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Physics · Ch 1 — Nature of Physical World and Measurement

Error Analysis

1.6.3

Error Analysis

Once nn repeated readings a1,a2,…,ana_1,a_2,\ldots,a_n of a quantity have been taken, the arithmetic mean am=1n∑iaia_m=\dfrac1n\sum_i a_i is treated as the best available estimate of the true value, and four related error measures are built from it.

i) Absolute error -- the magnitude of the difference between the mean (taken as the true value) and each individual reading:

∣Δa1∣=∣am−a1∣, ∣Δa2∣=∣am−a2∣, …, ∣Δan∣=∣am−an∣.|\Delta a_1|=|a_m-a_1|,\ |\Delta a_2|=|a_m-a_2|,\ \ldots,\ |\Delta a_n|=|a_m-a_n|.

ii) Mean absolute error -- the arithmetic mean of all the individual absolute errors:

Δam=∣Δa1∣+∣Δa2∣+⋯+∣Δan∣n=1n∑i=1n∣Δai∣.\Delta a_m=\frac{|\Delta a_1|+|\Delta a_2|+\cdots+|\Delta a_n|}{n}=\frac1n\sum_{i=1}^n|\Delta a_i|.

The true value is then quoted as lying between am+Δama_m+\Delta a_m and am−Δama_m-\Delta a_m, written a=am±Δama=a_m\pm\Delta a_m.

iii) Relative (fractional) error -- the ratio of the mean absolute error to the mean value itself:

Relative error=Δamam.\text{Relative error}=\frac{\Delta a_m}{a_m}.

It expresses how large the absolute error is compared to the size of the quantity being measured -- e.g. a speedometer reading 60 km h−1^{-1} when the true speed is 62 km h−1^{-1} has absolute error 22 km h−1^{-1} and relative error 2/60=0.0332/60=0.033.

iv) Percentage error -- the relative error expressed as a percentage:

Percentage error=Δamam×100%.\text{Percentage error}=\frac{\Delta a_m}{a_m}\times100\%.

A percentage error close to zero means the measurement is close to the target/true value -- good and acceptable. It is important to always understand why an error occurred: is it from the limits of the equipment, or from a mistake in how the experiment was carried out? …