TY - GEN
T1 - Dynamic response of the long channel resting on the soil and Excited by SH waves
AU - Hayir, Abdul
PY - 2009
Y1 - 2009
N2 - The purpose of this paper is to discuss the response of the channel having semi-circular crosssection and the constant thickness in the case of SH waves. The dynamic interaction of soil and the channel that takes place during the passage of seismic waves through the soil has been of much interest to engineers. It has a bearing on the stresses in the channel and the changes in the time history of incident ground motion. It is assume that the channel is flexible, stiff and rigid, and soil is only elastic. The results are calculated from flexible case to stiff one for comparison. They are also determined for rigid case. If the channel is stiff enough, it might be assumed as rigid. An analytical solution is derived using wave-expansion method in polar coordinates for elastic channel. For the solutions of rigid channel, the equation of motion(Newton Second Law) is derived. This solution method takes into account dynamic interactions between soil and the structure. The results are derived depending on the incident wave angles and dimensionless wave numbers. Absolute responses of the channel are illustrated with respect to dimensionlessfrequencies and compared.
AB - The purpose of this paper is to discuss the response of the channel having semi-circular crosssection and the constant thickness in the case of SH waves. The dynamic interaction of soil and the channel that takes place during the passage of seismic waves through the soil has been of much interest to engineers. It has a bearing on the stresses in the channel and the changes in the time history of incident ground motion. It is assume that the channel is flexible, stiff and rigid, and soil is only elastic. The results are calculated from flexible case to stiff one for comparison. They are also determined for rigid case. If the channel is stiff enough, it might be assumed as rigid. An analytical solution is derived using wave-expansion method in polar coordinates for elastic channel. For the solutions of rigid channel, the equation of motion(Newton Second Law) is derived. This solution method takes into account dynamic interactions between soil and the structure. The results are derived depending on the incident wave angles and dimensionless wave numbers. Absolute responses of the channel are illustrated with respect to dimensionlessfrequencies and compared.
UR - http://www.scopus.com/inward/record.url?scp=69949148042&partnerID=8YFLogxK
U2 - 10.1061/41031(341)287
DO - 10.1061/41031(341)287
M3 - Conference contribution
AN - SCOPUS:69949148042
SN - 9780784410318
T3 - Proceedings of the 2009 Structures Congress - Don't Mess with Structural Engineers: Expanding Our Role
SP - 2625
EP - 2634
BT - Proceedings of the 2009 Structures Congress - Don't Mess with Structural Engineers
T2 - 2009 Structures Congress - Don't Mess with Structural Engineers: Expanding Our Role
Y2 - 30 April 2009 through 2 May 2009
ER -