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DESIGN OF RIPRAP FOR PROTECTION AGAINST. SCOUR ...

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

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

From this table, it is evident that Worman's method over predicts the size by about<br />

5 to 8 times, and Chiew's method gives 2 times larger size than that of observed in the<br />

experiments, where as in case of data collected in the present study it is 1.6 times<br />

(average) larger in comparison with observed size of rip rap.<br />

ANALYSIS <strong>OF</strong> <strong>RIPRAP</strong> TmCKNESS<br />

For studying the effectiveness of riprap in reduction of scour, the parameter C. =<br />

C a /C b has been calculated. Here C b is the value of constant obtained ill Kothyari et al.<br />

(1992) equation for scour in clear water studies, for non-uniform base material (Eq.<br />

(10».. .<br />

(87)<br />

(10)<br />

C is value of C when riprap was used and some scour was observed.<br />

~<br />

The ratio of C/C b called C. takes in to account the effect ofU, Y, opening ratio a<br />

and /1.Ys on scour and hence, it should be function of D,= dsJDso and T. = T/3cr. Dso<br />

related to rip rap layer and bed material size only. Thickness of riprap layer can be non<br />

dimensionalised by maximum size of the riprap material, which can be expressed as<br />

3. Dso. Anew term therefore, introduced and expressed as T. =T/3cr a D so ' where T<br />

is the thickness of the riprap layer, cr is the standard deviation of riprap mixture<br />

a .<br />

given by ~D84 /D 16 and Dso is median size ofriprap mixture. lfthe sizesin riprap are<br />

distributed normally, 99.73 percent values will be within the range ofD so± 3c •. Hence,<br />

3cra Dso is as good as maximum size of the riprap mixture when D100 is not known.<br />

The experimental data having eight ranges of D. starting from 0.045 and 0.78<br />

were plotted as C/C b Vs T. for respective range ofDiand the equation between them<br />

is obtained as<br />

C a _ C = 0.5 D~·98 T.- 2 . 50<br />

C b - • (ll)<br />

By assuming that at a value of C. as low as 0.05, riprap around the bridge pier will<br />

be stable. Hence, this equation can be solved for with this value for determining the<br />

thickness of riprap. Data collected by Worman (1989) and Chiew (1995) are used for<br />

the comparison of the thickness of riprap layer computed using Eq. (10). Figure 3<br />

shows the thickness of riprap layer used by these investigators in their experiments<br />

for zero scour condition and thickness computed using Eq. (11). The plot shows 86%<br />

of Worman's data points and 68 % ofChiew's data points fall within the error band of<br />

. '\<br />

ISH JOURNAL <strong>OF</strong> HYDR,AULIC ENGlNEERING, VOL. 16,2010, NO. 1_<br />

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