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科技譯文 科技譯文 AUTOMATIC FIXTURE SYNTHESIS IN 3D Kamen Penev Programmable Automation Laboratory Computer Science Department and Institute for Robotics and Intelligent Systems University of Southern California Los Angeles CA 90089 0781Aristides A G Requicha Programmable Automation Laboratory Computer Science Department and Institute for Robotics and Intelligent Systems University of Southern California Los Angeles CA 90089 0781 ABSTRACT A fixture is an arrangement of fixturing modules that locate and hold a workpart during a manufacturing operation In this work we consider fixtures with frictionless point contacts and present a method for placement of contact points on a non prismatic 3D workpart It is a non deterministic potential field algorithm for contact point placement The method provides a basic framework for the integration of heterogeneous high level fixturing agents through an interface based on zones of attraction and repulsion on the workpart boundary The algorithm may produce redundant fixtures and can augment partial solutions to complete form closure fixtures 1 INTRODUCTION A fixture is an arrangement of fixturing modules that locate and hold a workpart during a manufacturing operation such as machining assembly and inspection Fixturing is of essential importance to industrial manufacturing and constitutes a significant part of all manufacturing costs Therefore fixture design automation is very important Fixture design involves a great variety of considerations such as restraint deterministic location loadability and tool accessibility Efficient algorithms that address the whole range of fixturing issues for a comprehensive domain of workparts do not yet exist Recently Brost and Peters published an algorithm Brost Peters 1996 that extends the earlier classic work of Brost and Goldberg Brost Goldberg 1994 to the 3D domain This algorithm however requires vertical and horizontal planar surfaces to constitute a substantial part of the workpart boundary It generates all possible fixtures and then rates them accordingly to certain metrics This is computationally expensive Wagner et al presented an algorithm that uses seven modular struts mounted in a box to fixture polyhedra Wagner et al 1995 This algorithm is not complete in the sense that it cannot effectively handle certain cases such as a cube with faces parallel to the box It also suffers from high computational complexity Wallack and Canny suggested another method with an enumerate and rate flavor Wallack Canny 1996 It can fixture prismatic workparts with planar and cylindrical vertical surfaces Ponce proposed an algorithm that utilizes curvature effects to compute fixtures with four fingers for polyhedral parts Ponce 96 The reduced number of contacts should provide for better complexity of this algorithm but the quality of the produced fixtures seems to be inferior to the ones that utilize more contacts and provide classical form closure In this paper we present a new potential field algorithm that efficiently produces quality fixture designs Our algorithm works for arbitrary workparts and provides convenient universal means for representing various fixturing requirements This algorithm is a direct generalization of the 2D potential field fixturing algorithm of Penev and Requicha Penev Requicha 1996 We consider fixtures with frictionless point contacts It has been proven that seven contacts are necessary1 Somoff 1900 and sufficient Markenscoff et al 1990 to immobilize any workpart2 in 3D Following a least commitment strategy the process of fixture synthesis may be separated into three stages fixturing task analysis contact point placement and fixture layout design In the fixturing task analysis phase the workpart geometry and manufacturing process are analyzed to identify various parameters of the fixturing problem such as cutting forces inaccessible or forbidden areas and also to find features that may be useful for applying fixturing devices such as machined flat surfaces horizontal and vertical surfaces pairs of parallel surfaces pairs of perpendicular surfaces etc Figure 1 Contact point placement In the contact point placement phase a number of contact points are placed on the workpart boundary Figure 1 so that the resulting configuration of contacts satisfies the constraints identified in the analysis phase as well as certain kinematic requirements that must be satisfied by any fixture such as total restraint ba Figure 2 From contact point configuration to fixture layout design In the layout design phase towers of fixturing components are built and placed around the workpart 科技譯文 so as to contact the part at the point locations computed in the contact point placement phase For example a contact point on a horizontal workpart surface Figure 2a may lead to the instantiation of an overhead clamp that contacts the workpart at that particular point Figure 2b This is a design for function problem constrained by the set of available fixturing modules and their parameters The set of contact points are the functional specification and the fixture layout is a configuration of components that achieves it In this research we focus on contact point placement and its integration with part and task analysis An arrangement of contact points must satisfy certain kinematic conditions in order to be a basis for a good fixture In particular it must provide form closure deterministic location clamping stability detachability and loadability Asada By The algorithm uses a discretization of the workpart boundary similar to the meshes used in FEA However unlike FEA our attention is on the mesh nodes rather than on the mesh elements Discretization was chosen for the following reasons First we can handle workparts with arbitrary geometry as long as the part s boundary is a collection of smooth surfaces which we know how to mesh This requirement is satisfied by all surfaces used in modern CAD systems Second discretization is necessary in order to avoid an expensive computation of geodesic curves Third discretization should not significantly affect the results as long as the number of discrete candidate locations on the boundary is much larger than the number of surfaces In our implementation the discretized boundary consists of several hundred points only Experimental evidence indicates that this is sufficient for realistic workparts We introduce a potential field on the workpart boundary defined by zones of attraction and repulsion which we call P zones The contacts are modeled as charged particles that move on the boundary driven by this potential field The contacts are also subject to mutual repulsion based on the distance between each two contacts in the wrench vector space The algorithm executes a series of simulation epochs Each epoch starts with a random configuration proceeds through a certain number of steps toward lower potential energy and ends with a test for kinematic conditions form closure The algorithm terminates when an epoch produces satisfactory configuration To spread the contact points on the boundary we simulate repulsion between each pair of them The intensity of repulsion between two contact points depends on the distance between their corresponding wrenches in the wrench vector space Our simulation proceeds in a limited number of steps or until equilibrium is reached The resulting placement should have a good chance of leading to a good fixture Such a randomized method assumes that the set of n tuples of contact points for n greater than three that satisfy the kinematic requirements has measure greater than zero and is relatively large That is the solution space is large Although we have not been able to prove this hypothesis mathematically our experiments have confirmed it Moreover the measure increases with the number of contact points e g it is easier to find a form closure arrangement with eight points than with seven The notion of repulsion is essential in our method as it allows other considerations to be accommodated easily We can put additional repulsion spots on the workpart boundary to represent forbidden regions We can also introduce centers of attraction These correspond to areas that were recommended by the analysis phase as desirable for placing contact points e g datum surfaces Thus we propose a potential field for uniformly representing heterogeneous fixturing information Regions of repulsion correspond to areas with positive potential Negative potential is associated with attraction Zero potential corresponds to neutral areas The initial randomly selected contact points are regarded as particles that are being attracted or repelled by a potential field that includes a pairwise repulsion The goal of the system of contact points is to minimize its total potential energy 2 THE INPUT The input to our algorithm consists of CAD models of the workpart boundary and a set of solid P zones Each P zone defines a potential field influencing region with non zero charge 3 DISCRETIZING THE WORKPART BOUNDARY The first step in our method is to discretize the boundary of the workpart thus creating the candidate contact point locations which we call nodes Discretization is done by invoking a standard faceter embedded in the geometric modeler we use The discretization is stored in an oriented graph data structure Each node of the graph corresponds to a node on the mesh The edges of the graph correspond to edges of the mesh connecting neighboring nodes At each node the screw representing the point contact is computed and stored A screw is a concise and convenient representation of the surface normal and the location of the node It is used in all kinematic tests based on screw theory 4 COMPUTING THE POTENTIAL FIELD The contact points in our algorithm are subject to the combined action of two components forming the potential field The background potential field is one of these components It is generated by the P zones and does not depend on the location of the contact points The background potential field is computed only once in the beginning of the algorithm The other component is dynamic and is due to the repulsion between the contacts The dynamic component is computed at each epoch The computation of the background potential field proceeds as follows First we find all nodes that lie inside P zones We perform membership classification of each node against each P zone Tilove 1980 If the node is inside a certain P zone the charge of the P zone contributes to the node s charge The contribution may be positive or negative depending on the sign of the zone s charge After this procedure the nodes that classify outside all P zones remain with zero charge If a node m classifies inside P zones z1 z2 zk its charge Cm equals the sum of the charges of those P zones ziki 1 After the charge of the nodes inside P zones is evaluated we proceed by computing the potential of all nodes We define the potential at a charged node to be initially equal to its charge Pm Cm For each charged node m with charge Cm we perform a breadth first traversal of its neighbors updating their potential according to the formula Pdnnm 1210 Here d m n is the distance between nodes m the charged node and n and d0 is a constant called distance of influence The distance between two nodes is defined as the number of edges on the 科技譯文 shortest path between them on the mesh boundary approximation Figure 3 n m d m n 7 Figure 3 Distance between two nodes on the mesh Assuming the mesh satisfies certain common quality requirements this distance approximates quite well the actual geodesic distance between two points on the object s boundary The breadth first traversal goes only d0 nodes deep Thus a charged node causes updates of the potential only in its d0 neighborhood For example if the three dark nodes in Figure 4 have charge 100 and d0 3 the potential in this part of the mesh will be as shown by the numbers next to each node 0 0 0 0 0 0 0 0 0 8 8 16 16 16 16 16 8 8 8 8 8 16 8 8 74 74 74 49 49 49 49 16 16 16 49 49 Figure 4 Potential field generated by three charged nodes The dynamic potential represents repulsion between the contact points The repulsion between two contacts depends on how distant their corresponding screws are as 6 dimensional vectors Pmnn 1142 Here is a small number to avoid division by zero is a scaling factor that makes the dynamic potential compatible with the background component and m n is the Euclidean distance between the screws at nodes m and n The rationale behind repulsion based on screw distance is the following A necessary and sufficient condition for form closure is that the set of contact screws positively spans the entire R6 Wagner et al 1995 As the contact screws repel each other they will tend to distribute regularly in the space thus increasing the possibility of form closure 5 EPOCHS Each epoch starts with a random initial placement of contact points Then these contact points are subjected to the combined forces due to the background potential field and the repulsion between the contact points themselves The algorithm proceeds in an iterative fashion First the dynamic component of the aggregated potential field is computed accordingly to 3 The dynamic potential is computed only at the contacts and their immediate neighbors After the combined potential is computed each contact is moved to the neighbor node with the lowest potential Thus a step is completed If the number of steps has reached a certain limit or no contact was moved i e equilibrium has been reached the epoch is completed Throughout this process special attention is paid to nodes that lie on edges and vertices of the workpart These nodes do not have a screw associated with them as there is no normal defined there Therefore they cannot be a possible contact location Instead they serve merely as transit nodes in the simulation This is achieved by always considering the neighbors of such a node whenever the node itself is addressed The net result of an epoch is that the initially random configuration transforms into one that has more regular distribution of contact screws in the screw vector space while at the same time keeping away from repulsion zones and providing contacts inside attraction zones 6 TEST In the test phase we check whether the placement of contact points provides form closure This is done using the method of Chou et al Chou et al 19 It tests whether there exists a non zero motion screw that complies with the constraints imposed by the contact wrenches swiCi 01 The existence of s is tested using linear programming techniques If no such motion exists the arrangement of contacts provides form closure If the test succeeds the algorithm terminates Otherwise a new epoch is initiated If the test fails and a certain number of generations have been tried we increase the number of contact points C Increasing C improves the probability of ending up with a form closure configuration as well as having more contacts in P zones of attraction The algorithm ensures that no two contact points are placed on the same mesh node Therefore in the extreme case there are three contacts on each face Such a placement obviously immobilizes any polyhedral part Hence the completeness of the algorithm at least for polyhedral parts After a redundant form closure configuration is computed the algorithm can remove the extra contacts in the order of decreasing background potential i e starting with the ones in P zones of highest repulsion Redundant fixtures are sometimes preferred as they minimize part deflection and vibration The system can operate with or without redundancy reduction The decision might be guided by the analysis phase based on the geometric shape of the part and the magnitude of the external forces or a human operator may allow redundancy manually and even force it by setting the initial number of contacts to be more than the theoretical minimum 7 in 3D 科技譯文 It is possible for the kinematic test to succeed but the potential at some contacts to be high This can happen if a contact is trapped in a local minimum of the potential field where the potential is high To handle such situations we introduce a threshold parameter called maximum allowable potential Arrangements with potential at any contact higher than the threshold are discarded This new test may lead to situations in which the algorithm does not terminate because no fixture exists with sufficiently small potential Imagine the extreme example that the entire workpart boundary is a forbidden region Therefore we limit the number of epochs to ensure termination In the case of such termination the algorithm outputs the solution with the lowest maximum potential 7 DISCUSSION The proposed algorithm solves the essential problem in fixture design placing contact points on the workpart that provide form closure It can be incorporated in a complete fixture design system that provides modules for fixturing task analysis and layout design The algorithm provides a simple but powerful interface to the fixturing task analysis modules based on zones of attraction and repulsion Admittedly not every contact configuration can be implemented by a certain fixturing toolkit in the layout design phase It may be necessary to invoke the contact placement algorithm several times until a feasible configuration is produced 7 1 Fixturing Task Analysis Various fixturing heuristics and requirements can be expressed in terms of zones of higher attraction or repulsion For example attraction zones may be used to represent datum surfaces machined surfaces surfaces with good orientation areas with good accessibility areas that need additional support to prevent deflection and deformation Repulsion zones can represent inaccessible areas forbidden areas due to tool accessibility requirements surfaces with poor orientation cast surfaces sensitive surfaces that are vulnerable to scratching etc An important open problem is how to assign numerical values to the P zone potential One possibility is to classify the constraints into a small number of categories e g strong repulsion repulsion neutral attraction strong attraction All constraints within the same category are assigned the same potential While such a scheme does not reflect subtle differences in priorities of the fixturing constraints it will probably capture the most important ones 7 2 Fixture Completion An important property of the algorithm is that it allows partial fixtures to be input Partial fixtures may be produced by other fixturing agents humans or computer programs who place certain fixels they know are necessary and hand the work over to our algorithm for completion The algorithm then places additional contacts so that form closure is achieved We represent the partial fixture as fixed contacts which participate in the mutual repulsion with the free contacts but are not allowed to move In this light the algorithm may be viewed as a fixture completion engine 7 3 Non determinism and Redundancy Due to the randomness of the initial placement in each generation the algorithm is non deterministic i e it can produce different solutions given the same input This is desirable as a contact point configuration may be rejected by the layout design module and the algorithm will have to produce another solution The algorithm may produce redundant fixtures in certain cases Redundant fixtures have drawbacks as well as advantages over the minimal ones Certainly they impair loadability and waste components However they may also minimize part deflection and deformation In practice human designers often produce redundant fixtures 7 4 Efficiency The running time of the algorithm does not depend directly on the complexity of the workpart boundary A simple cuboid and a complex curved workpart will be discretized with a comparable number of mesh nodes This decision is based on the intuitive assumption that a few hundred evenly distributed nodes on