Flexure and shear load rating evaluation of composite bridge superstructure under effect of different trucks load types

Author(s):  
Ali Fadhil Naser ◽  
Hussam Ali Mohammed ◽  
Ayad Ali Mohammed
2001 ◽  
Vol 54 (4) ◽  
pp. 427-444 ◽  
Author(s):  
Rigoberto Burgueño ◽  
Vistasp M. Karbhari ◽  
Frieder Seible ◽  
Robert T. Kolozs

2000 ◽  
Vol 4 (3) ◽  
pp. 120-128 ◽  
Author(s):  
M. D. Hayes ◽  
J. J. Lesko ◽  
J. Haramis ◽  
T. E. Cousins ◽  
J. Gomez ◽  
...  

2009 ◽  
Vol 79-82 ◽  
pp. 1855-1858 ◽  
Author(s):  
Yan Lei Wang ◽  
Qing Duo Hao ◽  
Jin Ping Ou

The concept of the fiber reinforced polymer (FRP)-concrete composite design was exploited in a new type of bridge superstructure. The proposed FRP-concrete composite bridge superstructure is intended to have durable, structurally sound, and cost effective composite system that will take full advantage of the inherent and complementary properties of FRP material and concrete. As a trial case, a prototype bridge superstructure was designed as a simply supported single-span one-lane bridge with a span length of 10 m. The bridge superstructure consists of two bridge decks and each bridge deck is comprised of four FRP box sections combined with a thin layer of concrete in the compression zone. A test specimen, fabricated as a one-third scale model of the prototype bridge superstructure, was subjected to four-points loading to simulate the two heaviest axles of the Chinese design truck load. The test results indicate that the proposed bridge model meets the stiffness requirement and has significant reserve strength.


Geophysics ◽  
1990 ◽  
Vol 55 (8) ◽  
pp. 1047-1056 ◽  
Author(s):  
H. J. Stam

The two‐dimensional elastodynamic P- and SV-wave motion generated by an arbitrary distributed impulsive surface load on the boundary of a semiinfinite perfectly elastic solid is investigated theoretically. With the aid of the Cagniard‐de Hoop method, closed‐form expressions are obtained for the particle velocity and the stress of the generated wave motion. The cases of a uniformly distributed strip load of the normal‐load and the shear‐load types are worked out in detail. Synthetic seismograms are presented for an array of receivers close to the strip source and for an array of receivers at depth. The results are important as test cases for accuracy in the computational modeling of elastodynamic wave problems, by time‐domain finite‐difference or finite‐element methods.


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