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Chapter 7
Statistical Data Treatment
and Evaluation
Experimentalist use statistical calculations to sharpen
their judgments concerning the quality of experimental
measurements. These applications include:
• Defining a numerical interval around the mean of a set
of replicate analytical results within which the
population mean can be expected to lie with a certain
probability. This interval is called the confidence
interval (CI).
• Determining
the
number
of
replicate
measurements required to ensure at a given
probability that an experimental mean falls
within a certain confidence interval.
• Estimating the probability that (a) an
experimental mean and a true value or (b) two
experimental means are different.
• Deciding whether what appears to be an outlier
in a set of replicate measurements is the result of
a gross error or it is a legitimate result.
• Using the least-squares method for constructing
calibration curves.
CONFINENCE LIMITS
_
Confidence limits define a numerical interval around x
that contains  with a certain probability. A confidence
interval is the numerical magnitude of the confidence
limit. The size of the confidence interval, which is
computed from the sample standard deviation, depends
on how accurately we know s, how close standard
deviation is to the population standard deviation .
Finding the Confidence Interval when s Is a Good
Estimate of 
A general expression for the confidence limits (CL) of a
single measurement
_
CL = x  z
For the mean of N measurements, the standard error of
the mean, /N is used_ in place of 
CL for  = x  z/N
Finding the Confidence Interval when  Is
Unknown
We are faced with limitations in time or the
amount of available sample that prevent us from
accurately estimating . In such cases, a single
set of replicate measurements must provide not
only a mean but also an estimate of precision. s
calculated from a small set of data may be quite
uncertain. Thus, confidence limits are necessarily
broader when a good estimate of  is not
available.
…continued…
To account for the variability of s, we use the important
statistical parameter t, which is defined in the same way as
z except that s is substituted for .
t = (x - ) / s
t depends on the desired confidence level, but t also
depends on the number of degrees of freedom in the
calculation of s. t approaches z as the number of degrees
of freedom approaches infinity.
_
The confidence limits for the mean x of N replicate
measurements can
be calculated from t by an equation
_
CL for  = x  ts/N
Comparing an Experimental Mean with the True
Value
A common way of testing for bias in an analytical method
is to use the method to analyze a sample whose
composition is accurately known. Bias in an analytical
method is illustrated by the two curves shown in Fig. 7-3,
which show the frequency distribution of replicate results
in the analysis of identical samples by two analytical
methods. Method A has no bias, so the population mean
A is the true value xt. Method B has a systematic error, or
bias, that is given by
bias = B - xt = B - A
bias effects all the data in the set in the same way and that
it can be either positive or negative.
…continued…
_
The difference x – xt is compared with the difference that
could be caused by random error. If the observed
difference is less than that computed _ for a chosen
probability level, the null hypothesis that x and xt are the
same cannot be rejected. It says only that whatever
systematic error is present is so small
that it cannot be
_
distinguished from random error. If x –xt is significantly
larger than either the expected or the critical value, we
may assume that the difference is real and that the
systematic error is significant.
The critical value for rejecting the null hypothesis is
calculated by _
x – xt=  ts /N
Comparing Two Experimental Means
The results of chemical analyses are frequently used to
determine whether two materials are identical. The chemist
must judge whether a difference in the means of two sets of
identical analyses is real and constitutes evidence that the
samples are different or whether the discrepancy is simply a
consequence of random errors in the two sets. Let us assume
that
N1 replicate analyses of material 1 yielded a mean value of
_
x1 and that N2 analyses of
_ material 2 obtained by the same
method gave a mean of x2. If the data were collected in an
identical way, it is usually safe to assume that the standard
deviations of two sets of measurements are the same.
We invoke the null hypothesis that the samples_ are_identical
and that the observed difference in the results, (x1 – x2), is the
result of random errors.
…continued…
_
The standard deviation of the mean x1 is
sm1 
s1
N1
sm2 
s2
N2
_
and like wise for x2,
_
_
Thus, the variance s2d of the difference (d = x1 – x2)
between the means is given by
s2d = s2m1 + s2m2
…continued…
By substituting the values of sd, sm1, and sm2 into
this equation, we have
2
2
 sd 
 sm1 
 sm2  2

  
  

 N
 N1 
 N2 
If we then assume that the pooled standard
deviation spooled is a good estimate of both sm1 and
sm2, then
2
2
2
2  N1  N 2
 sd 
 spooled 
 spooled 


  
  
 = s pooled 
 N 1N 2 
 N
 N1 
 N2 
and
1/2
 sd 
 N1  N 2


 = s pooled 
 N 1N 2 
 N
Substituting this equation, we find that
_ _
N1  N 2
x1  x 2   tspooled
N 1N 2
_ _
or the test value of t is given by
x1  x 2
t
N1  N 2
spooled
N 1N 2
We then compare our test value of t with the critical value
obtained from the table for the particular confidence level
desired. If the absolute value of the test statistic is smaller
than the critical value, the null hypothesis is accepted and
no significant difference between the means has been
demonstrated. A test value of t greater than the critical
value of t indicates that there is a significant difference
between the means.
DETECTING GROSS ERRORS
A data point that differs excessively from the mean in a
data set is termed an outlier. When a set of data contains
an outlier, the decision must be made whether to retain or
reject it. The choice of criterion for the rejection of a
suspected result has its perils. If we set a stringent
standard that makes the rejection of a questionable
measurement difficult, we run the risk of retaining results
that are spurious and have an inordinate effect on the mean
of the data. If we set lenient limits on precision and
thereby make the rejection of a result easy, we are likely to
discard measurements that rightfully belong in the set,
thus introducing a bias to the data. No universal rule can
be invoked to settle the question of retention or rejection.
Using the Q Test
The Q test is a simple and widely used statistical
test. In this test, the absolute value of the
difference between the questionable result xq and
its nearest neighbor xn is divided by the spread w
of the entire set to give the quantity Qexp:
xq  xn
xq  xn
Q exp 

w
xhigh  xlow
This ratio is then compared with rejection values
Qcrit found in Table. If Qexp is greater the Qcrit, the
questionable result can be rejected with the
indicated degree of confidence.
1.
2.
3.
4.
5.
How Do We Deal with Outliers?
Reexamine carefully all data relating to the outlying
result to see if a gross error could have affected its
value.
If possible, estimate the precision that can be
reasonably expected from the procedure to be sure that
the outlying result actually is questionable.
Repeat the analysis if sufficient sample and time are
available.
If more data cannot be obtained, apply the Q test to the
existing set to see if the doubtful result should be
retained or rejected on statistical grounds.
If the Q test indicates retention, consider reporting the
median of the set rather than the mean.
ANALYZING TWO-DIMENSIONAL DATA: THE
LEAST-SQUARES METHOD
Many analytical methods are based on a calibration curve
in which a measured quantity y is plotted as a function of
the known concentration x of a series of standards. The
typical calibration curve shown in Fig. 8-9. The ordinate
is the dependent variable and the abscissa is the
independent variable. As is typical (and desirable), the
plot approximates a straight line. However, because of the
indeterminate errors in the measurement process, not all
the data fall exactly on the line. Thus, the investigator
must try to draw the “best” straight line among the points.
A statistical technique called regression analysis provides
the means for objectively obtaining such a line and also
for specifying the uncertainties associated with its
subsequent use.
Assumptions of the Least-Squares Method
When the method of least squares is used to generate a
calibration curve, two assumptions are required. The first is the
there is actually a linear relationship between the measured
variable (y) and the analyte concentration (x). The mathematical
relationship that describes this assumption is called the
regression model, which may be represented as
y = mx + b
where, b is the y intercept (value of y when x is zero) and m is
the slope of the line. We also assume that deviation of individual
points from the straight line results from error in the
measurement. That is, we must assume that there is no error in
the x values of the points. We assume that exact concentrations
of the standards are known. Both of these assumption are
appropriate for many analytical methods.
Computing the Regression Coefficients and
Finding the Least-Squares Line
The vertical deviation of each point from the
straight line is called a residual. The line generated
by the least-squares method is the one that
minimizes the sum of the squares of the residuals
for all the points. In addition to providing the best
fit between the experimental points and the straight
line, the method gives the standard deviations for
m and b.
…continued…
We define three quantities Sxx, Syy, and Sxy as
follows:
Sxx = (xi – x)2 = x2i – (xi)2 / N
Syy = (yi – y)2 = y2i – (yi)2 / N
Sxy = (xi – x)(yi – y) = xiyi– [(xiyi)] / N
where, xi and yi are individual pairs of data for x
and y, N is the number of pairs of data used in
preparing the calibration curve, and x and y are the
average values for the variables; that is,
x = xi / N and
y = yi / N
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