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Bouguer relationship

The Beer-Lambert law (also called the Beer-Lambert-Bouguer law or simply Beer s law) is the linear relationship between absorbance and concentration of an absorber of electromagnetic radiation. The general Beer-Lambert law is usually written as ... [Pg.81]

The multivariate quantitative spectroscopic analysis of samples with complex matrices can be performed using inverse calibration methods, such as ILS, PCR and PLS. The term "inverse" means that the concentration of the analyte of interest is modelled as a function of the instrumental measurements, using an empirical relationship with no theoretical foundation (as the Lambert Bouguer-Beer s law was for the methods explained in the paragraphs above). Therefore, we can formulate our calibration like eqn (3.3) and, in contrast to the CLS model, it can be calculated without knowing the concentrations of all the constituents in the calibration set. The calibration step requires only the instrumental response and the reference value of the property of interest e.g. concentration) in the calibration samples. An important advantage of this approach is that unknown interferents may be present in the calibration samples. For this reason, inverse models are more suited than CLS for complex samples. [Pg.171]

The law from Bouguer, (5.107), is not exactly valid for water vapour and CO2. Therefore, relationships used for the transmission coefficients 7yw and Ty< have a form different from (5.116). These equations can be found in M. Iqbal [5.34], where the associated absorption coefficients are given as functions of the wavelength. Fig. 5.47 shows the pattern of t w and taG These spectral transmissivities have values close to one at wavelengths around 1.2 and 1.6 pm as well as at 2.2 and 3.9 pm. These narrow wavebands are called atmospheric windows, as here the atmosphere allows solar radiation and also radiation from the earth s surface to pass through with virtually no attenuation. [Pg.563]

CD spectra carry much more information than do UV spectra the intensity of the CD absorption is dependent upon the spatial relationship between the chromo-phore and groupings at the chiral centre and therefore there is no chromo-phore-intensity-of-absorption relationship such as that which exists for UV spectra (i.e. the Bouguer-Bccr Lambert law does not apply to CD spectra). Also, the sign of the CD feature can be positive or negative, unlike the isotropic absorption (i.e. the UV spectrum), which has no sign. [Pg.40]

The amount of radiation absorbed depends on the thickness of the absorbing layer and on the concentration of the solution [4,5]. In 1729 Bouguer established the relationship between the amount of absorption (the absorbance) and the thickness of the absorbing layer. A mathematical formulation of this relationship was given by Lambert in 1769. In 1852, Beer settled a relationship between the absorbance and the concentration of coloured solutions. In the formula derived (the Bouguer-Lambert-Beer law) both the solution concentration and the layer thickness are taken into account. [Pg.28]

Some 30 years later, Jean-Henri Lambert (1728-1777) proposed the first mathematical relationship the logarithm of the decrease in light intensity (today we would say the inverse of the transmittance) is equal to the product of the opacity of the medium times its thickness. Finally in 1850, Auguste Beer established a relation between concentration and optical density (now called absorbance), which led to the current form of the Beer-Lambert law (also called Lambert-Beer law or even Lambert-Beer-Bouguer law). [Pg.166]

Although the equation that relates absorbance, concentration, and light path bears the names of Beer and Lambert, it is believed that Pierre Bouguer (1698-1758), a French mathematician, first formulated the relationship in 1729. [Pg.324]

In general absorbance varies during a photochemical reaction. Therefore within the rate laws either the concentrations have to be substituted by the absorbances or the absorbance at the wavelength of irradiation by the concentrations to be able to calculate the integrals, eqs. (3.43) and (3.44), respectively. In principle the relationship between absorbance and concentration is given by the Bouguer-Lambert-Beer law as derived in Section 1.4.3 by Fig. 1.2. For uniform reactions, absorbance at the wavelength of irradiation is defined in Section 1.4.4 by eq. (1.38) to... [Pg.197]

Equation (2.9), which summarizes the relationship between absorbance, concentration of the species measured, sample path length, and the absorptivity of the species is known as the Beer-Lambert-Bouguer Law or, more commonly, as Beer s Law. [Pg.79]

Organic compounds that possess an ultraviolet- or visible-absorbing chromophore obey the Beer Lambert or Beer-Bouguer law of spectrophotometry. In what is generally termed molecular absorption spectrophotometry, a cuvette (in the case of stand-alone UV-vis spectrophotometers) or a micro-flow cell (in the case of flow through HPLC UV-vis detectors). We now proceed to derive the fundamental equation that relates absorbance as measured on an UV-vis HPLC detector to concentration because this relationship is important to the practice... [Pg.384]

The relationship between absorbance and concentration is known as Beer s law (also referred to by other names such as the Beer-Lambert law and the Bouguer-Lambert-Beer law) and is defined by the equation ... [Pg.4457]

The principle of optical spectroscopy involves the measurement of the amount of light (radiation) that is absorbed by the sample when the radiation interacts with the sample. The most basic method involves the determination of the fraction of the radiation that is actually transmitted through a sample. The aspects of the measurement, and their relationship to the actual absorption of radiation are illustrated in Fig. 56. In this example, 7o is the power of the incident radiation from the infrared light source, and I is the actual amount of radiation transmitted through the sample. The fundamental relationships are provided with Fig. 56, and these form the basis of a fundamental expression that is used to correlate the analytical spectrum with the amount(s) of material(s) present in a sample. This fundamental expression is a simple rendering of the Beer-Lambert-Bouguer law, which is used in one form or another in the quantitative determination of material composition. [Pg.296]

Many years ago. Bouguer. Lamberi. and Beer discovered a relationship between the number of particles in a sample, their properties, the path length of the sample, and the observed attenuation of light [22]. [23],... [Pg.424]

It is often found, within certain concentration limits, that the intensity of the absorption is proportional to both the concentration, c (mole per liter), and the thickness, / (centimeter), of the sample in the beam that is, the absorbance = tic, where e is defined as the molar extinction coeffident. This relationship is referred to as Beer s law or the Beer Lambert law. The law is named after August Beer (1825-1863), a lecturer in Bonn who studied optics, and Johann H. Lambert (1728-1777), a Swiss mathematician. It has been suggested that Beer s law was initially discovered by the French mathematician Pierre Bouguer (1698-1758). Lambert made reference (with attribution) to it and, much later, Beer extended it to its present form. [Pg.54]

The first assumption in spectroscopic measurements is that Beer s law relationship applies between a change in spectrometer response and the concentration of analyte material present in a sample specimen. The Bouguer, Lambert, and Beer relationship assumes that the transmission of a sample within an incident beam is equivalent to 10 exponent the negative product of the molar extinction coefficient (in L mol" cm ), multiplied by the concentration of a molecule in solution (in mol L times the path-length (in cm) of the sample in solution. There are some obvious (and not so obvious) problems with this assumption. The main difficulty in the assumed relationship is that the molecules often interact, and the extinction coefficient (absorptivity) may vary due to changes in the molecular configuration of the sample. The obvious temperature, pressure, and interference issues also create a less than ideal situation for the analyst. However, for many (if not most) analytical problems the relationship holds well enough. [Pg.4]

The following are properties of the Bouguer, Lambert, and Beer (Beer s law) relationship ... [Pg.4]

Quantitation can be carried out using absorption or fluorescence spectroscopy. Measurements can be carried out in transmittance or reflectance mode. The basis of quantitative absorption spectroscopy in transmission mode (UVA IS and FUR) is the usual linear relationship of the Beer-Bouguer-Lambert law, which states that the absorbance A of a solute is directly proportional to its concentration c ... [Pg.633]

Beer s law, also referred to as the Beer-Lambert law, or the Beer-Lambert-Bouguer law, expresses the relationship of the absorption of radiation by the sample to the concentration of the desired component and to the path length of the sample. One of the forms in which the law is written follows ... [Pg.303]

The absorption of light by a compound depends on its chromophor, the wavelength of the light and the thickness of the sample. Bouguer derived the relationship between absorption and the thickness of the sample. The integrated form of the equation is shown in Equation [1] where is the intensity of the incident radiation and I the intensity of the transmitted radiation. The factor a related to the absorptivity of the chromophor and b is a measure of the sample thickness. [Pg.767]

The quantitative relationship between the concentration, c, of a component in a sample and its absorbance, A, is given by the Bouguer-Beer law ... [Pg.125]


See other pages where Bouguer relationship is mentioned: [Pg.117]    [Pg.83]    [Pg.265]    [Pg.295]    [Pg.264]    [Pg.19]    [Pg.168]    [Pg.78]    [Pg.5]    [Pg.407]    [Pg.74]    [Pg.238]    [Pg.15]    [Pg.444]    [Pg.33]    [Pg.126]    [Pg.48]   


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