A bucket filled with water to a height h has a blocked hole on the bottom. The measurements of both the height h and the height of the hole from the bottom of the bucket is measured. Taking th difference between these two measurements gives the height of the hole to the surface of water. Measuring as accurately as possible, the height h is 13.6 cm and the height from the bottom is 2.5 cm both with an uncertainty of +- .05 cm giving the height from the hole to the surface of the water as 11.1 cm +- .10 cm. The diameter of the hole is measured again as accurately as possible giving a value of .55 cm +- .05 cm. The area of that hole can then be calculated by taking half the diameter, squaring it, then multiplying by pi.
Using the volume emptied 400 mL, area of drain hole 2.38 * 10^-5 m/s, acceleration due to gravity 9.8 m/s/s, and height of water 11.1 cm, the theoretical time taken given by:
Even using the values of uncertainty, the experimental values did not agree with the theoretical values entirely. All the time difference errors were near 1 to 4 seconds uncertainty did not calculate to be that great. To correct this problem a greater value of uncertainty should be estimated. Fluid experiments seem to have larger uncertainty than some branches of physics because the exact volume measured is more difficult to catch precisely. Other main uncertainties come from reaction time of starting the stopwatch and stopping it since this requires two people. The biggest form of uncertainty comes from the inaccurate volume measurement since water is flowing fairly quickly and it is less obvious to tell what the volume is precisely. The beaker itself has an uncertainty when filling up because of how precise the beaker is constructed. Many beakers, graduated cylinders, and other glassware contain an uncertainty and it is printed on the glassware. For example 500 mL +-.5 mL.
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