9.9.9: Characterizing Experimental Errors (2024)

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    In this course, you will need to determine the confidence in your results by doing appropriate error analysis. This section and the next are meant to review the types of experimental errors that affect accuracy and precision and to remind you of the simple methods for propagating error.

    Errors That Affect Accuracy

    Accuracy is how close a measure of central tendency is to its expected value, \(\mu\). We express accuracy either as an absolute error, e

    \[e = \overline{X} - \mu \label{4.1}\]

    or as a percent relative error, %e

    \[\% e = \frac {\overline{X} - \mu} {\mu} \times 100 \label{4.2}\]

    Although Equation \ref{4.1} and Equation \ref{4.2} use the mean as the measure of central tendency, we also can use the median.

    The convention for representing a statistical parameter is to use a Roman letter for a value calculated from experimental data, and a Greek letter for its corresponding expected value. For example, the experimentally determined mean is \(\overline{X}\) and its underlying expected value is \(\mu\). Likewise, the experimental standard deviation is s and the underlying expected value is \(\sigma\).

    We identify as determinate an error that affects the accuracy of an analysis. Each source of a determinate error has a specific magnitude and sign. Some sources of determinate error are positive and others are negative, and some are larger in magnitude and others are smaller in magnitude. The cumulative effect of these determinate errors is a net positive or negative error in accuracy.

    It is possible, although unlikely, that the positive and negative determinate errors will offset each other, producing a result with no net error in accuracy.

    We assign determinate errors into four categories—sampling errors, method errors, measurement errors, and personal errors—each of which we consider in this section.

    Sampling Errors

    A determinate sampling error occurs when our sampling strategy does not provide a us with a representative sample. For example, if we monitor the environmental quality of a lake by sampling from a single site near a point source of pollution, such as an outlet for industrial effluent, then our results will be misleading. To determine the mass of a U. S. penny, our strategy for selecting pennies must ensure that we do not include pennies from other countries.

    An awareness of potential sampling errors especially is important when we work with heterogeneous materials. Strategies for obtaining representative samples are covered in Chapter 5 of Harvey's Analytical Chemistry text on LibreTexts.

    Method Errors

    In any analysis the relationship between the signal, Stotal, and the absolute amount of analyte, nA, or the analyte’s concentration, CA, is

    \[S_{total} = k_A n_A + S_{mb} \label{4.3}\]

    \[S_{total} = k_A C_A + S_{mb} \label{4.4}\]

    where kA is the method’s sensitivity for the analyte and Smb is the signal from the method blank. A method error exists when our value for kA or for Smb is in error. For example, a method in which Stotal is the mass of a precipitate assumes that k is defined by a pure precipitate of known stoichiometry. If this assumption is not true, then the resulting determination of nA or CA is inaccurate. We can minimize a determinate error in kA by calibrating the method. A method error due to an interferent in the reagents is minimized by using a proper method blank.

    Measurement Errors

    The manufacturers of analytical instruments and equipment, such as glassware and balances, usually provide a statement of the item’s maximum measurement error, or tolerance. For example, a 10-mL volumetric pipet (Figure 9.9.9.1) has a tolerance of ±0.02 mL, which means the pipet delivers an actual volume within the range 9.98–10.02 mL at a temperature of 20 oC. Although we express this tolerance as a range, the error is determinate; that is, the pipet’s expected volume, \(\mu\), is a fixed value within this stated range.

    9.9.9: Characterizing Experimental Errors (2)

    Volumetric glassware is categorized into classes based on its relative accuracy. Class A glassware is manufactured to comply with tolerances specified by an agency, such as the National Institute of Standards and Technology or the American Society for Testing and Materials. The tolerance level for Class A glassware is small enough that normally we can use it without calibration. The tolerance levels for Class B glassware usually are twice that for Class A glassware. In other words, Class B is less accurate. Other types of volumetric glassware, such as beakers and graduated cylinders, are not used to measure volume accurately. Table 9.9.9.1 provides a summary of typical measurement errors for Class A volumetric glassware. Tolerances for digital pipets and for balances are provided in Table 9.9.9.2 and Table 9.9.9.3.

    Tolerance Limits for Class A Volumetric Glassware

    Table 9.9.9.1: Measurement Errors for Class A Volumetric Glassware
    Volumetric Pipets Volumetric Flasks Burets
    Capacity (mL) Tolerance (mL) Capacity (mL) Tolerance (mL) Capacity (mL) Tolerance (mL)
    1 \(\pm 0.006\) 5 \(\pm 0.02\) 10 \(\pm 0.02\)
    2 \(\pm 0.006\) 10 \(\pm 0.02\) 25 \(\pm 0.03\)
    5 \(\pm 0.01\) 25 \(\pm 0.03\) 50 \(\pm 0.05\)
    10 \(\pm 0.02\) 50 \(\pm 0.05\)
    20 \(\pm 0.03\) 100 \(\pm 0.08\)
    25 \(\pm 0.03\) 250 \(\pm 0.12\)
    50 \(\pm 0.05\) 500 \(\pm 0.20\)
    100 \(\pm 0.08\) 1000 \(\pm 0.30\)
    2000 \(\pm 0.50\)

    Tolerance limits for Digital Pipettes

    Table 9.9.9.2: Measurement Errors for Digital Pipets
    Pipet Range Volume (mL or \(\mu \text{L}\)) Percent Measurement Error
    10–100 \(\mu \text{L}\) 10 \(\pm 3.0\%\)
    50 \(\pm 1.0\%\)
    100 \(\pm 0.8\%\)
    100–1000 \(\mu \text{L}\) 100 \(\pm 3.0\%\)
    500 \(\pm 1.0\%\)
    1000 \(\pm 0.6\%\)
    1–10 mL 1 \(\pm 3.0\%\)
    5 \(\pm 0.8\%\)
    10 \(\pm 0.6\%\)

    The tolerance values for the volumetric glassware in Table 9.9.9.1 are from the ASTM E288, E542, and E694 standards. The measurement errors for the digital pipets in Table 9.9.9.2 are from www.eppendorf.com.

    Tolerance Limits for Some Common Balances

    Table 9.9.9.3: Measurement Errors for Selected Balances
    Balance Capacity (g) Measurement Error
    Precisa 160M 160 \(\pm 1 \text{ mg}\)
    A & D ER 120M 120 \(\pm 0.1 \text{ mg}\)
    Metler H54 160 \(\pm 0.01 \text{ mg}\)

    We can minimize a determinate measurement error by calibrating our equipment. Balances are calibrated using a reference weight whose mass we can trace back to the SI standard kilogram. Volumetric glassware and digital pipets are calibrated by determining the mass of water delivered or contained and using the density of water to calculate the actual volume. It is never safe to assume that a calibration does not change during an analysis or over time. One study, for example, found that repeatedly exposing volumetric glassware to higher temperatures during machine washing and oven drying, led to small, but significant changes in the glassware’s calibration [Castanheira, I.; Batista, E.; Valente, A.; Dias, G.; Mora, M.; Pinto, L.; Costa, H. S. Food Control 2006, 17, 719–726]. Many instruments drift out of calibration over time and may require frequent recalibration during an analysis.

    Personal Errors

    Finally, analytical work is always subject to personal error, examples of which include the ability to see a change in the color of an indicator that signals the endpoint of a titration, biases, such as consistently overestimating or underestimating the value on an instrument’s readout scale, failing to calibrate instrumentation, and misinterpreting procedural directions. You can minimize personal errors by taking proper care.

    Identifying Determinate Errors

    Determinate errors often are difficult to detect. Without knowing the expected value for an analysis, the usual situation in any analysis that matters, we often have nothing to which we can compare our experimental result. Nevertheless, there are strategies we can use to detect determinate errors.

    The magnitude of a constant determinate error is the same for all samples and is more significant when we analyze smaller samples. Analyzing samples of different sizes, therefore, allows us to detect a constant determinate error. For example, consider a quantitative analysis in which we separate the analyte from its matrix and determine its mass. Let’s assume the sample is 50.0% w/w analyte. As we see in Table 9.9.9.4, the expected amount of analyte in a 0.100 g sample is 0.050 g. If the analysis has a positive constant determinate error of 0.010 g, then analyzing the sample gives 0.060 g of analyte, or an apparent concentration of 60.0% w/w. As we increase the size of the sample the experimental results become closer to the expected result. An upward or downward trend in a graph of the analyte’s experimental concentration versus the sample’s mass (Figure 9.9.9.2) is evidence of a constant determinate error.

    Table 9.9.9.4: Effect of a Constant Determinate Error on the Analysis of a Sample That is 50.0% w/w Analyte
    Mass of Sample (g) Expected Mass
    of Analyte (g)
    Constant Error (g) Experimental
    Mass of Analyte (g)
    Experimental
    Concentration of Analyte (% w/w)
    0.100 0.050 0.010 0.060 60.0
    0.200 0.100 0.010 0.110 55.0
    0.400 0.200 0.010 0.210 52.5
    0.800 0.400 0.010 0.410 51.2
    1.600 0.800 0.010 0.810 50.6
    9.9.9: Characterizing Experimental Errors (3)

    A proportional determinate error, in which the error’s magnitude depends on the amount of sample, is more difficult to detect because the result of the analysis is independent of the amount of sample. Table 9.9.9.5 outlines an example that shows the effect of a positive proportional error of 1.0% on the analysis of a sample that is 50.0% w/w in analyte. Regardless of the sample’s size, each analysis gives the same result of 50.5% w/w analyte.

    Table 9.9.9.5: Effect of a Proportional Determinate Error on the Analysis of a Sample That is 50.0% w/w Analyte
    Mass of Sample (g) Expected Mass
    of Analyte (g)
    Proportional
    Error (%)
    Experimental
    Mass of Analyte (g)
    Experimental
    Concentration of Analyte (% w/w)
    0.100 0.050 1.00 0.0505 50.5
    0.200 0.100 1.00 0.101 50.5
    0.400 0.200 1.00 0.202 50.5
    0.800 0.400 1.00 0.404 50.5
    1.600 0.800 1.00 0.808 50.5

    One approach for detecting a proportional determinate error is to analyze a standard that contains a known amount of analyte in a matrix similar to our samples. Standards are available from a variety of sources, such as the National Institute of Standards and Technology (where they are called Standard Reference Materials) or the American Society for Testing and Materials. Table 9.9.9.6, for example, lists certified values for several analytes in a standard sample of Gingko biloba leaves. Another approach is to compare our analysis to an analysis carried out using an independent analytical method that is known to give accurate results. If the two methods give significantly different results, then a determinate error is the likely cause.

    Table 9.9.9.6: Certified Concentrations for SRM 3246: Gingko bilbo (Leaves)
    Class of Analyte Analyte Mass Fraction (mg/g or ng/g)
    Flavonoids/Ginkgolide B (mass fraction in mg/g) Qurecetin \(2.69 \pm 0.31\)
    Kaempferol \(3.02 \pm 0.41\)
    Isorhamnetin \(0.517 \pm 0.0.99\)
    Total Aglycones \(6.22 \pm 0.77\)
    Selected Terpenes (mass fraction in mg/g) Ginkgolide A \(0.57 \pm 0.28\)
    Ginkgolide B \(0.470 \pm 0.090\)
    Ginkgolide C \(0.59 \pm 0.22\)
    Ginkgolide J \(0.18 \pm 0.10\)
    Bilobalide \(1.52 \pm 0.40\)
    Total Terpene Lactones \(3.3 \pm 1.1\)
    Selected Toxic Elements (mass fraction in ng/g) Cadmium \(20.8 \pm 1.0\)
    Lead \(995 \pm 30\)
    Mercury \(23.08 \pm 0.17\)

    The primary purpose of this Standard Reference Material is to validate analytical methods for determining flavonoids, terpene lactones, and toxic elements in Ginkgo biloba or other materials with a similar matrix. Values are from the official Certificate of Analysis available at www.nist.gov.

    Constant and proportional determinate errors have distinctly different sources, which we can define in terms of the relationship between the signal and the moles or concentration of analyte (Equation \ref{4.3} and Equation \ref{4.4}). An invalid method blank, Smb, is a constant determinate error as it adds or subtracts the same value to the signal. A poorly calibrated method, which yields an invalid sensitivity for the analyte, kA, results in a proportional determinate error.

    Errors that Affect Precision

    Precision is a measure of the spread of individual measurements or results about a central value, which we express as a range, a standard deviation, or a variance. Here we draw a distinction between two types of precision: repeatability and reproducibility. Repeatability is the precision when a single analyst completes an analysis in a single session using the same solutions, equipment, and instrumentation. Reproducibility, on the other hand, is the precision under any other set of conditions, including between analysts or between laboratory sessions for a single analyst. Since reproducibility includes additional sources of variability, the reproducibility of an analysis cannot be better than its repeatability.

    The ratio of the standard deviation associated with reproducibility to the standard deviation associated with repeatability is called the Horowitz ratio. For a wide variety of analytes in foods, for example, the median Horowtiz ratio is 2.0 with larger values for fatty acids and for trace elements; see Thompson, M.; Wood, R. “The ‘Horowitz Ratio’–A Study of the Ratio Between Reproducibility and Repeatability in the Analysis of Foodstuffs,” Anal. Methods, 2015, 7, 375–379.

    Errors that affect precision are indeterminate and are characterized by random variations in their magnitude and their direction. Because they are random, positive and negative indeterminate errors tend to cancel, provided that we make a sufficient number of measurements. In such situations the mean and the median largely are unaffected by the precision of the analysis.

    Sources of Indeterminate Error

    We can assign indeterminate errors to several sources, including collecting samples, manipulating samples during the analysis, and making measurements. When we collect a sample, for instance, only a small portion of the available material is taken, which increases the chance that small-scale inhom*ogeneities in the sample will affect repeatability. Individual pennies, for example, may show variations in mass from several sources, including the manufacturing process and the loss of small amounts of metal or the addition of dirt during circulation. These variations are sources of indeterminate sampling errors.

    During an analysis there are many opportunities to introduce indeterminate method errors. If our method for determining the mass of a penny includes directions for cleaning them of dirt, then we must be careful to treat each penny in the same way. Cleaning some pennies more vigorously than others might introduce an indeterminate method error.

    Finally, all measuring devices are subject to indeterminate measurement errors due to limitations in our ability to read its scale. For example, a buret with scale divisions every 0.1 mL has an inherent indeterminate error of ±0.01–0.03 mL when we estimate the volume to the hundredth of a milliliter (Figure 9.9.9.3).

    9.9.9: Characterizing Experimental Errors (4)

    Evaluating Indeterminate Error

    Indeterminate errors associated with our analytical equipment or instrumentation generally are easy to estimate if we measure the standard deviation for several replicate measurements, or if we monitor the signal’s fluctuations over time in the absence of analyte (Figure 9.9.9.4) and calculate the standard deviation. Other sources of indeterminate error, such as treating samples inconsistently, are more difficult to estimate.

    9.9.9: Characterizing Experimental Errors (5)

    Error and Uncertainty

    Analytical chemists make a distinction between error and uncertainty [Ellison, S.; Wegscheider, W.; Williams, A. Anal. Chem. 1997, 69, 607A–613A]. Error is the difference between a single measurement or result and its expected value. In other words, error is a measure of bias. As discussed earlier, we divide errors into determinate and indeterminate sources. Although we can find and correct a source of determinate error, the indeterminate portion of the error remains.

    Uncertainty expresses the range of possible values for a measurement or result. Note that this definition of uncertainty is not the same as our definition of precision. We calculate precision from our experimental data and use it to estimate the magnitude of indeterminate errors. Uncertainty accounts for all errors—both determinate and indeterminate—that reasonably might affect a measurement or a result. Although we always try to correct determinate errors before we begin an analysis, the correction itself is subject to uncertainty.

    Here is an example to help illustrate the difference between precision and uncertainty. Suppose you purchase a 10-mL Class A pipet from a laboratory supply company and use it without any additional calibration. The pipet’s tolerance of ±0.02 mL is its uncertainty because your best estimate of its expected volume is 10.00 mL ± 0.02 mL. This uncertainty primarily is determinate. If you use the pipet to dispense several replicate samples of a solution and determine the volume of each sample, the resulting standard deviation is the pipet’s precision. Table 9.9.9.8 shows results for ten such trials, with a mean of 9.992 mL and a standard deviation of ±0.006 mL. This standard deviation is the precision with which we expect to deliver a solution using a Class A 10-mL pipet. In this case the pipet’s published uncertainty of ±0.02 mL is worse than its experimentally determined precision of ±0.006 ml. Interestingly, the data in Table 9.9.9.8 allows us to calibrate this specific pipet’s delivery volume as 9.992 mL. If we use this volume as a better estimate of the pipet’s expected volume, then its uncertainty is ±0.006 mL. As expected, calibrating the pipet allows us to decrease its uncertainty [Kadis, R. Talanta 2004, 64, 167–173].

    Table 9.9.9.8: Experimental Results for Volume Dispensed by a 10–mL Class A Transfer Pipet
    Replicate Volume (ml) Replicate Volume (mL)
    1 10.002 6 9.983
    2 9.993 7 9.991
    3 9.984 8 9.990
    4 9.996 9 9.988
    5 9.989 10 9.999
    9.9.9: Characterizing Experimental Errors (2024)

    FAQs

    How do you calculate the experimental error? ›

    When keeping the sign for error, the calculation is the experimental or measured value minus the known or theoretical value, divided by the theoretical value and multiplied by 100%.

    What is the acceptable range of experimental error? ›

    If you find that your percent difference is more than 10%, there is likely something wrong with your experiment and you should figure out what the problem is and take new data. Precision is measured using two different methods, depending on the type of measurement you are making.

    What is the uncertainty of a 10mL pipette? ›

    Suppose you purchase a 10-mL Class A pipet from a laboratory supply company and use it without any additional calibration. The pipet's tolerance of ±0.02 mL is its uncertainty because your best estimate of its expected volume is 10.00 mL ± 0.02 mL. This uncertainty primarily is determinate.

    How do you describe an experimental error? ›

    The definition of experimental error is any variance between a measurement taken during an experiment and the established value.

    What is the formula for %error? ›

    Percent error formula is the absolute value of the difference of the measured value and the actual value divided by the actual value and multiplied by 100. Why percent error is required? Percent error calculation helps to know how close a measured value is to a true value.

    How do you calculate sample error? ›

    Calculating Sampling Error

    The sampling error is calculated by dividing the standard deviation of the population by the square root of the size of the sample and then multiplying the resultant with the Z-score value, which is based on the confidence interval.

    What is an acceptable error level? ›

    The acceptable margin of error usually falls between 4% and 8% at the 95% confidence level. While getting a narrow margin of error is quite important, the real trick of the trade is getting that perfectly representative sample.

    What is a good error value? ›

    For a good measurement system, the accuracy error should be within 5% and precision error should within 10%.

    What is a good standard error for an experiment? ›

    With a 95% confidence level, 95% of all sample means will be expected to lie within a confidence interval of ± 1.96 standard errors of the sample mean. Based on random sampling, the true population parameter is also estimated to lie within this range with 95% confidence.

    What is the tolerance of a 10mL volumetric pipette? ›

    Eisco Labs 10mL Volumetric Pipette, Borosilicate glass, Class A with +/-0.020 tolerance as per DIN ISO 648 standard.

    What is the range of a 10 mL pipette? ›

    Product Specifications
    Volume Range1 mL – 10 mL
    Accuracy ±5 % / 50 µL ; 1 % / 50 µL ; 0.6 % / 60 µL
    Precision ±0.3 % / 3 µL ; 0.2 % / 10 µL ; 0.16 % / 16 µL
    Tip TechnologyUniversal-Fit Shaft
    Channels1
    3 more rows

    What is the precision of a 10 mL pipette? ›

    The precision of a volumetric pipette comes from the design of the pipette. It is calibrated to deliver 10.00 mL ± 0.01 mL so long as the bottom of the meniscus lies at the center of the calibration line.

    How to calculate experimental error? ›

    How to calculate error
    1. Subtract the actual value from the expected value. First, subtract the actual value from the expected value. ...
    2. Divide by the actual value. After you find the difference between the actual and expected value, you can divide the result of the calculation by the actual value. ...
    3. Multiply the value by 100.
    Jul 2, 2024

    What percent error is too high? ›

    College professors generally look for error levels closer to 5%. However, the harder it is to measure, the closer the acceptable error rate gets to 10%. Experiments that should be very precise may need to have percent error rates that are closer to 1%.

    How to reduce experimental error? ›

    All measurements in an experiment should occur under controlled conditions to prevent systematic error. Changes in external conditions such as humidity, pressure, and temperature can all skew data, and you should avoid them.

    What is the error of the experimental value? ›

    The experimental value of a measurement is the value that is measured during the experiment. Suppose that in your experiment, you determine an experimental value for the aluminum density to be 2.42g/cm3. The error of an experiment is the difference between the experimental and accepted values.

    What is the formula for percentage error in an experiment? ›

    The percentage error formula is % error = (|experimental - accepted|) / (accepted) x 100.

    What is the formula for estimating error? ›

    The error can be estimated as an absolute error, a percentage error, or a relative error. The absolute error measures the total difference between the value you expect from a measurement (X0) and the obtained value (Xref), equal to the absolute value difference of both, Abs = | Xo-Xref |.

    What is the formula for probability error? ›

    Step 1: Based on the above question, Power = 0.85. This means that the probability of correctly rejecting the null hypothesis is 0.85 or 85%. Step 2: We can use the formula 1 - Power = P(Type II Error) to find our probability. Then we have 1 - 0.85 = 0.15 and the probability of a Type II Error is 0.15 or 15%.

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    Name: Dan Stracke

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    Phone: +398735162064

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    Introduction: My name is Dan Stracke, I am a homely, gleaming, glamorous, inquisitive, homely, gorgeous, light person who loves writing and wants to share my knowledge and understanding with you.