The author has done a fine job in adopting the discusser's thesis work [l] 3 to the case where the Fourier integrals have singularities on the real axis of the transform variables. The discusser has several comments regarding the use of [1] in the author's paper.The author has mentioned that Miklowitx [4] in that he was able to obtain results for the interior of the half space as well as for the surface for a distributed surface load.The form of solution obtained bj r the author in equations (48) The integrals in equations (49) and (50) do not exist for x = 0 and y = 0 because their integrands are indeterminate. Physically, the x = 0 and y = 0 planes are special because the cylindrical waves which emanate from under the sides of the quadrant load are discontinuous iu these planes. However, the hemispherical waves generated by the point load in the corner of the quadrant are also discontinuous in the x = 0 and y -0 planes in such a way as to render the velocities vp continuous over these planes. The discontinuities in the hemispherical waves can be deduced by evaluating the integrals in equations (49) and (50) as x -*• ±0 and y -*• ±0. This type of overlapping of waves was also foundThe solutions obtained by the author are uniformly valid in z for z > 0; i.e., the interior of the half space. However, for z -0, the surface of the half space, the solutions must be reassessed to include the contribution of the Rayleigh surface wave.-.. The additional manipulations necessary to obtain the Milutions for z = {) are shown in [1,5], In addition, as noted by the author, the discusser has found that interior solutions can be u-ed for numerical evaluation of the disturbance near the surface. The discusser's numerical calculations [6, 7] for points near the .--urface show a response similar to that found by Pekeris [4] for surface points.