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<br />Test results showed definite fluctuations in both gages, with <br />maximum departures from the starting point of 0.010 and 0.015 <br />inch respectively. These are illustrated in Figures 17 and <br />18 in Appendix A. The departures were in opposite directions <br />for the two gages; one gage showed an increase from the <br />starting point at about the halfway point in the test. After <br />that time, the traces gradually converged towards the <br />starting point. Both units were within 0.005 inch of the <br />initial point at the end of the test period. The source of <br />these deviations is unknown but it is apparent that <br />precipitation totals from storm events of one-half day or <br />longer duration could be subject to errors of approximately <br />0.01 inch if these gages are typical. <br /> <br />i <br />I <br /> <br />( <br />" <br />I <br /> <br />3. Storm total accuracy. <br /> <br />Each of the tests in which simulated precipitation was <br />added to the beaker within the gage bucket allowed a precise <br />comparison between the "true" catch and that indicated on the <br />chart record. The collection beaker (with evaporation <br />suppressant) was weighed to the nearest 0.1 g before each <br />trial, and then re-weighed with the collected water after the <br />conclusion of each day's tests. Tests conducted before gage <br />trials disclosed that for the evaporation suppressant and <br />beakers used, evaporation losses were negligible over time <br />periods far exceeding those between weighings. Thus, any <br />discrepancies between the weighed accumulation in the beakers <br />and the chart readings are not due to evaporation. <br /> <br />In the initial tests the rise in the chart trace seemed <br />to lag behind that expected from the calculated input flow <br />rate. This suggested that perhaps hysteresis was occurring <br />in the gage mechanism. Consequently, with most later tests <br />(beginning on 18 November 1982) the chart cylinders were not <br />removed from the drives and the collection beakers were not <br />taken from the buckets and weighed until the morning after <br />the final test flow was ended. This allowed more time for <br />the hysteresis to correct itself. In addition, just before <br />the beaker and the chart were .removed, the gage bucket <br />platform was tapped with a pencil to remove any remaining <br />frictional drag in the mechanism. <br /> <br />The indicated chart levels were then determined for the <br />following times: (1) at the immediate end of simulated <br />precipitation input; (2) after several hours of zero <br />precipitation input; and (3) after the mechanism was tapped. <br />Results are presented in Table 3. It can be seen that, on <br />the average, the gages consistently undermeasured for all <br />three measurement times. The average undermeasurement at the <br />point simulated precipitation input was ended was 0.017 <br />inch. The data suggest that the error increases with total <br />precipitation amount, but additional trials would be required <br />to confirm this. This level of accuracy is quite im~ressive, <br />as it implies that the basic gage is capable of prov1ding <br /> <br />10 <br />