... consider (11. 5)Clearly, For the second block, (11. 6) γγγ γγn n n nnn n n nnn nn n nnfl l fl l l−−− −−− −− −−−−−=− =− − 111 1112 22 2112 2[]/,[ ]/, .,, , , , KKLLTjjj−−−= 111 .KKkkkL0L0TTTTjjjjjjjjjjjjjjll==−−−111λλλλ,kjjjjj ... that (11. 37)γγjHλj2λjjjjj2=−γγγγγγγγHHKMMK==1001 11 1212 22 kkkk.() [ ] [ ] ,λλ22 11 222 11 22 1220++ + +=kk kk kλ+−=− + ± + − +[]=− + ± − −[],[][][ ][][]2 11 22 11 222 11 22 122 11 22 11 222122124124kk ... ,KM+=λj200749_Frame_C11 Page 159 Wednesday, February 19, 2003 5:13 PM© 2003 by CRC CRC Press LLC 162 Finite Element Analysis: Thermomechanics of Solids Since the jkth entries of XTMX and XTKX...