Transcript

COMBINATORIAL METHOD FOR CHARACTERIZING SINGULAR CONFIGURATIONS IN PARALLEL MECHANISMS

INTRODUCTION

THE EQUIMOMENTAL LINE AND EQUIMOMENTAL SCREW

THE KENNEDY AND DUAL KENNEDY METHOD

APPLYING THE COMBINATORIAL METHOD FOR FINDING

SINGULARITY CONDITIONS

CONCLUSION

TABLE OF CONTENTS

INTRODUCTIONParallel manipulators have a specific mechanical architecture where all the links areconnected both at the base.

3/6 Stewart Platform-3D Triad

6/6 Stewart Platform 3D Double Triad 3D Tetrad

Hunt (1978) found a singular configuration of Stewart Platformwhen all the lines meeting one given line

Merlet (1989) studied the singularity of six-DOF 3/6-SP basedon the Grassmann line geometry. He discovered many newsingularities, including 3C, 4B, 4D, 5A, and 5B

Shoham and Ben-Horin (2006) proved that there is a class of144 combinations in which their singularity condition isdelineated to be the intersection of four planes at one point

Huang et al. (2014) introduced, based on the kinematicalrelationship of rigid bodies, that these four planes includethree normal planes of three velocities of three non-collinearpoints in the end effector, and the plane is determined bythese three points themselves

3C

4D 5A

5B

4B

THE EQUIMOMENTAL LINE AND EQUIMOMENTAL SCREW

Two absolute equimomental Screw $𝟏 and $𝟐 and their relative equimoment screw $𝟏,𝟐

Forces 𝑭𝑰 and 𝑭𝑰𝑰 acting along lines of action π’†π’’π’Žπ’ 𝑰,𝟎 and π’†π’’π’Žπ’ 𝑰𝑰,𝟎

Absolute equimomental line- a line upon which the moment exertedRelative equimomental line- for any two forces there exists a line along

which they exert the same moment at eachpoint on the line by the force is equal to zero

Relative equimomental screw- The relative eqms is a line where thedifference between the two forces, 𝑆1π‘Žπ‘›π‘‘ 𝑆2, and the difference betweenthe two moments of the two forces along this line, 𝑆01 and 𝑆02, are bothin the same direction

Property 1: For any two adjacent faces if the relative eqml passes through themeeting point of the two absolute eqml of these two faces themechanism is in a singular configuration

Non-singular configuration Singular configuration

THE KENNEDY AND DUAL KENNEDY METHOD

The Arnohold-Kennedy theorem states thatthe relative instant centers of any three linksi, j and k of the mechanism, 𝐼𝑖𝑗, πΌπ‘–π‘˜ and πΌπ‘—π‘˜,

must lie on a straight line

The dual Kennedy Theorem in statics: For anythree forces: π‘­π’Š, 𝑭𝒋 and π‘­π’Œ the three relative

eqml: π’†π’’π’Žπ’ π’Š,𝒋 , π’†π’’π’Žπ’ 𝒋,π’Œ and π’†π’’π’Žπ’ π’Š,π’Œ

intersect at the same point

APPLYING THE COMBINATORIAL METHOD FOR FINDING SINGULARITY CONDITIONS

π‘’π‘žπ‘šπ‘™ 𝐼,0 = 5 = 8

π‘’π‘žπ‘šπ‘™ 𝐼𝐼𝐼,0 = 3 = 7

π‘’π‘žπ‘šπ‘™ 𝐼,𝐼𝐼𝐼 = 1 ∨ 2 ∧ 7 ∨ 8

The dual Kennedy circle of a 3C configuration

Bundle Singularity (3C): A singular bundleoccurs when four lines of the six legsintersect at a common point

3C singular configuration with the eqml where faces IV, V, VI, VII are zero faces.

π‘’π‘žπ‘šπ‘™ 𝐼,0 = 1 ∨ 2 ∧ 9 ∨ 10

π‘’π‘žπ‘šπ‘™ 𝐼,𝑉𝐼𝐼 = 7 ∨ 8 ∧ 9 ∨ 12

π‘’π‘žπ‘šπ‘™ 0,𝑉 = 3 ∨ 4 ∧ 10 ∨ 11

π‘’π‘žπ‘šπ‘™ 𝑉𝐼𝐼,𝑉 = 5 ∨ 6 ∧ 11 ∨ 12

π‘’π‘žπ‘šπ‘™ 𝐼𝑋,0 = 10

π‘’π‘žπ‘šπ‘™ 𝐼𝑋,𝑉𝐼𝐼 = 12

π‘’π‘žπ‘šπ‘  0,𝑉𝐼𝐼 = 𝐼, 0 ∨ 𝐼, 𝑉𝐼𝐼 ∧ 0, 𝑉 ∨ 𝑉𝐼𝐼, 𝑉 ∧

𝐼𝑋, 0 ∨ 𝐼𝑋, 𝑉𝐼𝐼

𝑛1 be the normal to π‘’π‘žπ‘šπ‘™ 0,𝑉 and π‘’π‘žπ‘šπ‘™ 𝑉𝐼𝐼,𝑉

𝑛2 be the normal to π‘’π‘žπ‘šπ‘™ 𝐼,0 and π‘’π‘žπ‘šπ‘™ 𝐼,𝑉𝐼𝐼

The 3D Tetrad is in a singular position if and only if there exists a line which is perpendicular to both: 𝑛1, 𝑛2 and 𝑛3

𝑛3 be the normal to π‘’π‘žπ‘šπ‘™ 𝐼𝑋,0 and π‘’π‘žπ‘šπ‘™ 𝐼𝑋,𝑉𝐼𝐼

CONCLUSION

The method presented is consistent with other approaches thatappear in the literature

It seems that the method introduced is applicable in finding thesingularity of many other types of mechanisms and is not limited to aparticular mechanism

The method is based on discrete mathematics thus can becomputerized easily

I believe that equimomental line/ screw is a fundamental concept instatics and have a significant potential in characterizing singularity ofspatial parallel mechanisms


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