Authors: Russell C. Hibbeler
ISBN-13: 978-0133915426
See our solution for Question 99P from Chapter 17 from Hibbeler's Engineering Mechanics.
We are given the mass, horizontal force and length of bar as $m = 12\;{\rm{kg}}$, $F = 80\;{\rm{N}}$ and $L = 2\;{\rm{m}}$ respectively.
We are asked to determine the acceleration of the center of the roller at the instant the force is applied.
The following is the free body diagram.

To find the forces in x-direction, we will use the relation,
\[\begin{array}{c} \Sigma {F_x} = ma\\ \left( {80\;{\rm{N}}} \right) = \left( {12\;{\rm{kg}}} \right)a\\ a = 6.66\;{\rm{m/}}{{\rm{s}}^2} \end{array}\]To find the angular acceleration, we will use the relation,
\[\begin{array}{c} \Sigma {M_A} = {M_0}\\ \left( {ma \times h} \right) = \left( {I\alpha } \right)\\ \left( {ma \times h} \right) = \left( {\frac{1}{{12}}m{L^2}} \right)\alpha \end{array}\]Here, h is the height of the bar from point A to G.
On plugging the values in the above relation, we get,
\[\begin{array}{c} \left( {12\;{\rm{kg}} \times 6.66\;{\rm{m/}}{{\rm{s}}^2} \times 1\,{\rm{m}}} \right) = \left( {\frac{1}{{12}}\left( {12\;{\rm{kg}}} \right){{\left( {2\;{\rm{m}}} \right)}^2}} \right)\alpha \\ \alpha = 19.98\;{\rm{rad/}}{{\rm{s}}^2} \end{array}\]To find the acceleration of the center of the roller, we will use the relation,
\[\begin{array}{c} \vec a = {{\vec a}_A} + \left( {\alpha \times h} \right) - {\omega ^2}r\\ ai + a'j = {a_A}i + \left( { - 19.98k \times 1j} \right) - 0\\ 6.66i + a'j = \left( {{a_A} - \left( {19.98} \right)} \right)i \end{array}\]On equating the components of $i$, we get,
\[\begin{array}{c} 6.66 = {a_A} - 19.98\\ {a_A} = 26.64\;{\rm{m/}}{{\rm{s}}^2} \end{array}\]On equating the components of $j$, we get,
\[a' = 0\]