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Principles of Laboratory Practice

Statistical Analysis of Experimental Data

Physics I 192 words Free to read

When you repeat a measurement NN times, statistics summarises the results.

Mean (best estimate):

xˉ=1Ni=1Nxi\bar{x} = \frac{1}{N}\sum_{i=1}^N x_i

Standard deviation (spread of individual measurements):

s=1N1i=1N(xixˉ)2s = \sqrt{\frac{1}{N-1}\sum_{i=1}^N (x_i - \bar{x})^2}

Standard error of the mean (uncertainty in xˉ\bar{x}):

σxˉ=sN\sigma_{\bar{x}} = \frac{s}{\sqrt{N}}

Key relationships

QuantityWhat it measures
ssSpread of the data
σxˉ\sigma_{\bar{x}}Uncertainty in the mean
NNMore repeats \to smaller σxˉ\sigma_{\bar{x}}

Gaussian distribution — For many random errors, measurements follow a bell curve where 68%\approx 68\% of values lie within xˉ±s\bar{x} \pm s and 95%\approx 95\% within xˉ±2s\bar{x} \pm 2s.

Outlier detection — A point more than 3s3s from the mean is suspicious. Use Chauvenet's criterion or the Grubbs test to decide whether to reject it.

Tip: Increasing NN from 4 to 16 halves the standard error. But going from 100 to 400 only halves it again — diminishing returns set in.
Common pitfall: The standard deviation describes the scatter of single readings; the standard error (σ/N\sigma/\sqrt{N}) describes the reliability of the mean. Quoting the wrong one misstates your precision by a factor of N\sqrt{N}.
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Principles of Laboratory Practice