To determine where the force acts, you need to understand the flow of stress in the supports--- the bridge is deforming the supports slightly due to its sag, and the contact is most significantly stressed at the point closest to the center of the bridge, and this is where you place the force. If the supports were metal springs instead of rigid blocks, you could calculate the deformation in each spring, and see that it is somewhat bigger nearer the center, but as the spring gets saggier, the force distributes more equally. In the limit of complete sagginess, the force is distributed over the whole meter length of the support, and in the limit of complete rigidity, it is right at the end closest to the center. Assuming complete rigidity is the closer approximation, your calculations are correct, and equal to the answer in the book to the given precision.