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Robot Modeling and the Forward Kinematic Solution ME 3230 R. R. Lindeke

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Looking Closely at the T 0 n Matrix At the end of our discussion of “Robot Mapping” we found that the T 0 n matrix related the end of the arm frame (n) to its base (0) – Thus it must contain information related to the several joints of the robot It is a 4x4 matrix populated by complex equations for both position and orientation (POSE)

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Looking Closely at the T 0 n Matrix To get at the equation set, we will choose to add a series of coordinate frames to each of the joint positions The frame attached to the 1 st joint is labeled 0 – the base frame! – while joint two has Frame 1, etc. The last Frame is the end or n Frame

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Looking Closely at the T 0 n Matrix As we have seen earlier, we can define a HTM (T (i-1) i ) to the transformation between any two SO 3 based frames Thus we will find that the T 0 n is given by a product formed by:

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Looking Closely at the T 0 n Matrix For simplicity, we will redefine each of the of these transforms (T (i-1) i ) as A i Then, for a typical 3 DOF robot Arm, T 0 n = A 1 *A 2 *A 3 While for a full functioned 6 DOF robot (arm and wrist) would be: T 0 n = A 1 *A 2 *A 3 *A 4 *A 5 *A 6 A 1 to A 3 ‘explain’ the arm joint effect while A 4 to A 6 explain the wrist joint effects

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Looking At The Frame To Frame Arrangements – Building A Modeling Basis When we move from one frame to another, we will encounter: Two translations (in a controlled sense) Two rotations (also in a controlled sense) A rotation and translation WRT the Z i-1 These are called the Joint Parameters A rotation and translation WRT the X i These are called the Link Parameters

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A model of the Joint Parameters NOTE!!!

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A model of the Link Parameters a i or

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Talking Specifics – Joint Parameters i is an angle measured about the Z i-1 axis from X i-1 to X i and is a variable for a revolute joint – its fixed for a Prismatic Joint d i is a distance measured from the origin of Frame (i-1) to the intersection of Z i-1 and X i and is a variable for a prismatic joint – its fixed for a Revolute Joint

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Talking Specifics – Link Parameters a i (or l i ) is the Link length and measures the distance from the intersection of Z i-1 to the origin of Frame i measured along X i i is the Twist angle which measures the angle from Z i-1 to Z i as measured about X i Both of these parameters are fixed in value regardless of the joint type. A Further note: Fixed does not mean zero degrees or zero length just that they don’t change

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Very Important to note: Two Design Axioms prevail in this modeling approach Axiom DH1: The Axis X i must be designed to be perpendicular to Z i-1 Axiom DH2: The Axis X i must be designed to intersect Z i-1 Thus, within reason we can design the structure of the coordinate frames to simplify the math (they are under our control!)

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Returning to the 4 ‘Frame-Pair’ Operators: 1 st is which is an operation of pure rotation about Z or: 2 nd is d which is a translation along Z or:

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Returning to the 4 Frame Operators: 3 rd is a Translation Along X or: 4 th is which is a pure Rotation about X or:

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The Overall Effect is:

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Simplifying this Matrix Product: This matrix is the general transformation relating each and every of the frame pairs along a robot structure

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So, Since We Can Control the Building of this Set Of Frames, What Are The Rules? We will employ a method called the Denavit- Hartenberg Method It is a Step-by-Step approach for modeling each of the frames from the initial (or 0) frame all the way to the n (or end) frame This modeling technique makes each joint axis (either rotation or extension) the Z-axis of the appropriate frame (Z 0 to Z n-1 ). The Joint motion, thus, is taken W.R.T. the Z i-1 axis of the frame pair making up the specific transformation matrix under design

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The D-H Modeling Rules: 1) Locate & Label the Joint Axes: Z 0 to Z n-1 2) Establish the Base Frame. Set Base Origin anywhere on the Z 0 axis. Choose X 0 and Y 0 conveniently and to form a right hand frame. 3) Locate the origin O i where the common normal to Z i-1 and Z i intersects Zi. If Z i intersects Z i-1 locate O i at this intersection. If Z i-1 and Z i are parallel, locate O i at Joint i+1

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The D-H Modeling Rules: 4) Establish X i along the common normal between Z i-1 and Z i through O i, or in the direction Normal to the plane Z i-1 – Z i if these axes intersect 5) Establish Y i to form a right hand system Set i = i+1, if i

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The D-H Modeling Rules: 7) Create a table of “Link” parameters: 1) i as angle about Z i-1 between X’s 2) d i as distance along Z i-1 3) i as angle about X i between Z’s 4) a i as distance along X i 8) Form HTM matrices A 1, A 2, … A n by substituting , d, and a into the general model 9) Form T 0 n = A 1 *A 2 *…*A n

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Some Issues to remember: If you have parallel Z axes, the X axis of the second frame runs perpendicularly between them When working on a revolute joint, the model will be simpler if the two X directions are in alignment at “Kinematic Home” – ie. Our model’s starting point To achieve this kinematic home, rotate the model about moveable axes (Z i-1 ’s) to align X’s Kinematic Home is not particularly critical for prismatic joints An ideal model will have n+1 frames However, additional frames may be necessary – these are considered ‘Dummy’ frames since they won’t contain joint axes

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Applying D-H to a General Case:

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General Case: Considering Link i Connects Frames: i-1 and I and includes Joint i This information allowed us to ‘Build’ The L.P. (link parameter) Table as seen here FramesLinkVar da S C S C i -1 to iiR + 37 17.5 u47.8 u17.8 0.306.952S( + 37 )C( + 37 )

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Leads to an A i Matrix:

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Frame Skeleton for Prismatic Hand Robot

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LP Table: FramesLinkVar da S C S C 0 11R 11 00-90 0S1C1 1 22R 22 600 01S2C2 2 33R 33 0.5090 10S3C3 3 44P00 d 4 + 4.25000 01S4C4 4 n5R 55 1000 01S5C5 Depends on Location of n(end)-frame!

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Leading to 5 A i Matrices

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#5 is: Now, Lets Form the FKS: T 0 n = A 1 *A 2 *A 3 *A 4 *A 5 I’ll use a software: Mathematica This value is called the Hand Span and depends on the Frame Skeleton we developed

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Solving for FKS Here we have a special case – two of the Joints are a “planer arm” revolute model – i.e. parallel, consecutive revolute joints These are contained in the A 2 and A 3 Matrices These should be pre-multiplied using a trigonometric tool that recognizes the sum of angle cases ((Full)Simplify in mathematica) Basically then: T 0 n = A1*{A2 A3}*A4*A5

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Finalizing the FKS – perform a physical verification Physical verification means to plug known angles into the variables and compute the A i ’s and FKS against the Frame Skeleton

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Another? 6dof Articulating Arm – ( The Figure Contains Frame Skelton)

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LP Table Frame s Lin k Var da S C S C 0 11R 11 0090 0S1C1 1 22R 22 0a200 01S2C2 2 33R 33 0a300 01S3C3 3 44R 44 0a4-90 0S4C4 4 55R 55 0090 10S5C5 5 66R 6*6*d6000 01S6C6 * With End Frame in Better Kinematic Home. Here, as shown, it would be ( 6 - 90 ), which is a problem!

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A Matrices

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A Matrices, cont. At Better Kinematic Home!

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Leads To: FKS of: After Preprocessing A2-A3-A4, with (Full)Simplify function, the FKS must be reordered as A1-A 234 -A5-A6 and Simplified

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Solving for FKS Pre-process {A 2 *A 3 *A 4 } with Full Simplify They are the “planer arm” issue as in the previous robot model Then Form: A 1 * {A 2 *A 3 *A 4 }*A 5 *A 6 Simplify for FKS!

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Simplifies to (in the expected Tabular Form): nx = C1·(C5·C6·C234 - S6·S234) - S1·S5·C6 ny = C1·S5·C6 + S1·(C5·C6·C234 - S6·S234) nz = S6·C234 + C5·C6·S234 ox = S1·S5·S6 - C1·(C5·S6·C234 + C6·S234) oy = - C1·S5·S6 - S1·(C5·S6·C234 + C6·S234) oz = C6·C234 - C5·S6·S234 ax = C1·S5·C234 + S1·C5 ay = S1·S5·C234 - C1·C5 az = S5·S234 dx = C1·(C234·(d6·S5 + a4) + a3·C23 + a2·C2) + d6·S1·C5 dy = S1·(C234·(d6·S5 + a4) + a3·C23 + a2·C2) - d6·C1·C5 dz = S234·(d6·S5 + a4) + a3·S23 + a2·S2

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Verify the Model Again, substitute known’s (typically 0 or 0 units) for the variable kinematic variables Check each individual A matrix against your robot frame skeleton sketch for physical agreement Check the simplified FKS against the Frame skeleton for appropriateness

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After Substitution: nx = C1·(C5·C6·C234 - S6·S234) - S1·S5·C6 = 1(1-0) – 0 = 1 ny = C1·S5·C6 + S1·(C5·C6·C234 - S6·S234) = 0+ 0(1 – 0) = 0 nz = S6·C234 + C5·C6·S234 = 0 + 0 = 0 ox = S1·S5·S6 - C1·(C5·S6·C234 + C6·S234) = 0 – 1(0 + 0) = 0 oy = - C1·S5·S6 - S1·(C5·S6·C234 + C6·S234) = -0 – 0(0 + 0) = 0 oz = C6·C234 - C5·S6·S234 = 1 – 0 = 1 ax = C1·S5·C234 + S1·C5 = 0 + 0 = 0 ay = S1·S5·C234 - C1·C5 = 0 – 1 = -1 az = S5·S234 = 0 dx = C1·(C234·(d6·S5 + a4) + a3·C23 + a2·C2) + d6·S1·C5 = 1*(1(0 + a4) + a3 + a2) + 0 = a4 + a3 + a2 dy = S1·(C234·(d6·S5 + a4) + a3·C23 + a2·C2) - d6·C1·C5 = 0(1(0 + a4) + a3 + a2) – d6 = -d6 dz = S234·(d6·S5 + a4) + a3·S23 + a2·S2 = 0(0 + a4) + 0 + 0 = 0

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