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<br />2 <br /> <br />TECHNIQUES OF WATER-RESOURCES INVESTIGATIONS <br /> <br />. <br /> <br />frequencies indicates that the binomial distri- <br />bution is applicable to this problem. <br /> <br />Table <br /> <br />1.-Results of dice-tossing <br />[After Kendall (19.52)] <br /> <br />experiment <br /> <br />~o. of <br />sixes <br /> <br />Fre- <br />quency <br /> <br />Relative <br />frequency <br /> <br />Theoretical <br />relative <br />frequency <br /> <br />0____________ 447 0.109 0.112 <br />L___________ 1, 145 .280 .269 <br />2____________ 1, 181 .2S8 .296 <br />3____________ 796 .194 .197 <br />4____________ 380 .093 .089 <br />5____________ 115 .028 .029 <br />6____________ 24 .006 .007 <br />7 and over____ 8 .002 .001 <br />TotaL-___ __ 4,096 1.00 1. 00 <br /> <br />The binomial distribution is a discrete dis- <br />tribution, that is, it can take values only at <br />specific points along a scale. In the dice-tossing <br />experiment, it is possible to obtain an integer <br />number of sixes only; there is no such thing as <br />5.5 or 3.2 sixes. <br />More commonly, a variable may take any <br />value along a scale. Such a variable and its <br />distribution are known as continuous. A <br />variable may be classified as continuous :if it <br />can take any value along a scale even though <br />the limitations of measurement restrict the <br />observations to discrete values. This condition <br />exists with most natural phenomena. <br />To aid in understanding a distribution, con- <br />sider 1,000 tree-ring indices ranging in size from <br />2 to 240. If these are grouped by six-unit in- <br />orements of size, a histogram, or frequency <br />distribution, is obtained (fig. 1). The irregu- <br />larity of the profile of this distribution is due <br />to the small (in a statistical sense) number of <br />indices used in its preparation. The greater the <br />number used, the smoother would be the profile <br />of the frequency distribution. If the number of <br />observations approaches infinity and the size <br />increment approaches zero, the enveloping line <br />of the frequency distribution will approach a <br />smooth curve. Then if the ordinate values are <br />divided by a number such that the area under <br />the curve becomes one, the resulting curve is a <br />probability density curve, or probability dis- <br />tribution, such as figure 2. The process just <br />described requires the additional assumption <br />that the variable can take any value within the <br /> <br />range, that the variable is continuous, not <br />discrete. <br />80 <br /> <br />if> <br />W <br />~ 60 <br />o <br />.-: <br />040 <br />0: <br />'" <br />'" <br />" 20 <br />=> <br />z <br /> <br /> <br />o <br />o 30 60 90 120 150 180 210 240 <br />WIDTH INDEX <br /> <br />Figure 1.-Histogram, or frequency distribution, of 1,000 <br />tree-ring indices. <br /> <br />, <br /> <br />>- <br />$' <br />z <br />w <br />o <br />>- <br />f- <br />:J <br />in <br /><< <br />'" <br />o <br />0: <br />CL <br /> <br /> <br />240 <br /> <br />o <br /> <br />I <br />30 60 90 120 150 <br />WIDTH INDEX <br /> <br />. <br /> <br />Figure 2.-Probobility density curve of 1,000 tree-ring <br />indices. <br /> <br />A theoretical probability distribution de- <br />scribes the relation between size (or some other <br />other characteristic) and probability. For this <br />relation to be valid, the individuals must oceur <br />randomly or be drawn randomly. The size of <br />any individual drawn should not depend on <br />the size of anyone previously drawn. Probabil- <br />ity, in the concept of frequency distributions, <br />is defined as relative frequeney. The distribu- <br />tion of the number of sixes obtained from re- <br />peated tosses of 12 dice may be illustrated by <br />plotting the theoretical relative frequencies of <br />table 1. The relati ve frequencies of each of the <br />6-unit increments in figure 1 could likewise be <br />computed. In the first of these examples, a <br />probability is associated with each possible <br />outcome. In the second, a probability i~ assoei- <br />ated with eaeh increment of size; here the <br />probability is of obtaining not a specific indi- <br />vidual but any individual within the increment <br />of size. This interpretation is required for con- <br />tinuous distributions because there is an infinite <br />number of possible valnes and, thus, no proba- <br />bility of occurrence of a particular individual. <br /> <br />. <br />