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Chapter 2. Prehension

Chapter 2. Prehension

Chapter 2. Prehension

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240 THE PHASES OF PREHENSION<br />

6.3.2 Fingertip force and joint torques<br />

We have just considered the issue of transmitting forces through<br />

the fingertips in order to counterbalance the weight of the object. The<br />

vector F identifies the required intensities of the wrenches at the<br />

fingertips. The second issue to consider is how those forces are<br />

generated in an intrinsic body space, such as muscle lengths. In<br />

robotics, a similar but somewhat simpler problem is to determine the<br />

forces and torques at the joints that wil generate these desired fingertip<br />

contact forces. Multi-jointed fingers in a hand apply forces at the<br />

fingertips that are a function of the joint angles and the forces and<br />

moments at the joints. What is needed is a relationship between the<br />

contact forces and the joint torques.<br />

Starting with one finger with three joints, a coordinate frame is<br />

placed at the fingertip, as seen in Figure 6.13. The infinitesimal joint<br />

angles of the jth finger, &j=[&jl,&j2,&j31' *, can be transformed to a<br />

fingertip position (x,y,z) and onentation ( Q~, qZ) as follows:<br />

where J is the Jacobian matrix that maps from joint space (the joint<br />

angles) to Cartesian space (end point position and orientation). Let tj<br />

be the twist system at the jth finger. Then, for the jth finger, Equation<br />

5 can be written as:<br />

t. J = J.4. J J (6)<br />

For a five fingered hand, equation (6) expands into the following:

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