Problem Diagram
Rotation and Translation Related
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As with all dynamics problems, first start with a detailed diagram showing all forces and accelerations involved ( shown at the left).
Summing the forces acting on the spool give
ΣFx => fA = max
ΣFy =>
NA - mg = 0
Since the spool rotates about its center of gravity, the moments are
summed at the center, giving
ΣMcg => fAr = Icg α
There are four unknowns (fA, ax, NA, α) but only three equations. Thus, to complete the solution, a fourth equation must be derived that relates the acceleration of the spool's center of gravity to the angular acceleration.
Because the spool does not slip, the acceleration of point A can be related to the acceleration of the cg point,
acg = aA + acg/A
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Acceleration Vectors for
Link Between Points cg and A
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acg-xi + 0j = [aA-xi + aA-y j] + [acg-xi - acg-y j]
axi + 0j = [atrucki + ω2r j] + [α r i - ω2r j]
Equating i terms give
ax = atruck - rα
There are now four equations to solve for the four unknowns (fA, ax, NA, α). Combining gives two equations,
(max) r = Icgα
ax = atruck - rα
Reducing to one equation,
mr (atruck - rα) = Icgα
or
α = m r atruck / [Icg + mr2]
= 140 (0.5) (1) / [17.5 + 140 (0.5)2]
= 1.333 rad/s2
and
ax = atruck - rα = 1 - 0.5(1.333) = 0.3333 m/s
Thus, the spool accelerates to in the same direction as the truck acceleration even though it rolls backwards with an angular acceleration of 1.333 rad/s2.
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Linear Acceleration Direction
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To determine the time it takes for the spool to reach the end of the truck, it helps to draw a diagram of the spool at the end of the truck.
From the diagram, when the spool reaches the end of the truck, the following relationship is true,
xtruck - 3.5 m = xcg
Use the acceleration of the center of gravity of the spool and the acceleration of the truck to integrate to find xcg and xtruck,
xcg(t) = 0.167 t2
xtruck(t) = 1/2 t2
Substituting the expressions for xcg and xtruck, gives
1/2 t2 - 3.5 = 0.167 t2
Solving for t,
t = 3.24 s |