{"responseHeader":{"status":0,"QTime":7,"params":{"q":"{!q.op=AND}id:\"95851\"","hl":"true","hl.simple.post":"","hl.fragsize":"5000","fq":"!embargo_tdt:[NOW TO *]","hl.fl":"ocr_t","hl.method":"unified","wt":"json","hl.simple.pre":""}},"response":{"numFound":1,"start":0,"docs":[{"modified_tdt":"2015-11-02T00:00:00Z","thumb_s":"/b1/a6/b1a62cd1f3c36720e0a22f1e540eec21dab17ad6.jpg","oldid_t":"compsci 3669","setname_s":"ir_computersa","file_s":"/be/38/be38554b84e39dabe9c37c4a88c875fb2d9c6740.pdf","title_t":"Page 19","ocr_t":"V4 V2 1 ~ Figure 2.2. The Standard Cell of FEA Cells Transformation Physical Coordinates Canonical Coordinates Figure 2.3. Coordinate System Transformation canonical coordinates are functions whose graphs pass through the first vertex of the cell and are parallel to the three edges emitting from the first vertex of the cell. Since the edges are straight, the canonical coordinates are linear polynomials of the world coordinates. Thus we have the following equations: [ Tx+k, (2.2) [ [ ~ 'TJ ( ]T' ell a12 a13 T a21 a22 a23 ), a31 a32 a33 x [ X y Z ]T' k [ kl k2 k3 ]T, By differentiating the canonical coordinates with respect to the world coordinates, the Jacobin matrix of the coordinate transformation can be computed as:","restricted_i":0,"id":95851,"created_tdt":"2015-11-02T00:00:00Z","format_t":"application/pdf","parent_i":95941,"_version_":1642982571740495874}]},"highlighting":{"95851":{"ocr_t":[]}}}