... β βββ ββββ12212 23 122 31 23 2 31 23 2 23 11212 12 1252 32 ggll112 1 23 12 0+()+()( )++()=ββββg l sin 53 32 12 53 13 12 32 1212 23 231 32 33 12212 23 122 3 ()+()++()+()[]+()+[]+()+()[]+()+()+()+()+()cos ... disk.αωαωαω112 233 ===˙, ˙, ˙˙ωωω1 232 233 11=−()III˙ωωω 231 331 122=−()III˙ωωω 31 2112 233 =−()IIIωωωω10 23 0===, 05 93_ C08_fm Page 2 53 Monday, May 6, 2002 2:45 PMPrinciples of Dynamics: ... 5 0 433 nnnbyz=+0 655 0 756 II IaaSOabSObbSO,, .and an n nbnnncnn n=−+=− + −=−+ 634 547 39 1 23 1 23 12 3 05 93_ C07_fm Page 233 Monday, May 6, 2002 2:42 PM 236 Dynamics of Mechanical...