Relative Velocity and Acceleration withTranslating and Rotating Frames
Example: (continued)
aP|F = aQ|F + aP|B + αB x rQP - ωB2 rQP + 2 ωB x vP|B
0 i + 0 j = aQ i + aP|B i1 + αB k x r i1 - ωB2 r i1 + 2 ωB k x vP|B i1
Next calculate cross products and collect terms using i1 and j1 components
0 i + 0 j = 0 i1 + 0 j1 = aQ i + aP|B i1 + r αB j1 - ωB2 r i1 + 2 ωB vP|B j1
Recall from coordinate transformation i = cos θ i1 ˗ sin θ j1 so
0 i1 + 0 j1 = aQ [ cos θ i1 ˗ sin θ j1 ] + aP|B i1 + r αB j1 - ωB2 r i1 + 2 ωB vP|B j1
0 i1 + 0 j1 = [ aQ cos θ + aP|B ˗ ωB2 r ] i1 + [ ˗ aQ sin θ + r αB + 2 ωB vP|B ] j1
Next equate i1 and j1 components.
0 = aQ cos θ + aP|B ˗ ωB2 r or 0 = ˗ 36 (4/5) + aP|B ˗ (32) 5 aP|B = 369/5
0 = ˗ aQ sin θ + r αB + 2 ωB vP|B 0 = 36 (3/5) + 5 αB + 2(3)(˗ 20) αB = 492/25
So aP|B = 369/5 i1 = 369/5 [ i cos θ + j sin θ ] = 1476/25 i + 1107/25 j m/sec2 (result)
and αB\F = 492/25 k rad/sec2 (result)
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