of DOF requires an even number of links and vice versa.
Proof: Given: All even integers can be denoted by 2m or by 2n, and all odd integers can be denoted by 2m - 1 or by 2n - 1, where n and m are any positive integers. The number of joints must be a positive integer.
Let: L = number of links, J = number of joints, and M = DOF = 2m (i.e., all even numbers)
Then: rewriting Gruebler's equation (Equation 2.1b) to solve for J,
![Page 4: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/4.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.1 NUMBER SYSTHESIS
Try: Substituting M=2m, and L=2n (i.e., both any even numbers)
This cannot result in J being a positive integer as required
Try: M=2m-1, and L=2n-1 (i.e., both any odd numbers)
This also cannot result in J being a positive integer as required
![Page 5: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/5.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.1 NUMBER SYSTHESIS
Try: M=2m-1, and L=2n (i.e., odd-even)
This is a positive integer for m>=1 and n>=2. Try: M=2m, and L=2n-1 (i.e., even-odd)
This is a positive integer for m>=1 and n>2
So, for our example of one-DOF mechanism we can only consider combinations of 2, 4, 6, 8 … links
![Page 6: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/6.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.1 NUMBER SYSTHESIS
Letting the order of the links be represented by:
The total number of links in any mechanism will be:
Since two link nodes are needed to make one joint
and nodes
![Page 7: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/7.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.1 NUMBER SYSTHESIS
Then
Substitute J and L in the Gruebler’s equation
The DOF is independent of number of ternary link in the mechanism. But because each ternary link has three nodes, it can only create or remove 3/2 joints
![Page 8: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/8.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.1 NUMBER SYSTHESIS
![Page 9: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/9.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.2 PARADOXES
The Gruebler’s criterion pays no attention to link sizes or shapes, it can give misleading results in the face of unique geometric configurations.
![Page 10: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/10.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.3 ISOMERS
The word isomer is from the Greek and means having equal parts.
Linkage isomers are analogous to chemical compounds in that the links (like atoms) have various nodes (electrons) available to connect to other link’s nodes.
![Page 11: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/11.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.4 LINKAGE TRANSFORMATION
There are several transformation techniques or rules that we can apply to planar kinematic chains
![Page 12: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/12.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.4 LINKAGE TRANSFORMATION
A fourbar crank-rocker linkage transformed into the fourbar slider-crank by the application of rule #1.
![Page 13: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/13.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.4 LINKAGE TRANSFORMATION
A fourbar slider-crank transformed via rule #4 by the substitution of a half joint for the coupler.
![Page 14: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/14.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.4 LINKAGE TRANSFORMATION
A fourbar linkage transformed into a earn-follower linkage by the application of rule #4. Link 3 has been removed and a half joint substituted for a full joint between links 2 and 4.
![Page 15: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/15.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.4 LINKAGE TRANSFORMATION
(a) shows the Stephenson's sixbar chain transformed by partial shrinkage of a ternary link (rule #5) to create a multiple joint. It is still a one-DOF Stephenson's sixbar.
(b) shows the Watt's sixbar chain from with one ternary link completely shrunk to create a multiple joint.
![Page 16: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/16.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.5 INTERMITENT MOTION
Is a sequence of motions and dwells. Dwell; is a period in which the output link remains stationary while the input link continues to move.
![Page 17: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/17.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.5 INTERMITENT MOTION
![Page 18: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/18.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.6 INVERSION
An inversion is created by grounding a different link in the kinematic chain. Thus there are as many inversions of a given linkage as it has links.
![Page 19: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/19.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.6 INVERSION
![Page 20: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/20.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.6 INVERSION – All inversions of the Grashof fourbar linkage
![Page 21: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/21.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.7 THE GRASHOF CONDITION
The four bar linkage, shown below, is a basic mechanism which is quite common. Further, the vast majority of planar one degree-of-freedom (DOF) mechanisms have "equivalent" four bar mechanisms. The four bar has two rotating links ("levers") which have fixed pivots, (bodies 2 and 4 above). One of the levers would be an input rotation, while the other would be the output rotation. The two levers have their fixed pivots with the "ground link"(body 1) and are connected by the "coupler link" (body 3).
![Page 22: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/22.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.7 THE GRASHOF CONDITION - Definitions
Crank- a ground pivoted link which is continuously rotatable.
Rocker- a ground pivoted link that is only capable of oscillating between two limit positions and cannot rotate continuously.
Grashof Condition- is a very simple relationship which predicts the rotation behavior or rotatability of a fourbar linkage's inversions based only on the link lengths
Let: S=length of shortest link L=length of longest link P=length of one remaining link Q=length of other remaining link
Then if: S+L<=P+Q
![Page 23: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/23.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.7 THE GRASHOF CONDITION
The linkage is Grashof and at least one link will be capable of making a full revolution with respect to the ground plane. This is called a Class I kinematic chain. If the inequality is not true, then the linkage is non-Grashof and no link will be capable of a complete revolution relative to any other link. This is a Class II kinematic chain.
For the Class I case, S + L < P + Q: Ground either link adjacent to the shortest and you get a
crank-rocker, in which the shortest link will fully rotate and the other link pivoted to ground will oscillate.
Ground the shortest link and you will get a double-crank, in which both links pivoted to ground make complete evolutions as does the coupler.
Ground the link opposite the shortest and you will get a Grashof double-rocker, in which both links pivoted to ground
oscillate and only the coupler makes a full revolution.
![Page 24: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/24.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.7 THE GRASHOF CONDITION
![Page 25: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/25.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.7 THE GRASHOF CONDITION
For the Class II case, S + L > P + Q: All inversions will be triple-rockers in which no link can
fully rotate. For Class III, S+L = P+Q
All inversion will be either double-cranks, or crank-rocker
![Page 26: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/26.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.7 THE GRASHOF CONDITION
![Page 27: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/27.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.7 THE GRASHOF CONDITION
![Page 28: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/28.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.8 LINKAGES OF MORE THAN FOUR BARS
Geared Fivebar Linkages
![Page 29: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/29.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.8 LINKAGES OF MORE THAN FOUR BARS
Sixbar Linkages
![Page 30: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/30.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can 2.9 EXAMPLES – GRASHOF CONDITION - SOLIDWORKS
http://www.me.unlv.edu/~mbt/320/Grashof.html http://wahyu-tjakraningrat.blogspot.com/2009/02/solidwo
rk-planar-joints.html
![Page 31: Mechanisms Ppt](https://reader033.vdocuments.site/reader033/viewer/2022061200/5477c37ab4af9f7b108b49f1/html5/thumbnails/31.jpg)
1. Kinematics FundamentalsMech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Mech
an
ism
s D
esi
gn
In
ter
Am
eri
can
Due, Tuesday, August 31, 2010
Homework2 www.bc.inter.edu/facultad/omeza