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Emissivity reading

It is required to have known quantities to which to compare the sample. These are absorption or emission readings or calibration constants obtained through known quantities. [Pg.180]

For many atoms the energy difference between their ground state orbital and the excited state is too great for thermal excitation of a significant number of electrons to take place. Where energy differences are too great to get an emission reading,... [Pg.126]

The effect of potassium. Take five replicate emission readings of each of the six potassium standards. Remember to zero the instrument between each standard while aspirating a blank. Calculate the mean emission and RSD for each standard and plot a graph of sodium emission intensity against potassium concentration. The RSD is defined as standard deviation (s) of the emission intensities divided by the mean emission intensity (jf)[RSD = (s/x) x 100]. [Pg.169]

Instrument that measures the fluorescence properties of solutions. It is composed of a high-energy lamp for excitation and a phototube for emission readings. Instruments are available in either tube or microplate formats. Volume 1(14). [Pg.390]

Using a spreadsheet, plot the emission readings for the standards against concentration and determine the concentration in the unknown solution from the calibration curve. From this, calculate the micrograms of solution in your unknown if it is water, and ppm or meq/L if it is serum (see footnote 1). [Pg.779]

Penner SS (1959) Quantitative Molecular Spectroscopy and Gas Emissivities. Reading. MA Addison-Wesley Pub. Co. [Pg.559]

Don t waste time and money on an instrument with an emissivity reading. Just make sure the pipe surface is nonreflective by using the tar, black paint, or blackish grease. I ve had no luck with the emissivity settings. [Pg.544]

Water Vapor The contribution to the emissivity of a gas containing H9O depends on Tc andp L and on total pressure P and partial pressure p . Table 5-8 gives constants for use in evaluating . Allowance for departure from the special pressure conditions is made by multiplying by a correction factor C read from Fig. 5-21 as a function of (p + P) and p ,L. The absorptivity 0t of water vapor for blackbody radiation is evaluated from Table 5-8 but at T instead of Tc and at p LT /Tc instead of p, h. Multiply by (Tc/Ti)° . ... [Pg.579]

Clouds of Nonblack Particles The correction for nonblackness of the particles is complicated by multiple scatter of the radiation reflected by each particle. The emissivity . of a cloud of gray particles of individual surface emissivity 1 can be estimated by the use of Eq. (5-151), with its exponent multiplied by 1, if the optical thickness alv)L does not exceed about 2. Modified Eq. (5-151) would predict an approach of . to 1 as L 0°, an impossibihty in a scattering system the asymptotic value of . can be read from Fig. 5-14 as /, with albedo (0 given by particle-surface refleclance 1 — 1. Particles with a perimeter lying between 0.5 and 5 times the wavelength of interest can be handledwith difficulty by use of the Mie equations (see Hottel and Sarofim, op. cit., chaps. 12 and 13). [Pg.582]

The most recent compilation of emission standards for processes and substances emitted from processes in the industrialized countries of the world was the companion Volume II of the source of Table 22-10 (see Jarrault in Suggested Reading). [Pg.418]

To reduce emissions from fuel-burning sources, one can limit the sulfur, ash, or volatile content of fuels. A listing of such limitations as they existed in 1974 is given in Martin and Stem (see Suggested Reading). [Pg.418]

V. Means for Implementing Emission Standards References Suggested Reading Questions... [Pg.580]

Direct-reading polychromators (Figure 3b) have a number of exit slits and photomultiplier tube detectors, which allows one to view emission from many lines simultaneously. More than 40 elements can be determined in less than one minute. The choice of emission lines in the polychromator must be made before the instrument is purchased. The polychromator can be used to monitor transient signals (if the appropriate electronics and software are available) because unlike slew-scan systems it can be set stably to the peak emission wavelength. Background emission cannot be measured simultaneously at a wavelength close to the line for each element of interest. For maximum speed and flexibility both a direct-reading polychromator and a slew-scan monochromator can be used to view emission from the plasma simultaneously. [Pg.641]

Test a hypothesis about the source of the problem, such as checking emissions from a piece of equipment. Testing for "indicator" compounds associated with particular types of building conditions Peak carbon dioxide CO2) concentrations over 1000 ppm (parts per million) are an indicator of underventilation. Carbon monoxide (CO) over several ppm indicates inappropriate presence of combustion by-products (which may also account for high CO2 readings). Compare any measured concentrations to guidelines or standards. [Pg.225]

Direet reading instruments also ean provide an indieation of site emission levels. [Pg.60]

With particles, the contaminant concentration in the duct is determined by isokinetic sampling with subsequent laboratory analysis use of a calibrated direct reading instrument. If the concentration distribution in the duct is uneven, a complete survey of the concentration distribution with the corresponding duct velocities and cross-sectional area is required. National and ISO standards provide information on isokinetic sampling and velocity measurements. In the case of particles, the airborne emission differs from the total emission, for example in the case of granular particulate. The contaminant settling on surfaces depends on particle distribution, airflow rates, direction in the space, electrical properties of the surfaces and the material, and the amount of moisture or grease in the environment. [Pg.1018]

TTie system can be used for continuous measurement of the mass concentration at a single point for up to 12 hours, for traverse measurements of stack particulate mass concentrations using sample probe extensions, with the mass transducer up to 6 m in the stack, or for intermittendy measuring particulate mass concentrations of emission gases for long-term readings (e.g.. 30-sec samples every 60 minutes. ... [Pg.1290]

Table 6.2 presents an overview of surface-emissive powers measured in the British Gas tests, as back-calculated from radiometer readings. Peak values of surface-emissive powers were approximately 100 kW/m higher than these average values, but only for a short duration. Other large-scale tests include those conducted to investigate the performance of fire-protection systems for LPG tanks. [Pg.165]


See other pages where Emissivity reading is mentioned: [Pg.180]    [Pg.148]    [Pg.149]    [Pg.169]    [Pg.170]    [Pg.227]    [Pg.206]    [Pg.872]    [Pg.294]    [Pg.56]    [Pg.67]    [Pg.76]    [Pg.491]    [Pg.134]    [Pg.674]    [Pg.180]    [Pg.148]    [Pg.149]    [Pg.169]    [Pg.170]    [Pg.227]    [Pg.206]    [Pg.872]    [Pg.294]    [Pg.56]    [Pg.67]    [Pg.76]    [Pg.491]    [Pg.134]    [Pg.674]    [Pg.139]    [Pg.379]    [Pg.317]    [Pg.232]    [Pg.468]    [Pg.2172]    [Pg.545]    [Pg.641]    [Pg.641]    [Pg.329]    [Pg.154]    [Pg.178]    [Pg.452]    [Pg.456]    [Pg.740]    [Pg.791]    [Pg.800]   
See also in sourсe #XX -- [ Pg.544 ]




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