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Theory of Machines-I
Kinematic Analysis of Mechanisms
Basics of Instantaneous Centre of Rotation (ICR)
Prof. K N Wakchaure
Department of Mechanical Engineering
Sanjivani College of Engineering, Kopargaon
Basics of ICR
โ€ข The instant center of rotation (ICR), also called instantaneous velocity center,
or also instantaneous center or instant center, is the point fixed to a body
undergoing planar movement that has zero velocity at a particular instant of
time.
โ€œPoint on a rigid body whose velocity is zero at a given instantโ€
ICR method is used to find velocity of different links and points in the Mechanism.
Steering Gear MechanismFan
โ€ข Pin Joint
ICR is Located at the center of Pin
โ€ข For Sliding Pair: Straight/ Flat Surface
ICR lies at Infinity on the common normal at the point of
contact.
โ€ข For Sliding Pair: Curved Surface
ICR lies at centre of curvature of curved surface.
โ€ข For Rolling Pair
โ€ข ICR lies at the point of contact of two bodies.
Locations of ICR
Types of ICR
1. Fixed instantaneous centres
โ€ข I12 AND I14 are Fixed ICR which remain in the same place for all
configurations of the mechanism.
2. Permanent instantaneous centres
โ€ข I23 AND I34 as they move when the mechanism moves, but the joints are of
permanent nature.
3. Neither fixed nor permanent Centres
โ€ข I13 and I24 are neither fixed nor permanent instantaneous centres as they
vary with the configuration of the mechanism.
โ€ข Fixed and Permanent ICR can be find by viewing the mechanism but
for Neither fixed nor permanent Centres require to use Kennedys
Theorem
Kennedyโ€™s Theorem
โ€ข The Aronhold Kennedyโ€™s theorem states that if three bodies (Links) move relatively to
each other, they have three instantaneous centres and lie on a straight line.
1 2 3
I12 I23
I13
Suppose link 1,2,3 are having relative motion
According to Kennedys Theorem I12, I23, I13
should be along straight line irrespective of
sequence.
2 3 4
I23 I34
I24
I24, I23, I34
1 3 4
I13 I34
I24
I13, I34, I14
Procedure to Solve Numericals
Step-1:-Read the problem statement Carefully.
Step-2:-Draw the given Mechanism with Suitable Scale.
Step-3:-Give the numbers to the link in the mechanism starting with fixed LINK.
Step-4:-Find No. of ICR using Formula: N=
๐’โˆ—(๐’โˆ’๐Ÿ)
๐Ÿ
N= no of ICR
n=Total no. of links in the Mechanism
Procedure to Solve Numericals
Step-5:-Draw the table of Instantaneous centres.
1 2 3 4
I12 I23 I34
I13 I24
I14
3 2 1
Write no. of links
Total 6 ICR
Step-6:-Locate Fixed and Permanent ICR.
Procedure to Solve Numericals
Step-7:-Circle/ highlight the known ICR in the table..
1 2 3 4
I12 I23 I34
I13 I24
I14
3 2 1
Write no. of links
Total 6 ICR
I13 AND I24 are neither fixed nor permanent ICR
Kennedy's theorem is required to locate I13 and I24
Procedure to Solve Numericals
Step-7:-Draw one circle of Arbitrary diameter, divide it n number of Parts.
1 2 3 4
I12 I23 I34
I13 I24
I14
3 2 1
Step-8:-Draw one circle (Keneddyโ€™s Circle) of Arbitrary diameter, divide it โ€˜nโ€™
number of Parts.
n= No of Links in the Mechanism here n=4
Procedure to Solve Numericals
1 2 3 4
I12 I23 I34
I13 I24
I14
Step-9:- Join the points in Keneddyโ€™s circle for known ICR
Procedure to Solve Numericals
1 2 3 4
I12 I23 I34
I13 I24
I14
Step-10:- Use Kennedyโ€™s theoremm to locate I13 and I24
Now concentrate on I13,I13 should be diagonal of quadrilateral or
common side for two triangles
Here I13 is diagonal of Quad. 1234.
Join I13
I13 is making two triangles โˆ†I12.I23.I13
And โˆ†I14.I34.I13
I12 I23
I14 I34
I13
Join ICR I12 and I23 and extend line
Join ICR I14 and I34 and extend line
Above two line intersects at common point which is I13
Procedure to Solve Numericals
1 2 3 4
I12 I23 I34
I13 I24
I14
Step-10:- Use Kennedyโ€™s theoremm to locate I13 and I24
Now concentrate on I24,I24 should be diagonal of quadrilateral or
common side for two triangles
Here I24 is diagonal of Quad. 1234.
Join I24
I24 is making two triangles โˆ†I12.I14.I24
And โˆ†I23.I34.I24
I12 I๐Ÿ๐Ÿ’
I๐Ÿ๐Ÿ‘ I34
I24
Move ICR I14 at I12 and extend line
Join ICR I23 and I34 and extend line
Above two line intersects at common point which is I24
I34
Procedure to Solve Numericals
Step-11:- Find Velocity and Angular Velocity
Use Angular Velocity Ratio
Angular Velocity of any link in the mechanism if angular velocity
off any link/ input link is known to us
Find the angular velocity of link y when angular velocity of link x
is known to us
๐Ž ๐’š
๐Ž ๐’™
=
๐‘ฐ๐Ÿ๐’™ โˆ’ ๐‘ฐ๐’™๐’š
๐‘ฐ๐Ÿ๐’š โˆ’ ๐‘ฐ๐’™๐’š
angular velocity of link 3 when angular
velocity of link 2 is known
๐œ”3
๐œ”2
=
๐ผ12 โˆ’ ๐ผ23
๐ผ13 โˆ’ ๐ผ23
๐œ”2
Procedure to Solve Numericals
Step-12:- Find Velocity and Angular Velocity
Velocity of any point the mechanism
๐œ”2
Velocity of any point P which is on link Q
Then ๐‘‰๐‘ƒ = (๐ผ1๐‘„ โˆ’ ๐‘ƒ)X๐œ” ๐‘„*S.F
Velocity of any point P which is on link 3
Then ๐‘‰๐‘ƒ = (๐ผ13. ๐‘ƒ)X๐œ”3*S.F
P
๐‘ฝ ๐‘ท
Velocity of point C is the velocity of Slider
Velocity of any point C which is on link 3
Then ๐‘‰๐ถ = (๐ผ13. ๐ถ)X๐œ”3*S.F
Procedure to Solve Numericals
Step-12:- Find Velocity and Angular Velocity
Velocity of slider in the mechanism
๐œ”2
Velocity of Slider (N) in mechanism is the velocity of point(Say
M) at the contact between slider and adjacent link(k).
Velocity of any point M which is on link K
Then ๐‘‰๐‘ = ๐‘‰ ๐‘€ = (๐ผ1๐พ. ๐‘€)X๐œ” ๐พ*S.F
In this case velocity of slider(link 4) is the velocity of point
C(Point at the joint of link 3 and link 4).
By considering point C is on link 3
Then ๐‘‰4 = ๐‘‰๐‘ = (๐ผ13. ๐ถ)X๐œ”3*S.F
๐‘ฝ ๐‘ช = ๐‘ฝ ๐Ÿ’
โ€ขThankYou
Prof. K NWakchaureTheory of Machines-I

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Basics of Instantaneous Center rotation

  • 1. Theory of Machines-I Kinematic Analysis of Mechanisms Basics of Instantaneous Centre of Rotation (ICR) Prof. K N Wakchaure Department of Mechanical Engineering Sanjivani College of Engineering, Kopargaon
  • 2. Basics of ICR โ€ข The instant center of rotation (ICR), also called instantaneous velocity center, or also instantaneous center or instant center, is the point fixed to a body undergoing planar movement that has zero velocity at a particular instant of time. โ€œPoint on a rigid body whose velocity is zero at a given instantโ€ ICR method is used to find velocity of different links and points in the Mechanism. Steering Gear MechanismFan
  • 3. โ€ข Pin Joint ICR is Located at the center of Pin โ€ข For Sliding Pair: Straight/ Flat Surface ICR lies at Infinity on the common normal at the point of contact. โ€ข For Sliding Pair: Curved Surface ICR lies at centre of curvature of curved surface. โ€ข For Rolling Pair โ€ข ICR lies at the point of contact of two bodies. Locations of ICR
  • 4. Types of ICR 1. Fixed instantaneous centres โ€ข I12 AND I14 are Fixed ICR which remain in the same place for all configurations of the mechanism. 2. Permanent instantaneous centres โ€ข I23 AND I34 as they move when the mechanism moves, but the joints are of permanent nature. 3. Neither fixed nor permanent Centres โ€ข I13 and I24 are neither fixed nor permanent instantaneous centres as they vary with the configuration of the mechanism. โ€ข Fixed and Permanent ICR can be find by viewing the mechanism but for Neither fixed nor permanent Centres require to use Kennedys Theorem
  • 5. Kennedyโ€™s Theorem โ€ข The Aronhold Kennedyโ€™s theorem states that if three bodies (Links) move relatively to each other, they have three instantaneous centres and lie on a straight line. 1 2 3 I12 I23 I13 Suppose link 1,2,3 are having relative motion According to Kennedys Theorem I12, I23, I13 should be along straight line irrespective of sequence. 2 3 4 I23 I34 I24 I24, I23, I34 1 3 4 I13 I34 I24 I13, I34, I14
  • 6. Procedure to Solve Numericals Step-1:-Read the problem statement Carefully. Step-2:-Draw the given Mechanism with Suitable Scale. Step-3:-Give the numbers to the link in the mechanism starting with fixed LINK. Step-4:-Find No. of ICR using Formula: N= ๐’โˆ—(๐’โˆ’๐Ÿ) ๐Ÿ N= no of ICR n=Total no. of links in the Mechanism
  • 7. Procedure to Solve Numericals Step-5:-Draw the table of Instantaneous centres. 1 2 3 4 I12 I23 I34 I13 I24 I14 3 2 1 Write no. of links Total 6 ICR Step-6:-Locate Fixed and Permanent ICR.
  • 8. Procedure to Solve Numericals Step-7:-Circle/ highlight the known ICR in the table.. 1 2 3 4 I12 I23 I34 I13 I24 I14 3 2 1 Write no. of links Total 6 ICR I13 AND I24 are neither fixed nor permanent ICR Kennedy's theorem is required to locate I13 and I24
  • 9. Procedure to Solve Numericals Step-7:-Draw one circle of Arbitrary diameter, divide it n number of Parts. 1 2 3 4 I12 I23 I34 I13 I24 I14 3 2 1 Step-8:-Draw one circle (Keneddyโ€™s Circle) of Arbitrary diameter, divide it โ€˜nโ€™ number of Parts. n= No of Links in the Mechanism here n=4
  • 10. Procedure to Solve Numericals 1 2 3 4 I12 I23 I34 I13 I24 I14 Step-9:- Join the points in Keneddyโ€™s circle for known ICR
  • 11. Procedure to Solve Numericals 1 2 3 4 I12 I23 I34 I13 I24 I14 Step-10:- Use Kennedyโ€™s theoremm to locate I13 and I24 Now concentrate on I13,I13 should be diagonal of quadrilateral or common side for two triangles Here I13 is diagonal of Quad. 1234. Join I13 I13 is making two triangles โˆ†I12.I23.I13 And โˆ†I14.I34.I13 I12 I23 I14 I34 I13 Join ICR I12 and I23 and extend line Join ICR I14 and I34 and extend line Above two line intersects at common point which is I13
  • 12. Procedure to Solve Numericals 1 2 3 4 I12 I23 I34 I13 I24 I14 Step-10:- Use Kennedyโ€™s theoremm to locate I13 and I24 Now concentrate on I24,I24 should be diagonal of quadrilateral or common side for two triangles Here I24 is diagonal of Quad. 1234. Join I24 I24 is making two triangles โˆ†I12.I14.I24 And โˆ†I23.I34.I24 I12 I๐Ÿ๐Ÿ’ I๐Ÿ๐Ÿ‘ I34 I24 Move ICR I14 at I12 and extend line Join ICR I23 and I34 and extend line Above two line intersects at common point which is I24 I34
  • 13. Procedure to Solve Numericals Step-11:- Find Velocity and Angular Velocity Use Angular Velocity Ratio Angular Velocity of any link in the mechanism if angular velocity off any link/ input link is known to us Find the angular velocity of link y when angular velocity of link x is known to us ๐Ž ๐’š ๐Ž ๐’™ = ๐‘ฐ๐Ÿ๐’™ โˆ’ ๐‘ฐ๐’™๐’š ๐‘ฐ๐Ÿ๐’š โˆ’ ๐‘ฐ๐’™๐’š angular velocity of link 3 when angular velocity of link 2 is known ๐œ”3 ๐œ”2 = ๐ผ12 โˆ’ ๐ผ23 ๐ผ13 โˆ’ ๐ผ23 ๐œ”2
  • 14. Procedure to Solve Numericals Step-12:- Find Velocity and Angular Velocity Velocity of any point the mechanism ๐œ”2 Velocity of any point P which is on link Q Then ๐‘‰๐‘ƒ = (๐ผ1๐‘„ โˆ’ ๐‘ƒ)X๐œ” ๐‘„*S.F Velocity of any point P which is on link 3 Then ๐‘‰๐‘ƒ = (๐ผ13. ๐‘ƒ)X๐œ”3*S.F P ๐‘ฝ ๐‘ท Velocity of point C is the velocity of Slider Velocity of any point C which is on link 3 Then ๐‘‰๐ถ = (๐ผ13. ๐ถ)X๐œ”3*S.F
  • 15. Procedure to Solve Numericals Step-12:- Find Velocity and Angular Velocity Velocity of slider in the mechanism ๐œ”2 Velocity of Slider (N) in mechanism is the velocity of point(Say M) at the contact between slider and adjacent link(k). Velocity of any point M which is on link K Then ๐‘‰๐‘ = ๐‘‰ ๐‘€ = (๐ผ1๐พ. ๐‘€)X๐œ” ๐พ*S.F In this case velocity of slider(link 4) is the velocity of point C(Point at the joint of link 3 and link 4). By considering point C is on link 3 Then ๐‘‰4 = ๐‘‰๐‘ = (๐ผ13. ๐ถ)X๐œ”3*S.F ๐‘ฝ ๐‘ช = ๐‘ฝ ๐Ÿ’