COSMOS: Complete Online Solutions Manual Organization System
Chapter 3, Solution 116.
Let ( R, M D ) be the equivalent force-couple system at O.
Now ΣF : R = ΣF
= (1.8 lb )( − sin 40°i − cos 40°k ) + (11 lb )( − sin12° j − cos12°k ) + (18 lb )( − sin15° j − cos15°k )
or R = − (1.157 lb ) i − ( 6.95 lb ) j − ( 29.5 lb ) k
Note that each belt force may be replaced by a force-couple that is equivalent to the same force plus the
moment of the force about the shaft (x axis) of the sander. Then ...
ΣM O : M O = ΣM O
i
j
k
= (1.8 lb )
0
0.75 in. 2.2 in.
− sin 40°
0
− cos 40°
− ( 2.5 in.)(11 lb ) i − ( 9 in.) i × (11 lb )( − sin12° j − cos12°k )
+ ( 2.5 in.)(18 lb ) i − ( 9 in.) i × (18 lb )( − sin15° j − cos15°k )
= (1.8 )( −0.75cos 40°i − 2.2sin 40° j + 0.75sin 40°k ) − 27.5i
+ ( 99 )( sin12°k − cos12° j) + 45i + (162 )( sin15°k − cos15° j) ( lb ⋅ in.)
= ( −1.03416 − 27.5 + 45 ) i + ( −2.5454 − 96.837 − 156.480 ) j
+ ( 0.86776 + 20.583 + 41.929 ) k ( lb ⋅ in.)
or M O = (16.47 lb ⋅ in.) i − ( 256 lb ⋅ in.) j + ( 63.4 lb ⋅ in.) k
.
COSMOS Chapter 3 Solution 116
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