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Measurement figures Uncertainty

Significant figures are also important because they guide us in reporting the result of an analysis. When using a measurement in a calculation, the result of that calculation can never be more certain than that measurement s uncertainty. Simply put, the result of an analysis can never be more certain than the least certain measurement included in the analysis. [Pg.14]

The convention of significant figures automatically gives an indication of the uncertainty in a measurement. The uncertainty in the last number (the estimated number) is usually assumed to be 1 unless otherwise indicated. For example, the measurement 1.86 kilograms can be interpreted to mean 1.86 0.01 kilograms. [Pg.1079]

To learn to indicate a measurement s uncertainty by using significant figures... [Pg.133]

Here, I provide a brief review of the methods developed in constructing RSDI. The point here is not to decide which approach techniques to use or to say which approach appears to be the best combinations of the indicators and weights or to say that the objective approaches are in some way meaningful methods or better than subjective approaches. Rather, to show the differences (uncertainty) of these RSDI results from all approaches. There are some special statistical tools used to measure the uncertainty and sensitivity of the input data in contribution to the output variance, for example the uncertainties analysis method (UA) and sensitivity analysis (SA) a review of these methods is available in Saisana et al. (2005). Due to the small sample size and the nature of data used in this study, a simple method in comparing the RSDI approaches and results is presented in Table 5.6 and Figure 5.9. [Pg.82]

Measured value Precision of measurement Random uncertainty In the measurement Significant figures of measured value... [Pg.391]

Intervening variables mediation between the independent and dependent variables. An intervening variable is one that - as its name implies - intervenes between the independent variables that we manipulate and die dependent variables that we measure. When 1 described the effects of uncertainty on reaction time, I also used die term expectancy. In fact, to understand the relationship we posit a psychological, unobservable term that we believe intervenes between the independent and dependent variables. We assume that the physical measure of uncertainty is related to the unobservable variable of expectancy. Expectancy, in turn, is assumed to directly affect the dependent variable. Thus, the vertical chain of independent intervening dependent variables in Figure 2-1 constitutes the basic relationships that are the focus of most experimental research. [Pg.25]

The parameter determined by integration of the stress/strain history is the critical thermomechanical conversion factor, fic- As noted both in experiments [5] and in simulations [6], drawing is destabilised at a temperature of 50-60°C, i.e. within the range for which data were measured. Figure 4 shows that despite experimental and analytical uncertainties provides a very effective index for the plane stress fracture resistance Wpi they are related by a monotonic and, indeed, quite linear relationship. Figures 5 and 6 illustrate the robusmess of the procedure in that neither the initial temperature of the simulation nor the strain rate chosen to characterise plane stress separation unduly influences the result. [Pg.1625]

In this approach one uses narrow-band continuous wave (cw) lasers for continuous spectroscopic detection of reactant and product species with high time and frequency resolution. Figure B2.5.11 shows an experimental scheme using detection lasers with a 1 MFIz bandwidth. Thus, one can measure the energy spectrum of reaction products with very high energy resolution. In practice, today one can achieve an uncertainty-limited resolution given by... [Pg.2128]

Figure B2.5.11. Schematic set-up of laser-flash photolysis for detecting reaction products with uncertainty-limited energy and time resolution. The excitation CO2 laser pulse LP (broken line) enters the cell from the left, the tunable cw laser beam CW-L (frill line) from the right. A filter cell FZ protects the detector D, which detennines the time-dependent absorbance, from scattered CO2 laser light. The pyroelectric detector PY measures the energy of the CO2 laser pulse and the photon drag detector PD its temporal profile. A complete description can be found in [109]. Figure B2.5.11. Schematic set-up of laser-flash photolysis for detecting reaction products with uncertainty-limited energy and time resolution. The excitation CO2 laser pulse LP (broken line) enters the cell from the left, the tunable cw laser beam CW-L (frill line) from the right. A filter cell FZ protects the detector D, which detennines the time-dependent absorbance, from scattered CO2 laser light. The pyroelectric detector PY measures the energy of the CO2 laser pulse and the photon drag detector PD its temporal profile. A complete description can be found in [109].
There are a few basic numerical and experimental tools with which you must be familiar. Fundamental measurements in analytical chemistry, such as mass and volume, use base SI units, such as the kilogram (kg) and the liter (L). Other units, such as power, are defined in terms of these base units. When reporting measurements, we must be careful to include only those digits that are significant and to maintain the uncertainty implied by these significant figures when transforming measurements into results. [Pg.33]

Units are cm throughout. Measurements are of band heads, formed by the rotational stmcture, not band origins. Figures in parentheses are differences variations in differences (e.g. between the first two columns) are a result of uncertainties in experimental measurements. [Pg.251]


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Uncertainty in Measurement Significant Figures

Uncertainty in Measurement and Significant Figures

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