Random Error - Quantitative Analysis - Lecture Slides, Slides of Analytical Chemistry

This course is for chemistry students. Many methods for Quantitative Analysis are explained in this course. This lecture is about: Random Error, Nature of Random Errors, Sources of Random Errors, Thermometer, Viscosity of the Liquid, Samples and Populations, Systematic Error, Population Standard Deviation, Gaussian Curve, Sample Standard Deviation

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2012/2013

Uploaded on 09/26/2013

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Random Error
The Nature of Random Errors
Random, or indeterminate, errors occur whenever a
measurement is made. This type of error is caused by the
many uncontrollable variables that are an inevitable part of
every physical or chemical measurement. There are many
contributors to random error, but often we cannot
positively identify or measure them because they are small
enough to avoid individual detection. The accumulated
effect of the individual random uncertainties, however,
causes the data from a set of replicate measurements to
fluctuate randomly around the mean of the set.
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Random Error

The Nature of Random Errors

Random, or indeterminate, errors occur whenever a

measurement is made. This type of error is caused by the

many uncontrollable variables that are an inevitable part of

every physical or chemical measurement. There are many

contributors to random error, but often we cannot

positively identify or measure them because they are small

enough to avoid individual detection. The accumulated

effect of the individual random uncertainties, however,

causes the data from a set of replicate measurements to

fluctuate randomly around the mean of the set.

Three dimensional plot showing absolute error

Frequency distribution

Range of measured values, mL

Sources of Random Errors

Sources of random uncertainties in the calibration of a pipet include (1) visual judgments, such as the level of the water with respect to the marking on the pipet and the mercury level in the thermometer; (2) variations in the drainage time and in the angle of the pipet as it drains; (3) temperature fluctuations, which affect the volume of the pipet, the viscosity of the liquid, and the performance of the balance; and (4) vibrations and drafts that cause small variations in the balance readings. Undoubtedly, numerous other sources of random uncertainty also operate in this calibration process. It is difficult or impossible to determine the influence of any one of the random errors arising from these variables, but the cumulative effect is responsible for the scatter of data points around the mean.

Normal error curves

Samples and Populations

A finite number of experimental observations is

called a sample of data. The sample is treated as a

tiny fraction of an infinite number of observations

that could in principle be made given infinite time.

Statisticians call the theoretical infinite number of

data a population , or a universe , of data. Statistical

laws have been derived assuming a population of

data; often, they must be modified substantially

when applied to a small sample because a few data

points may not be representative of the population.

…continued…

To emphasize the difference between the two

means, the sample mean is symbolized by x and

the population mean by . When N is small, x

differs from  because a small sample of data does

not exactly represent its population. The probable

difference between x and  decreases rapidly as

the number of measurements making up the

sample increases; ordinarily, by the time N reaches

20 to 30, this difference is negligibly small.

The Population Standard Deviation()

The population standard deviation , which is a measure of

the precision or scatter of a population of data, is given by the equation

where, N is the number of data points making up the population.

The two normal error curves in Fig. 6-4 are for two populations of data that differ only in their standard deviations. The standard deviation for the data set yielding the broader but lower curve B is twice that for the measurements yielding curve A. the breadth of these curves is a measure of the precision of the two sets of data. Thus, the precision of the data leading to curve A is twice as good as that of the data that are represented by curve B.

  

 

 

x

N

i i

N

1

2

Areas under a Gaussian Curve

It can be shown that, regardless of its width,

68.3% of the area beneath a Gaussian curve for

a population of data lies within one standard

deviation ( 1 ) of the mean . Thus, 68.3% of

the data making up the population will lie

within these bounds. Furthermore,

approximately 95.4% of all data points are

within  2  of the mean and 99.7% within  3 .

Sample Standard Deviation

Standard Deviation equation must be modified when it is applied to a small sample of data. Thus, the sample standard deviation s is given by the equation

This equation differs from the standard deviation equation in two ways. First, the sample mean, x, appears in the numerator of sample standard deviation equation in place of the population mean, . Second, N in standard deviation equation is replaced by the number of degrees of freedom (N – 1).

The sample variance s^2 is also of importance in statistical calculations. It is an estimate of the population variance ^2.

 

 

 x^ x 

N

d

N

i i

N i i

N

1 1 1 1

(^22)

_