unit 1: analytical process and data handling Flashcards
activity (ax)
the effective concentration, taking into account the effect of ionic strength π΄π₯ = [π₯]πΎ subπ₯
absolute uncertainty
typically the standard deviation of multiple measurements or from (1) a calibration, (2) the manufactureβs stated tolerance (equation below), or (3) gradations on the device or instrument. π = Β± π‘ππππππππ /β6 = Β± π /β6
Activity coefficient (Ξ³x)
dimensionless quantity that measures the deviation of the behavior from ideality; can be calculated using the extended Debye-HΓΌckle equation (below, only applicable for solutions with ΞΌ β€ 0.1 M) or activity coefficient tables (table 8.1 in 10th edn of Harris)
ππππΎ = (β0.51π§ ^2 βπ ) /(1 + ( πΌβπ /305) )
Some trends: 1) For a given ionic strength, deviations from ideality increase with charge 2) For a given species, deviations from ideality increase with ionic strength 3) Small effects are seen for differences in hydrated radius; the effect of charge is greater 4) The activity coefficient of an uncharged molecule is approximately 1 (ideal) at any ΞΌ
blank
contains everything that is in the standards and sample solution, but no analyte; often further classified as a method blank (blank that has been process through the entire method) or a reagent blank (blank that contains just contains everything except analyte and has not been process through the entire method)
callibration curve
Translate signal output into a concentration. Plots concentration vs. signal, uses a least squares linear regression (or weighted linear regression) to determine a line that fits the calibration; using this line we can know the relation between any signal (y) and the concentration (x). Uncertainty in a calibration curve
π’π₯ = (π π¦ /|π|) (β (1/ π) +( 1/ π )+ (π¦ β π¦Μ )^2)/ π^2 β(π₯π β π₯Μ ) ^2
confidence interval
π₯Μ Β± (π‘π / βn)
confidence limits
The upper and lower bounds of the confidence interval
f-test
Answers the question: are the two standard deviations significantly different from one another? Can inform if one method is more precise than another πΉππππ = (π 1)^2 / (π 2)^ 2
figures of merit
metrics that give a measure of how βgoodβ the method/technique is
gaussian distribution
(also called a bell curve or normal error curve) Experiments repeated many, many times with purely random uncertainty will have results that cluster about the average (mean) and the distribution will resemble the Gaussian Distribution - Population mean (ΞΌ) and population standard deviation (Ο) - calculated from infinite (all) measurements and can completely define the Gaussian - Sample mean (π₯) and sample standard deviation (s) - calculated from a subset of measurements and are used to approximate the Gaussian
grubbs
Statistically determine if a data point is an outlier and should be removed πΊπππππ’πππ‘ππ = |ππ’ππ π‘πππππππ π£πππ’π β π₯Μ | / s
interferent
any substance (not the analyte) whose presence interferes with the signal
internal standard
Calibration method that accounts for differences in instrumental response, or to account for sample loss during the method Uses an internal standard that is similar enough in chemical makeup that it will go through the analytical method in the same way, but different enough to detect it as distinct from the analyte of interest. π΄π /[π] = πΉ ( π΄π /[π] )
ionic atmosphere
region of charge around an ion; charge of the ionic atmosphere is less than the charge of the ion at the center - Decreases the attraction between ions - Higher ionic strength leads to higher charges in the ionic atmosphere - Higher charges in the ionic atmosphere results in weaker attractions between cations and anions in solution
Ionic strength (ΞΌ)
measure of the total concentration of ions in solution, with more highly charged ions βcountedβ more π = (1/2) β (ππ)(π§π)^2
Note: equation only applicable for dilute (less than ~0.2 M) solutions with ions of low charges (>|2|)
Limit of Detection (LOD)
concentration of analyte that gives a signal that is significantly different than the blank πΏππ·πππππππ‘πππ‘πππ = 3π πππππ π or the concentration at S/N = 3
Limit of Quantification (LOQ)
smallest quantity of analyte that can be measured with reasonable accuracy πΏπππππππππ‘πππ‘πππ = 10π πππππ π or the concentration at S/N = 10
linear range
concentration range over which the calibration curve is linear
linearity
measure of how well does the calibration curve follows a straight line, demonstrating the proportionality between response and concentration Measures: R2 , how close the x intercept is to 0 (after blank subtraction) Linear range β concentration range over which the calibration curve is linear Dynamic range β concentration range over which there is a measureable response
matrix
components in a sample that are not the analyte(s) of interest
matrix effect
change in the analytical signal caused by anything other than the analyte of interest
measures of precision
Variance (s2 or Ο2 ): has the units of the measurement squared; are additive Standard deviation (s or Ο): has units of the measurement; are not additive; measures the width of the Gaussian Relative standard deviation (RSD = s/root π₯): often reported in ppt (x 1000) or as the coefficient of variation (CV, x 100) or %RSD (x 100)
method of validation
the process that proves the acceptability of a method for its intended purpose
prop of unc- addition and sub
Use the absolute uncertainties of individual terms to determine the uncertainty in the final result: ππ = βππ₯^2 + ππ¦^2 + πz^2
Propagation of Uncertainty β Multiplication and Division
Use the relative uncertainties of individual terms to determine the uncertainty in the final result: %ππ = β%ππ₯^2 + %ππ¦^22 + %ππ§^22 Reminder: %ππ₯ = ππ₯/π₯
random uncertainty
(Harris calls this random error) - uncertainty that causes data to be scattered evenly about an average value - effects the precision of the measurement
relative uncertainty
Relative uncertainty: %π = πππ πππ’π‘π π’πππππ‘ππππ‘π¦ / ππππππ‘π’ππ ππ ππππ π’ππππππ‘ Γ 100 (as a percent) ππππ‘ = πππ πππ’π‘π π’πππππ‘ππππ‘π¦ / ππππππ‘π’ππ ππ ππππ π’ππππππ‘ Γ 1000
repeatability and reproducability
Repeatability β precision of the same person, in the same lab, on the same instrument
Reproducibility (inter laboratory precision) β precision of different people in different labs with different equipment on a similar sample and the same method.
robustness
ability of the method to be unaffected by small, deliberate changes in operating conditions/parameters
sample
solution containing an unknown amount of analyte
sensitivity
ability of an instrument/technique to discriminate, based on signal, between similar concentrations; slope of the calibration line
specificity
ability of an analytical method to distinguish the analyte of interest from everything else present in the sample
standard
solutions containing a known amount of analyte
standard addition
X-not at 0. Calibration method that accounts for matrix effects; known quantities of the analyte of interest are added or βspikedβ into the sample When using standard addition where all solutions have a constant volume, the final concentration of unknown is the absolute value of the x intercept.
Systematic error
an error that consistently makes the measured value different from the true value - effects the accuracy of the measurement
E = xi - xt
πΈπ = (π₯πβπ₯π‘) / π₯π‘ Γ 100
t-test case 1
Answers the question: are the two means significantly different from one another? Case 1 T-Test: Comparison of an experimental mean with a known value π₯Μ Β± π‘π / βπ
t-test case 2
Case 2 T-Test: Comparison of two experimental means Must perform an F-test first to determine which set of equations to use. If standard deviations are not significantly different:
π‘ππππ = (|π₯Μ
1βπ₯Μ
2| / π ππππππ ) * (β π1π2 /π1+π2 )
( check eq sheet for porper format) π ππππππ = β π 1 2(π1β1)+π 2 2 (π2β1) π1+π2β2 If standard deviations are significantly different: π‘ππππ = |π₯Μ 1βπ₯Μ 2| β(π 1 2 /π1)+(π 2 2 /π2) πππππππ ππ πππππππ = (π 1 2 /π1+π 2 2 /π2) 2 (π 1 2/π1) 2 π1β1 + (π 2 2/π2) 2 π2β1
t-test case 3
Case 3 T-Test: Paired T-Test, Different methods used on the same set of samples π‘ππππ = |πΜ |βπ / π π