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Evaluation of a gravel transport sensor for bed load measurements in natural flows
A recent acoustic instrument (Gravel Transport Sensor, GTS) was tested for predicting sediment transport rate (bed load rate) in gravel bed streams. The GTS operation is based on the particle collision theory of submerged obstacles in fluids. When particles collide with the GTS cylinder their moment...
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Published in: | International journal of sediment research 2009-03, Vol.24 (1), p.1-15 |
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description | A recent acoustic instrument (Gravel Transport Sensor, GTS) was tested for predicting sediment transport rate (bed load rate) in gravel bed streams. The GTS operation is based on the particle collision theory of submerged obstacles in fluids. When particles collide with the GTS cylinder their momentum is recorded in the form of ping rates. The GTS is attractive for further consideration here because of its potential to provide continuous unattended local bed load measurements, especially in areas found in streams that access may be difficult under extreme conditions. Laboratory experiments coupled with numerical simulations for the same flow conditions were performed in order to determine the conditions under which particles of different size will hit the GTS cylinder and be able to register a ping rate. The GTS was able to detect the number of particles with diameter in the range of 15.9 to 25.4 mm, with reasonable accuracy, if the applied Shields effective stress τ*e = τ* - τ*cr was in the range of 0.006 to 0.015. A drawback of the tested prototype GTS, however, was that it exerted increased resistance on the incoming particles. The added drag effects increased the overall resistance that was exerted by the flow on particles and thus increased the likelihood that particles will rest in the ambient region of the cylinder instead of hitting it. Numerical simulation of the flow around the GTS cylinder revealed that changing the prototype geometry from cylindrical to ellipsoid or rhomboid will increase the likelihood of the particles hitting the instrument under the same flow conditions failed by the original tested GTS cylinder. |
doi_str_mv | 10.1016/S1001-6279(09)60012-3 |
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The GTS was able to detect the number of particles with diameter in the range of 15.9 to 25.4 mm, with reasonable accuracy, if the applied Shields effective stress τ*e = τ* - τ*cr was in the range of 0.006 to 0.015. A drawback of the tested prototype GTS, however, was that it exerted increased resistance on the incoming particles. The added drag effects increased the overall resistance that was exerted by the flow on particles and thus increased the likelihood that particles will rest in the ambient region of the cylinder instead of hitting it. 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(Thanos)</creatorcontrib><creatorcontrib>ELHAKEEM, Mohamed</creatorcontrib><creatorcontrib>KNAPP, Doug</creatorcontrib><title>Evaluation of a gravel transport sensor for bed load measurements in natural flows</title><title>International journal of sediment research</title><addtitle>International Journal of Sediment Research</addtitle><description>A recent acoustic instrument (Gravel Transport Sensor, GTS) was tested for predicting sediment transport rate (bed load rate) in gravel bed streams. The GTS operation is based on the particle collision theory of submerged obstacles in fluids. When particles collide with the GTS cylinder their momentum is recorded in the form of ping rates. The GTS is attractive for further consideration here because of its potential to provide continuous unattended local bed load measurements, especially in areas found in streams that access may be difficult under extreme conditions. Laboratory experiments coupled with numerical simulations for the same flow conditions were performed in order to determine the conditions under which particles of different size will hit the GTS cylinder and be able to register a ping rate. The GTS was able to detect the number of particles with diameter in the range of 15.9 to 25.4 mm, with reasonable accuracy, if the applied Shields effective stress τ*e = τ* - τ*cr was in the range of 0.006 to 0.015. A drawback of the tested prototype GTS, however, was that it exerted increased resistance on the incoming particles. The added drag effects increased the overall resistance that was exerted by the flow on particles and thus increased the likelihood that particles will rest in the ambient region of the cylinder instead of hitting it. Numerical simulation of the flow around the GTS cylinder revealed that changing the prototype geometry from cylindrical to ellipsoid or rhomboid will increase the likelihood of the particles hitting the instrument under the same flow conditions failed by the original tested GTS cylinder.</description><subject>Bed load measurement</subject><subject>Flume experiments</subject><subject>Gravel streams</subject><subject>Gravel transport sensors</subject><subject>Numerical simulations</subject><subject>传感器</subject><subject>粒子碰撞</subject><subject>负荷测量</subject><issn>1001-6279</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2009</creationdate><recordtype>article</recordtype><recordid>eNqFkU1vFDEMhucAEqXwE5AiDkAPA5kkk5mcEKrKh1QJiY9z5CTOkiWbbJOZrfrvyXYrjnCwLFuPbb1-u-7FQN8OdJDvvg-UDr1kk3pD1YVsBev5o-7sb_tJ97TWLaVczbM4675dHSCusIScSPYEyKbAASNZCqS6z2UhFVPNhfgWBh2JGRzZIdS14A7TUklIJMGyFojEx3xbn3WPPcSKzx_yeffz49WPy8_99ddPXy4_XPdWcL70k1WSjswI62aKox2EsSMqL9BIAM6kl6Nxs5xmZ4HBNBommGPW2Mm40c_8vLs47b2F5CFt9DavJbWLerNN9W6rkVGq6FF5Y1-f2H3JNyvWRe9CtRgjJMxr1YpyKWYlWSNf_ZPkQsx0nKcGjifQllxrQa_3Jeyg3OmB6qMX-t4LfXy6pkrfe6F5m3t_msP2m0PAoqsNmCy6UNAu2uXw3w0vHy7_ymlzE5p0A_a3DxE1U0ocJfM_n9iezw</recordid><startdate>20090301</startdate><enddate>20090301</enddate><creator>PAPANICOLAOU, Athanasios N. 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(Thanos)</au><au>ELHAKEEM, Mohamed</au><au>KNAPP, Doug</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Evaluation of a gravel transport sensor for bed load measurements in natural flows</atitle><jtitle>International journal of sediment research</jtitle><addtitle>International Journal of Sediment Research</addtitle><date>2009-03-01</date><risdate>2009</risdate><volume>24</volume><issue>1</issue><spage>1</spage><epage>15</epage><pages>1-15</pages><issn>1001-6279</issn><abstract>A recent acoustic instrument (Gravel Transport Sensor, GTS) was tested for predicting sediment transport rate (bed load rate) in gravel bed streams. The GTS operation is based on the particle collision theory of submerged obstacles in fluids. When particles collide with the GTS cylinder their momentum is recorded in the form of ping rates. The GTS is attractive for further consideration here because of its potential to provide continuous unattended local bed load measurements, especially in areas found in streams that access may be difficult under extreme conditions. Laboratory experiments coupled with numerical simulations for the same flow conditions were performed in order to determine the conditions under which particles of different size will hit the GTS cylinder and be able to register a ping rate. The GTS was able to detect the number of particles with diameter in the range of 15.9 to 25.4 mm, with reasonable accuracy, if the applied Shields effective stress τ*e = τ* - τ*cr was in the range of 0.006 to 0.015. A drawback of the tested prototype GTS, however, was that it exerted increased resistance on the incoming particles. The added drag effects increased the overall resistance that was exerted by the flow on particles and thus increased the likelihood that particles will rest in the ambient region of the cylinder instead of hitting it. Numerical simulation of the flow around the GTS cylinder revealed that changing the prototype geometry from cylindrical to ellipsoid or rhomboid will increase the likelihood of the particles hitting the instrument under the same flow conditions failed by the original tested GTS cylinder.</abstract><pub>Elsevier B.V</pub><doi>10.1016/S1001-6279(09)60012-3</doi><tpages>15</tpages></addata></record> |
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subjects | Bed load measurement Flume experiments Gravel streams Gravel transport sensors Numerical simulations 传感器 粒子碰撞 负荷测量 |
title | Evaluation of a gravel transport sensor for bed load measurements in natural flows |
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