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Isosteric heat of adsorption of nitrogen on molecular

Isosteric heat of adsorption q of nitrogen adsorbed at 77 K on non-porous and porous silica. gel A, mesofxirous

Isosteric heat of adsorption q of nitrogen adsorbed at 77 K on non-porous and porous silica. gel D,

Isosurface grid of chlorate anion

Isothemis of k for tran.s-stilbene photoisomerization in n-hexane at temperatures between

Isothemis showing the reduced external magnetic field B. P Bq ZcTj versus the order parameter s for various reduced temperatures J TIT.

Isotherm of composition change or surface excess isotherm for the adsorption of

Isothermal annealing at 380 C , respectively.

Isothermal energy release from cold-worked copper, measured calorimelrically

Isothermal section of Al—Cu—Li system at 350 C a, isothermal section b, limits of soHd solubility for a-phase. SoHd lines

Isothermal time temperature transformation curves for a eutectoid steel and

Isothermal transformation . Ae is A temperature at equiUbnum BHN, BrineU hardness number

Isotherms calculated according to the BET equation for the following values of c

Isotherms calculated according to the BET equation for the following values of c

Isotherms for polar adsorbates on natural montmorillonite at 323 K. O, adsorption x, desorption.

Isotherms for polar adsorbates on natural montmorillonite at 323 K. O, adsorption x, desorption.

Isotherms of argon . Open circles, adsorption solid circles,

Isotherms of argon . Open circles, adsorption solid circles,

Isotherms of water at 25 C on a sample of rutile, after outgassing in succession at 300 C

Isotherms on a natural sodium-rich montmorillonite. Circles denote adsorption, crosses desorption.

Isotherms on a natural sodium-rich montmorillonite. Circles denote adsorption, crosses desorption.

Isotopic enrichment of SFg by multiphoton dissociation following irradiation in the vibrational band of SFg. The absorption spectrum is shown

Isotropic yield surfaces in strain space.

Isotropic, nematic and chiral nematic phases. Here n denotes tire director. In tire chiral nematic phase, tire director undergoes a helical rotation, as schematically indicated by its reorientation around a cone.

Issues facing R D leaders in the face of the global dispersion of R D .

It can be appreciated that adjacent

It can be seen that in neutral 0-05 M Na2S04 containing 0-02m Cl . Comparison of Curves 2 and 3 illustrates the influence of Cl ions on the pitting process.

It can be seen that this molding technique produces a molded lip seal with the flash already removed. In general, when using a vacuum chamber on the press, to ensure that all the air and or gases are evacuated from the mold after closure, one or

It is assumed that by using an exactly symmetric cone a shear rate distribution, which is very nearly uniform, within the equilibrium . Therefore in this type of viscometry the applied torque required for the steady rotation of the cone is related to the uniform shearing stress on its surface by a simplihed theoretical equation given as

It is easy to see why he preselects packing over trays for a flow parameter of less than 0.1 for example.

It is important to understand the relationships among velocity, surface temperature, and fouling resistance for a given exchanger. Used by permission

It is seen from

It may take some time for the two reactive groups to diffuse together, but it will also take a while for them to diffuse apart this provides the opportunity to react. The rate at which independent A and B groups convert to ab linkages is thus seen to depend on the relative rates of three processes

It should be observed that the early, low pressure causes the largest increase in temperature due to the crush-up of the powder to densities approaching solid density. The spike in the temperature shown on the profiles at the interfaces of the powder and copper is an artifact due to numerical instabilities .

Iteration Procedure

IV-10 illustrates how F may vary with film pressure in a very complicated way although the v-a plots are relatively unstructured. The results correlated more with variations in film elasticity than with its viscosity and were explained qualitatively in terms of successive film structures with varying degrees of hydrogen bonding to the water substrate and varying degrees of structural regularity. Note the sensitivity of k to frequency a detailed study of the dispersion of k should give information about the characteristic relaxation times of various film structures.

IX Deep, hemispherical depressions on the external surface of an overhead condenser due to severe dezincification from internal surfaces see

IX is a complex reaction that occurs widely

J -maps of a sandstone reservoir eore whieh was soaked in brine,

J 3k Concept of solidified core ir concrete after meltdown

J Fault 1 ree oj F.n.

J Seismic hazard curves for a

J U curves and critical potential range for intergranular stress corrosion in boiling 35 NaOH — potentio-dynamically measured with 0.6 V h - - potential change after every 0.5 h At 0.1 V x-x-x potential change after every 0.5 hAf -0.1 V.

J U curves for aluminum alloys in 3.5 wt. NaCl solution, aerated and

J U curves for an aluminum alloy with 2 Zn and 0.1 Snin3.5 wt. NaCl solution, free convection, not aerated.

J U curves for magnesium in aqueous solutions at 70 C.

J U curves for pure zinc in 3.5 wt. NaCl solution, free convection, not aerated.

J U curves for zinc anodes in 3.5 wt. NaCl solution, aerated and stirred — at the start of the experiment -----after 90 h.

J-l transients for the permeation of hydrogen through ferrous alloys. The normal transient enables the diffusion coefficient to be evaluated from the relationship , L 6D, where , is the time at which J attains a value of 0-63 of the steady-state permeation J

J2-weighted images of the propagation of chemical waves in an Mn catalysed Belousov-Zhabotinsky reaction. The images were acquired in 40 s intervals using a standard spin echo pulse sequence. The slice thickness is 2 nun. The diameter of the imaged pill box is 39 nun. The bright bands



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