physicslab1

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Northeastern University *

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1152

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Chemistry

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Feb 20, 2024

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docx

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Report for Experiment #1 Measurement You name and stuff idk Abstract This experiment involved measuring cylinders with a ruler and scale, as well as measuring the background radiation count with a Geiger counter. The results from experiment one demonstrated the
linear relationship between mass and volume. The data from the Geiger counter was used to determine the FWHM and the standard deviation of the background radiation. Introduction A major source of error is the limit of precision of the instruments. In the instance of the scale, it only displays information up to the 10 th place in grams. This means that additional information measurement is lost. The greatest amount of lost information is .05 grams, because any larger than that, and it would round up to .1 grams which would be displayed. This is a source of random error due to lack of precision. In principle, random error is when repeated measurements produce different results under the exact same conditions. Systematic error is if there is an outside factor which constantly changes measurements. For example, if the scale was not zeroed, and dust weighing .2 grams fell on the scale, then each measurement would be .2 grams higher than the true value. Density is defined as the degree of compactness of a substance and is measured by the mass divided by the volume. Background radiation count rate is the radiation present in the natural environment, it comes from naturally occurring radioactive minerals. It is measured by detecting gamma rays, beta particles, and alpha particles. It is read in counts per minute. The goal of investigation 1 was to measure objects and model the mass and volume to observe the density. The goal of investigation 2 was to model the counts per minute of the Geiger counter to utilize standard deviation and histograms. Investigation 1 This experiment involved a digital scale, a ruler, and four cylinders. The diameter and length of each cylinder was measured with the ruler, and the weight was measured with the scale. The volume was then calculated with a standard equation. V = π D 2 L 4 Each scale was zeroed before measuring, however the mass recording still fluctuated due to dust on the scale. The weight displayed on the scale fluctuated within 1 gram before returning to the original weight displayed. There is the additional instrumental error which which created an imprecision in the data, which is displayed in the δm (g) row. This is the collected table with mass of the cylinder. Cylinder #1     #2     #3     #4
m ( g ) 23.0 21.2 11.9 4.6 δm ( g ) 0.05 0.05 0.05 0.05 δm/m 0.00217 0.00236 0.00420 0.0109 L ( cm ) 6.3 3.2 3.3 5 δL ( cm ) 0.05 0.05 0.05 0.05 δL/L 0.0079 0.017 0.015 0.010 D ( cm ) 1.2 1.5 1.1 0.6 δD ( cm ) 0.05 0.05 0.05 0.05 δD/D 0.042 0.033 0.045 0.083 V ( cm 3 ) 7.1 5.7 3.1 1.4 δV ( cm 3 ) 0.60 0.39 0.30 0.24 δV/V 0.084 0.068 0.092 0.17 ρ ( g/cm 3 ) 3.228 3.749 3.795 3.254 δρ ( g/cm 3 ) 0.05 0.05 0.05 0.05 δρ/ρ 0.01549 0.01334 0.01318 0.01537 The volume was calculated using the cylinder equation above. The errors were determined from the equation. δv v = ( 2 δD D ) 2 +( δL / L ) 2 The volume of the cylinders was also measured using the water immersion method. A volumetric flask was filled with 10ml water, then the cylinder was dropped into the flask, and the difference in ml was recorded. The results from the water volumetric are more accurate in principle than the first method because it relies on the water molecules enveloping the cylinder which is more precise than using a ruler. However, in this instance the results were nearly identical. The density of the cylinder was calculated by diving the weight by the volume. g cm 3 The error was calculating by dividing the instrumentation error, .05, by the density. Displayed is the graph directly copied from excel.
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