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<br />. <br /> <br />796 <br /> <br />HYDRAULIC ENGINEERING '94 <br /> <br />their survival rates (Shirazi and Selm 1981; Helfrich et. <br />a1. 1986). In order to accomplish this, it is <br />necessary to sample the different sediment composition~ <br />in an eff laient and unbiased manner. Wolcott and Churcr <br />(1991) addressed this issue and proposed that a sampl~ <br />representative of the entire region could be obtained b'. <br />taking sUbsamples of equal volumes and combining the; <br />into one sample. Based on the results of an empirica: <br />test they provide some guidelines and accuracy levels of <br />such a sample. This paper suggests that in the future. <br />similar approach may be possible using grid by number <br />samples. Such a method would have a statistical basis <br />and require less material to be sampled for the Same <br />accuracy levels. This paper will briefly discuss some 01 <br />the statistical properties and sample sizes of grid b) <br />number samples. <br /> <br />Aoouraov of Grid samDles <br /> <br />Fripp and oiplas (1993), among others, assumed that <br />the results of grid by number sampling are adequatel~' <br />described by the binomial distribution. They ther. <br />proceeded to calculate the accuracy level at which a <br />gi ven particle size is sampled, based on the number of <br />stones taken. Confidence intervals can then be given in <br />percent of the entire grain size distribution. A <br />computer program developed to simulate grid by number <br />sampling is employed here to check the validity of this <br />assumption. <br /> <br />Diplas and Sutherland (1988) found that the <br />following two properties applied to surface material: <br />"(1)On a sediment surface, each grain on average, <br />projects an area proportional to the square of its sieve <br />diameter; and (2) a size fraction occupying p% of the <br />volume of solids will occupy p% of the sample surface <br />area occupied by grains." Using these properties, a <br />computer can randomly select samples from a def ined <br />volumetric distribution to examine if the accuracy levels <br />of the sample do indeed correspond to a binomial <br />distribution as Fripp and Diplas (1993) suggest. In this <br />case, the selected distribution contained particle sizes <br />from 10 mm to 160 mm in increments of 10 mm while sieve <br />sizes ranged from 5 mm to 165 mm in increments of 10, <br />This was chosen out of convenience, but seems appropriate <br />since it is common practice in sieve analysis to lump the <br />particles between two sieve sizes into a single size <br />corresponding to the geometric mean of two adjacent sieve <br />sizes. <br /> <br />The accuracy of samples containing 45, 100 and 200 <br />.~.. -<< ......M " '""'" '" ...".. "' ... L <br /> <br />. <br /> <br />. <br /> <br />BENEFITS OF NUMBER SAMPLING <br /> <br />797 <br /> <br />sam ling intensity and calculatin9 their median ~alues <br />.1ndPdetermlnlng how many fell outSIde th.e 95% con~ldence <br />t rval calculated from the method prOVIded by Frlpp and <br />~~p~as (1993). For samples of 45 stones, 3.33% fell <br />t 'de this range while for 100 stones, 1 to 2% fell <br />0\.1 S1 " f th 1 <br />t ide the conf ldence Interval. None 0 e samp es <br />~~t~ 200 stones fell outside this region. These ~esu~ts <br />bout what we would expect and support the bInomIal <br />~~:t~ibution assumption. Figures 1 and 2 show sample <br />./ tributions obtained with 45 stones and 200 stones <br />~s tted beside the volumetric distribution and i~s 95% <br />p ofidence limits. The first figure shows that whIle at <br />c~n stones the median values stay within the co~fidence <br /><l tervals the distributions waiver and fall outSIde this <br />~~qion ne~r the t~ils. F~gure 2, h~we~er, shOWS t~at at <br />;00 stones the dIstributIons are WIthIn the conf1dence <br />Intervals and do ~ot waver back and forth nearly as much <br />as in the first fIgure. Samples taken at 100 stones, not <br />hown here are not as smooth as the 200 samples, but a~e <br />~etter nea~ the ends than obtained with ~5 sto~es. Th~S <br />phenomenon can be explained bY referencIng f 19u~e 2, In <br />rripp and oiplas (1993) which shows that for the bInomIal <br />distribution to be valid in obtaining the sam~ accuracy <br />levels near the tails, more stones are requlr.ed,' For <br />example, the binomial method is valid in deSCrIbIng the <br />accuracy level of 090 or 010 only when there are 200 or <br />~ore stones in the sample while 40 or more stones ~re <br />required to compute the accuracy level for the med1an <br />grain size (Fripp and Oiplas 1993). <br /> <br />Siz. of Grid samDles <br /> <br />Fripp and Diplas' (1993) figure 5 shows ~hat a grid <br />sample with 400 stones is equivalent to ~e VrIes' (~971) <br />low accuracy requirements for volumetrIc sample SIzes. <br />If we assume that the sieve diameter is close to the <br />nominal diameter of a particle and that 084 can be used <br />to calculate the average grain volume for the entire <br />distribution, as De Vries (1971) indicates, we c~n <br />compare the mass of a 400 stone sample,to ~he volumetrIc <br />sample mass. De vries' low accuracy crIterIon recom~ends <br />sample masses of about 136 kg and 458 kg for sedIment <br />deposits with 0 4 of 40 mm and 60 mm, respectively. ^ <br />sample of 400 stones for the same sediments res~lts in <br />volumes of about 36 kg and 120 kg, or about one thIrd the <br />size of those recommended by De Vries. <br /> <br />" <br />