Footnotes for Section

The molar absorptivity (molar extinction coefficient) E is defined as E = mol l cm , where is the absorbance at the 

The X columns give the wavelength of the absorption maximum at which E and hypochromicity (h3rperchromicity) values were determined wavelengths are marked by asterisks whenever X is not the wavelength of the maximum or was not specified as such in the reference. 

The h columns (oligonucleotides) give percent h3rpochromicity or h3rperchromicity values (the latter are followed by the symbol ). When these values are given in the Note column (for pol3mucleotides).. they are identified by abbreviations hpo. and hper., respectively h3 erchromicity accompanying the helix—coil transition is abbreviated as hper.(hx-c). Percent hypochromicity and h3 erchromicity are alternatively defined as follows  

The temperature at which absorptivity, hypochromicity, and hwerchromicity values were obtained is given in the Note and T(°C) columns for oligonucleotides and pol3mucleotides, respectively. Absence of temperature data indicates that they were not given in the reference temperature in such cases is usually understood as a room temperature. 

Molar absorptivity values are generally determined by phosphate analysis or from the monomer concentration. The latter is determined upon hydrolysis of the poljnner or oligomer from absorbance readings using literature E values for the monomer. The method of determination of E values may be indicated in the Note column by appropriate s5nnbols listed under Abbreviations. 

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If the person responsible for placing the product on the market can demonstrate that the disclosure in the SDS of the chemical identity of a substance will put at risk the confidential nature of his intellectual property, he/she may, in accordance with the provisions of REACH Annex II footnote for Section 3.3, refer to that substance by means of a name that identifies the most important functional chemical groups, or by means of an alternative name. 

The F-K s method of expanding the exponent is applied to make the exponential term integrable. Another example is presented with regard to Eqs. (25) (39) in Section 2.4. For this method, refer to a footnote in Section 2.7 as well. 

As commented in a footnote in Section 3.5, a value of p. measured for a chemical of the TD type by the BAM heat-accumulation storage test is referred to as the value of the BAM test for the chemical herein. 

After a thin gas-permeable silica fiber sheet has been placed on the bottom of a draft cell, i.e., the cell with which the sample cell is prepared, 0.3 g of the sawdust of Port Orford cedar, which is of course a kind of the moisture-containing gas-permeable oxidatively-heating substance, is charged in the cell. The glass jig mentioned in a footnote in Section 7.3 is used at this time to provide a thin vertical hole at the center of the sawdust charged in the cell in order to facilitate the insertion of the thermocouple into the sawdust. 0.3 g was chosen herein as the standard sample quantity in the adiabatic oxidatively-heating test performed for the sawdust of every wood species. For the procedure to prepare the sawdust of each wood species, refer to Subsection 8.2.1. 

Practically speaking, however, as commented in a footnote in Section 3.2, the larger the size of the chemical, the temperature of which has been maintained at room temperature until the placement, the longer becomes naturally the time required for the temperature of the ehemical as a whole to increase from room temperature up to the T,. 

It was already explained in a footnote to Section 5.2.5 that it is useful to have signature schemes with restricted message bounds. In particular, pure one-time signature schemes, where only one message can be authenticated, are interesting building blocks for more general schemes. 

This equation can be obtained as the approximate wave equation for a system of two particles constrained by a potential function which restricts the particles to a plane and keeps them a fixed distance apart by an argument similar to that used in the discussion of the diatomic molecule mentioned in the footnote to Section 35c. 

The wave equation for a diatomic molecule in a crystal, considered as a rigid rotator, obtained by introducing V into the equation for the free rotator given in a footnote of Section 35c, is... 

The parameter sq is called the permittivity of free space or the electric constant and has the value 8.85419 X IQ-12 q1 jvj-1 j -1 ggg footnote in Section 13.3.1 for a fuller explanation of electrostatic conventions followed in this book. 

The data in this table are mainly taken from A. J. Bard, J. Jordan, and R. Parsons, Eds., Standard Potentials in Aqueous Solutions, Marcel Dekker, New York, 1985 (prepared under the auspices of the Electrochemistry and Electroanalytical Chemistry Commissions of lUPAC). Other sources of standard potentials and thermodynamic data include (1) A. J, Bard and H. Lund, Eds., The Encyclopedia of the Electrochemistry of the Elements, Marcel Dekker, New York, 1973-1986. (2) G. Milazzo and S. Caroli, Tables of Standard Electrode Potentials, Wiley-Interscience, New York, 1977. The data here are referred to the NHE based on a 1-atm standard state for H2. See the footnote in Section 2.1.5 concerning the recent change in standard state. 

Hartwick (17) aligned uniformly sized fibers into a densely packed hexagonal array. The interstices between the fibers represented the flow channels. There was no transport between the channels. The performance of the device was low relative to its permeability. This is not unexpected A key property of a packed bed is the radial mass transfer, which evens out flow nonuniformities. Tto is not possible in a device consisting of parallel independent flow paths. In an array of circular parallel channels, the breakthrough time for an unretained sample is inversely proportional to the square of the diameter of the channel. To obtain a plate count of 10,000 plates, it would be necessary that the relative standard deviation of the channel diameter is under 0.5% (see also the footnote in Section 2.1.4). This is clearly a tall order. For retained peaks, similar demands would need to be placed on the uniformity of the stationary phase from channel to channel. 

Note the similarity of the wavefunction in equation 10.14 and the exponential form of the wavefunctions for the particle-in-a-box (shown in the first footnote in Section 10.8). In this case, however, the exponentials have real exponents, not imaginary eiqionents. 

Footnote This table shows only the major code sections. For more detail and to determine when a section was added, the reader should consult the official primed version of the U.S. Code. 

Corrections for gauche configurations and cis isomers are given in the footnotes to Table 6. Corrections for ring structures are given in Table 8. The sources of the ring correction terms are discussed in Section IV. 

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