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DESIGN OF RIPRAP FOR PROTECTION AGAINST. SCOUR ...

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I<br />

II<br />

VOL. 16, (No.1) <strong>DESIGN</strong> <strong>OF</strong> <strong>RIPRAP</strong> <strong>FOR</strong> PROTECfION <strong>AGAINST</strong><br />

(83)<br />

<strong>SCOUR</strong> AROUND BRIDGE PIER<br />

.,<br />

1. Incipient Scour of bed material around the pier<br />

2. Incipient scour of riprap of different size and thickness<br />

3. Scour with riprap protection.<br />

Over 150 runs were conducted using circular pier of 50 mrn diameter under clear<br />

water condition. Table 1 gives standard deviation, size of bed and riprap material<br />

tested in the experiments. The circular ring with engraved marking in nun was used to<br />

lay riprap of appropriate thickness and flush with original bed level, Bed material of<br />

predetermined thickness was removed from scoured area, weighed and riprap of same<br />

weight was then slowly added to the scour hole and levelled to the undisturbed bed<br />

level.<br />

In addition to the data collected in the present study, data collected by Knight<br />

(1975), Dey (1995), Chiew (1995), Melville (1997),ha:ve also been used for<br />

determining DIU c for incipient scour and those by Worman (1989) and Chiew (1995)<br />

for size and thickness of riprap layer. Worman (1989) had used three bed materials of<br />

median diameter 0.17,0.36 and 0.78 mm and five ripraps of size varying from 8 to 48<br />

mm. Depth of the flow varied from 300 to 400 mm whereas Chiew (1995) used bed<br />

material of mean size 0.96 mm and three riprap of size 2.60, 4 and 4.85 mm.<br />

TABLE-l<br />

CHARACTERISTICS <strong>OF</strong> BED AND <strong>RIPRAP</strong> MATERIAL<br />

(pRESENT STUDy)<br />

ANALYSIS <strong>OF</strong> DATA<br />

Bed Material Riprap Material<br />

d so (mm) 0'& Dso(mm) O'g<br />

0.20 2.45 1 1.37<br />

0.27 2.69 2. 1.90 .<br />

0.36 1.28 3 2.36<br />

0.40 2.53 4 2.50<br />

0.50 2.63 5 2.66<br />

0.68 2.73 8 1.58<br />

Limiting values ofUfUcfor Incipient Scour<br />

The critical velocity at which sediment of a given size will just move in an<br />

un~bstructed uniform flow was obtained by combining Shields' and Yalin-Karman<br />

relationship with Karman-Prandl's equation of Diu. in hydro-dynamically smooth<br />

and rough channels. Analyzing the generated data, following type of equation was<br />

obtained.<br />

(:;::X~:~~~~P:~::;:;'~~1::r~7:??·:·;·'·~:·?::;·::;·:·;<br />

>::. :::;:.:-:;~:: ;.::::~:::::. :':":"::~,, ::.' ~=:' . .'::'"'::'~:<br />

ISH JOURNAL <strong>OF</strong> HYDRAULIC ENGINEERING, VOL 16,2010, NO. I<br />

:.:;.:.;:.:~-y.:..:>~.?::~.:':;::::;:::::;:.::.:.:...;:::, ..... :..... : .. :.,,: ::.:':.::.::,::.. ::: ::.:::.: ... :;::::.... :.::::'::: ::::-, :::;: .. :.: '.: -:: : .::.:<br />

..>:-....~ .':.~-~".~: ~;~:~:.':' :'~..-::;

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