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P/<a calculations

An analytical procedure is often tested on materials of known composition. These materials may be pure substances, standard samples, or materials analyzed by some other more accurate method. Repeated determinations on a known material furnish data for both an estimate of the precision and a test for the presence of a constant error in the results. The standard deviation is found from Equation 12 (with the known composition replacing p). A calculated value for t (Eq. 14) in excess of the appropriate value in Table 2.27 is interpreted as evidence of the presence of a constant error at the indicated level of significance. [Pg.467]

A portable photometer with a linear response to radiation registered 73.6 p.A with a blank solution in the light path. Replacement of the blank with an absorbing solution yielded a response of 24.9 p,A. Calculate [Pg.820]

A similar formalism is used by Thompson and Goldstein [90] to predict residue accessibilities. What they derive would be a very useful prior distribution based on multiplying out independent probabilities to which data could be added to form a Bayesian posterior distribution. The work of Arnold et al. [87] is also not Bayesian statistics but rather the calculation of conditional distributions based on the simple counting argument that p(G r) = p(a, r)lp(r), where a is some property of interest (secondary structure, accessibility) and r is the amino acid type or some property of the amino acid type (hydro-phobicity) or of an amino acid segment (helical moment, etc). [Pg.339]

P.A. Hookham, D. Hatfield, and M. Rosenblatt, Calculation of the Interaction of Three Spherical Blast Waves Over a Planar Surface with an Adaptive-Grid TVD Code, California Research and Technology Report, Chatsworth, CA, 1991. [Pg.350]

Bash P A, U C Singh, F K Brown, R Langridge and P A Kollman 1987. Calculation of the Relat Change in Binding Free-Energy of a Protein-Inhibitor Complex. Science 235 574-576. [Pg.649]

Note the meaning of this expression for each choice of the initial and final position a and a , calculate the classical path that takes you from x to x" m time t. Specifically, calculate tire momentum along the path and the final momentum, p", and find out how p" varies with the initial position. This would give, for a multidimensional problem, a matrix dp"-Jdx"- whose absolute detenninant needs to be inverted. [Pg.2315]

Figure A2.5.6 shows a series of typical p, Fisothemis calculated using equation (A2.5.1). (The temperature, pressure and volume are in reduced units to be explained below.) At sufficiently high temperatures the pressure decreases monotonically with increasing volume, but below a critical temperature the isothemi shows a maximum and a minimum. Figure A2.5.6 shows a series of typical p, Fisothemis <a href="/info/using_a_calculator">calculated using</a> equation (A2.5.1). (The temperature, pressure and volume are in reduced units to be explained below.) At sufficiently <a href="/info/high_temperature_xii">high temperatures</a> the <a href="/info/pressure_decreased">pressure decreases</a> monotonically with increasing volume, but below a <a href="/info/critical_temperature_of_a_gas">critical temperature</a> the isothemi shows a maximum and a minimum.
Gas A, by itself, adsorbs to a of 0.02 at P = 200 mm Hg, and gas B, by itself, adsorbs tod = 0.02 at P = 20 mm Hg Tisll K in both cases, (a) Calculate the difference between (2a and (2b> the two heats of adsorption. Explain briefly any assumptions or approximations made, ib) Calculate the value for 6 when the solid, at 77 K, is equilibrated with a mixture of A and B such that the final pressures are 200 mm Hg each, (c) Explain whether the answer in b would be raised, lowered, or affected in an unpredictable way if all of the preceding data were the same but the surface was known to be heterogeneous. The local isotherm function can still be assumed to be the Langmuir equation. [Pg.672]

Kollman P A 1993. Free Energy Calculations Applications to Chemical and Bicx hemica] Phenojne. Chemical Reviews 93 23 -2417. [Pg.649]

Fs DFWM (jet exper.) [This workl Calculation B3LYP/6- 311+G(2d,p)a) Calculation MP2/ cc-pVTZ [Ref. 101 [Pg.67]

Now, also the coordinates of DGS curves are described also as group of points P (A, sJ. In both cases, the curve represents the registration level for defect evaluation, and, as far as the required evaluation result is concerned, any required value may be automatically calculated by the system and displayed digitally on the screen. Fig. 3. [Pg.814]

Fig. 18. Jet trajectory of a round jet in bounded cross flow where J = Pj V j p (a) flow geometry, ratio of height of tunnel to diameter of injection tube HID) = 12 and (b) flow streamlines where the data points are experimental deterrninations and the lines correspond to calculated predictions for (—) Fig. 18. Jet trajectory of a round jet in bounded <a href="/info/cross_flow">cross flow</a> where J = Pj V j p (a) <a href="/info/flow_geometries">flow geometry</a>, ratio of height of tunnel to diameter of <a href="/info/injection_tubing">injection tube</a> HID) = 12 and (b) <a href="/info/streamline_flow">flow streamlines</a> where the <a href="/info/gel_point_data">data points</a> are experimental deterrninations and the lines correspond to calculated predictions for (—)
Pearlman D A and P A Kollman 1989. A New Method for Carrying Out Free-Energy Perturbation Calculations - Dynamically Modified Wmdows. Journal Of Chemical Physics 90 2460-2470. [Pg.652]

S. Miyamoto and P. A. Kollman. Absolute and relative binding free energy calculations of the interaction of biotin and its analogs with streptavidin using molecular dynamics/free energy perturbation approaches. Proteins, 16 226-245, 1993. [Pg.96]

The concentration-velocity data shown below were obtained for an enzyme catalyzing a reaction S->P. (a) Calculate and [Pg.319]

Simmerling C, T Fox and P A Kollman 1998. Use of LocaUy Enhanced Sampling in Free Energ Calculations Testing and Application to the o —> /3 Anomerisation of Glucose. Journal of tl American Chemical Society 120 5771-5782. [Pg.653]

Figure 37. Variation of the dielectric constant s/s2 of a metal-insulator colloid solution as a function of the metallic phase (silver) p (a) calculation based on the Lorentz model (b) calculation based on the fractal model. Figure 37. Variation of the <a href="/info/e_dielectric_constant">dielectric constant</a> s/s2 of a <a href="/info/metals_and_insulators">metal-insulator</a> <a href="/info/solutions_colloids">colloid solution</a> as a function of the <a href="/info/metal_phases">metallic phase</a> (silver) p (a) calculation based on the <a href="/info/the_lorentz_model">Lorentz model</a> (b) calculation based on the fractal model.
C. A. Coulson and A. Streitwieser, Jr., Dictionary of n-Electron Calculations, W. H. Freeman, San Francisco, 1965 E. Heilbronner and P. A. Straub, Hiickel Molecular Orbitals, Springer-Verlag, Berlin, 1966. [Pg.32]

Eriksson M A L, J Pitera and P A Kollman 1999. Prediction of the Binding Free Energies of New TIBO-like HIV-1 Reverse Transcriptase Inhibitors Using a Combination of PROFEC, PB/SA, CMC/MD, and Free Energy Calculations. Journal of Medicinal Chemistry 42 868-881. [Pg.650]


See other pages where P/<a calculations is mentioned: [Pg.136]    [Pg.27]    [Pg.74]    [Pg.498]    [Pg.705]    [Pg.782]    [Pg.401]    [Pg.117]    [Pg.380]    [Pg.16]    [Pg.619]    [Pg.1148]    [Pg.2218]    [Pg.2227]    [Pg.32]    [Pg.161]    [Pg.607]    [Pg.282]    [Pg.182]    [Pg.230]    [Pg.270]    [Pg.587]    [Pg.652]    [Pg.198]    [Pg.70]    [Pg.80]    [Pg.38]    [Pg.203]    [Pg.175]    [Pg.585]    [Pg.2052]    [Pg.55]   
See also in sourсe #XX -- [ Pg.433 , Pg.452 ]




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