Rigid-Body mechanics Instant Screw of rigid-Body Motion(cont'd) ATA=w1, Ab=n(a-S2a a-na) wxa-wx Jw2 wl2
Rigid-Body Mechanics • Instant Screw of Rigid-Body Motion (cont'd)
Rigid-Body mechanics Instant Screw of rigid-body motion - example H Unit Cube H e B C E A Seek: L Q=00 100
Rigid-Body Mechanics • Instant Screw of Rigid-Body Motion - Example e'1 = e3 e'2 = -e1 Q = e'3 = -e2 z x A y B C D E F G H A' B' C' D' E' F' G' H' e1 e2 e3 e' 1 e' 3 e' 2 1 Unit Cube − − 1 0 0 0 0 1 0 1 0 Seek: L
Rigid-Body mechanics Instant Screw of rigid-Body motion- example tr(Q)=1+2 cosd=0 φ=120 vect(Q)=sinde sino e To get equation for L, we still need a (Q-1)2(Qa-a) p0= 2(1-co6o) ford≠0
Rigid-Body Mechanics • Instant Screw of Rigid-Body Motion – Example tr(Q) = 1 + 2 cos = 0 cos = - vect(Q) = sine = sin = e = To get equation for L, we still need a: 2 1 = − − 3 1 3 1 3 1 2 3 1 1 1 2 1 2 3 = 120º − 3 1 3 1 3 1
Rigid-Body mechanics Instant Screw of Rigid-Body motion- Example(cont'd Use point a as reference point 000 Q-I 1010 (Q-1)(-a) 1-10|3=-3cp= 31+12 >x+1=y-3=z+
Rigid-Body Mechanics • Instant Screw of Rigid-Body Motion – Example (cont'd) Use point A as reference point a = a' = Q – I = (Q – I) (- a') = p0 = L: x + 1 = y – 3 = z + 2 0 0 0 −1 3 0 − − − − − 1 0 1 0 1 1 1 1 0 − − − = − − − − − − 2 3 1 1 3 0 0 1 1 1 1 0 1 0 1 − − − 3 2 1 3 1 T 3 1 3 2 3 1 1 3 1 3 1 + = − + = + z y x