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Calculating volume from

Calculating Volume from Mass by Using Density... [Pg.755]

Program to Calculate Volume from van der Waals Equation WIKDOW 1, "van der Waals Voliane", (0,0)- (400,300)... [Pg.203]

Di-n-amyl ether. Use 50 g. (61 5 ml.) of n-amyl alcohol (b.p. 136-137°) and 7 g. (4 ml.) of concentrated sulphuric acid. The calculated volume of water (5 ml.) is collected when the temperature inside the flask rises to 157° (after 90 minutes). Steam distil the reaction mixture, separate the upper layer of the distillate and dry it with anhydrous potassium carbonate. Distil from a 50 ml. Claisen flask and collect the fractions of boiling point (i) 145-175° (13 g.), (ii) 175-185° (8 g.) and (iii) 185-190° (largely 185-185-5°) (13 g.). Combine fractions (i) and (u), reflux for 1 hour in a small flask with 3 g. of sodium, and distil from the sodium amyloxide and excess of sodium this yields 9 5 g. of fairly pure n-amyl ether (iv). The total yield is therefore 22 - 5 g. A perfectly pure product, b.p. 184 185°, is obtained by further distillation from a Little sodium. [Pg.313]

The table convincingly demonstrates how the unsuspected presence of micropores can lead to an erroneous value of the specific surface calculated from a Type II isotherm by application of the standard BET procedure. According to the foregoing analysis, the external specific surface of the solid is 114m g" the micropore volume (from the vertical separation of isotherms A and E) is 105 mm g but since the average pore width is not precisely known, the area of the micropore walls cannot be calculated. Thus the BET figure of 360m g calculated from isotherm E represents merely an apparent and not a true surface area. [Pg.214]

The vapor/hquid ratio tests measure the amount of vapor formed from a given volume of Hquid at a given temperature at atmospheric pressure. A common measure used in specifying gasoline is the temperature at which the vapor/Hquid ratio is 20 (fV/L=2o ) Although V/L can be measured experimentally, it is a difficult and time consuming test to carry out, and techniques have been developed to calculate it from RVP and D86 values. [Pg.182]

No tables of the coefficients of thermal expansion of gases are given in this edition. The coefficient at constant pressure, l/t)(3 0/3T)p for an ideal gas is merely the reciprocal of the absolute temperature. For a real gas or liquid, both it and the coefficient at constant volume, 1/p (3p/3T),, should be calculated either from the equation of state or from tabulated PVT data. [Pg.172]

Step 1. Calculate a new inlet volume using the value of displaced volume from the previous example. [Pg.106]

With these facts in mind, it seems reasonable to calculate the pore volume from the calibration curve that is accessible for a certain molar mass interval of the calibration polymer. A diagram of these differences in elution volume for constant M or AM intervals looks like a pore size distribution, but it is not [see the excellent review of Hagel et al. (5)]. Absolute measurements of pore volume (e.g., by mercury porosimetry) show that there is a difference on principle. Contrary to the absolute pore size distribution, the distribution calcu-... [Pg.437]

For double-acting cylinders, the clearance at the head end should be calculated separately from that of the crank end, because for small cylinders, the volume occupied by the piston rod is significant when cylinder unloading is considered. [Pg.422]

Based on the practical history of scale-up, most fermentation processes for alcohol and organic acid production have followed the concepts of geometric similarity and constant power per unit volume. From the above concept, and as a strong basis for translation of process criteria, only physical properties of the process were considered in the scale-up calculation. For power consumption in an agitated vessel, there is a fixed relation between impeller speed, N, and impeller diameter, l)t. The constant power per unit volume, for a mechanical agitated vessel is given by ... [Pg.288]

The number of the constraints to chain mobility shown in Fig. 16 decreases with increasing temperature, reflecting the increase of the free volume. From a comparison of the spectra in Fig. 15 with line shapes calculated for flexible chains on a diamond lattice 23 (one can infer that the average length of the flexible unit increases from 3-5 bonds at room temperyture to about 10-15 bonds at 380 K. Our model thus can quantitatively explain the gradual increase of the number of conformations accessible to the chain motion. The earlier XH wide line data 72 are also in accord with our findings. [Pg.41]

Calculate the steady-state value for the reactor volume from Vpo/Pout- If this is significantly different than the desired working volume in the reactor, go back to Step 0, but now start the simulation with the tank at the concentrations and temperature just calculated. [Pg.126]

The shear stress Is uniform throughout the main liquid slab for Couette flow ( ). Therefore, two Independent methods for the calculation of the shear stress are available It can be calculated either from the y component of the force exerted by the particles of the liquid slab upon each reservoir or from the volume average of the shear stress developed Inside the liquid slab from the Irving-Kirkwood formula (JA). For reasons explained In Reference (5) the simpler version of this formula can be used In both our systems although this version does not apply In general to structured systems. The Irvlng-Klrkwood expression for the xy component of the stress tensor used In our simulation Is... [Pg.269]

This favors a sample s contraction V is the volume). This attractive force, which will be temperature dependent, is balanced by the regular temperature-independent elastic energy of the lattice Fsiast/V = K/2) 6V/V). Calculating the equilibrium volume from this balance allows us to estimate the thermal expansion coefficient a. More specifically, the simplest Hamiltonian describing two local resonances that interact off-diagonally is... [Pg.181]

This expression reproduces the experimentally measured ionization efficiency curves surprisingly well, considering the simplicity of the model on which it is based. There is a discontinuity in the function at the maximum (when X = Xmax) but this affects only a small region of the ionization efficiency curve, and satisfactory values of the cross section are still obtained over this region. A great advantage of this method is that it is very simple to apply, depending on only three parameters the molecular polarizability volume, the ionization potential, and the maximum electron impact ionization cross section. These can be measured or calculated values (from the ab initio EM method described above, for example). [Pg.338]


See other pages where Calculating volume from is mentioned: [Pg.134]    [Pg.185]    [Pg.111]    [Pg.184]    [Pg.111]    [Pg.86]    [Pg.134]    [Pg.185]    [Pg.111]    [Pg.184]    [Pg.111]    [Pg.86]    [Pg.284]    [Pg.248]    [Pg.298]    [Pg.130]    [Pg.739]    [Pg.135]    [Pg.396]    [Pg.606]    [Pg.16]    [Pg.187]    [Pg.305]    [Pg.43]    [Pg.240]    [Pg.201]    [Pg.244]    [Pg.235]    [Pg.160]    [Pg.592]    [Pg.336]    [Pg.350]    [Pg.68]    [Pg.117]    [Pg.29]    [Pg.353]    [Pg.200]    [Pg.35]   
See also in sourсe #XX -- [ Pg.182 ]

See also in sourсe #XX -- [ Pg.182 ]




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