Rogue data points
In a set of measurements subject to
random error, measurements with a very large error sometimes occur at random
and unpredictable times, where the magnitude of the error is much larger than
could reasonably be attributed to the expected random varia[1]tions in
measurement value. Sources of such abnormal error include sudden transient
voltage surges on the mains power supply and incorrect recording of data (e.g.
writing down 146.1 when the actual measured value was 164.1). It is accepted
practice in such cases to discard these rogue
measurements, and a threshold level
of a š3 deviation is often used to determine what should be discarded. It
is extremely rare for measure[1]ment errors to
exceed š3 limits when only normal random effects are affecting the
measured value.
Special case when the number of
measurements is small
When the number of measurements of a
quantity is particularly small and statistical analysis of the distribution of
error values is required, problems can arise when using standard Gaussian
tables in terms of z as defined in equation (3.16) because the mean of only a small
number of measurements may deviate significantly from the true measure[1]ment value. In
response to this, an alternative distribution function called the Student-t
distribution can be used which gives a more accurate prediction of the error
distribution when the number of samples is small. This is discussed more fully
in Miller (1990).
3.6 Aggregation of measurement system
errors
Errors in measurement systems often
arise from two or more different sources, and these must be aggregated in the
correct way in order to obtain a prediction of the total likely error in output
readings from the measurement system. Two different forms of aggregation are
required. Firstly, a single measurement component may have both systematic and
random errors and, secondly, a measurement system may consist of several
measurement components that each have separate errors.
3.6.1 Combined effect of systematic
and random errors
If a measurement is affected by both
systematic and random errors that are quantified as ±x (systematic errors) and ±y
(random errors), some means of expressing the combined effect of both types of
error is needed. One way of expressing the combined error would be to sum the
two separate components of error, i.e. to say that the total possible error is
e = ±(x + y). However, a more usual course of action is to express the likely
maximum error as follows:
It can be shown (ANSI/ASME, 1985)
that this is the best expression for the error statistically, since it takes
account of the reasonable assumption that the systematic and random errors are
independent and so are unlikely to both be at their maximum or minimum value at
the same time.
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