Distribution of Measured Values
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To explore the range over which a measured value is distributed, we repeat measurements. When fluctuations in measurements are dominated by random events that are mutually independent, repeated values measured for y describe a Gaussian distribution about their mean value ym:
![f(y) \ = \ \frac {1}{s\sqrt{2\pi}} \exp \left [ \frac {-(y - y_m)^2}{2s^2} \right]](/w/images/math/f/6/4/f64678b0f6d09e6864bd5a4421d2d30c.png)
This is sometimes called the normal distribution, because it is the one that normally occurs. In (1) the quantity s is called the standard deviation; it measures the width of the distribution f(y), as in Figure 1. For N repeated measurements, yi (i = 1, 2, ... , N), it is computed by

Physically, the sum of the squares of the deviations in (2) is proportional to the "noise" in the N measurements, while N is proportional to the "strength" of the signal represented by the average ym; therefore, the standard deviation in (2) is inversely proportional to the signal-to-noise ratio:[1]

Consequently, large values of s imply a relatively large amount of noise—measured values are widely scattered about their mean. We attempt to increase the signal-to-noise ratio by increasing N. Note that if we make only one measurement (N = 1), then (2.5) gives s = 0/0; that is, a single measurement gives us no information about the width of the distribution.
If we integrate portions of the Gaussian, we obtain the number of values that lie within a specified distance from the mean. In particular, we find that, as in Figure 2,
- 68.3% of the measured values lie within ±1s of the mean ym,
- 95.5% lie within two standard deviations ±2s of ym, and
- 99.7% lie within three standard deviations ±3s of ym.
Note in Figure 2 that the maximum in the Gaussian distribution occurs at the mean value; that is, the mean is the most probable value—the value most likely to be measured.
Reference
- ↑ J. M. Haile, Analysis of Data, Macatea Productions, Central, SC, 2003. ISBN 0-9728602-0-7.



