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Relative error distribution due to instruments

For many contemporary spectrophotometers it is possible to measure absorbance up to within 4 or 5 units. These high values correspond to transmitted intensities that are extremely weak (I/Ig = 10 for A = 5), giving results that are considered as less reliable. [Pg.198]

As these sources of error are additive, the total error in the concentration corresponds — in accepting the three expressions above — to a curve whose ordinate of each point is the sum of the ordinate of the three individual errors discussed above. This curve passes through a minimum generally located around A = 0.7. For quantitative measurements it is therefore advisable to adjust the dilutions in order that the absorbances are situated in this favourable domain. [Pg.199]

From the Lambert—Beer law it is also possible to link relative standard deviation (see Section 22.2) on the measurement of concentration C to the relative standard deviation made on the transmittance T (curve 4). [Pg.199]


See other pages where Relative error distribution due to instruments is mentioned: [Pg.198]    [Pg.199]   


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