Each applied force is perpendicular to the lever arm, i.e., \(\theta = {90^{\rm{o}}}\). Suppose the forces oriented in the anti-clockwise direction are negative and those directed in the clockwise direction are positive.
Therefore, the torque due to the three applied forces is given by the following:
\(\begin{align}{\tau _{{\rm{applied}}\;{\rm{forces}}}} &= {r_2}{F_1} + {r_1}{F_2} + {r_2}{F_3}\\ &= \left( {0.24\;{\rm{m}}} \right)\left( {18\;{\rm{N}}} \right) + \left( {0.12\;{\rm{m}}} \right)\left( {35\;{\rm{N}}} \right) - \left( {0.24\;{\rm{m}}} \right)\left( {28\;{\rm{N}}} \right)\\ &= 1.8\;{\rm{m}}\;{\rm{N}}\end{align}\)
This torque is clockwise, so assume that the wheel is rotating clockwise.