𝔖 Bobbio Scriptorium
✦   LIBER   ✦

Measurements of orthobaric-liquid densities of multicomponent mixtures of lng components (N2, CH4, C2H6, C3H8, CH3CH(CH3)CH3, C4H10, CH3CH(CH3)C2H5, and C5H12) between 110 and 130 K

✍ Scribed by W.M Haynes


Publisher
Elsevier Science
Year
1982
Tongue
English
Weight
645 KB
Volume
14
Category
Article
ISSN
0021-9614

No coin nor oath required. For personal study only.


πŸ“œ SIMILAR VOLUMES


Unimolecular reactions of the isolated i
✍ Richard D. Bowen; Alex. W. Colburn; Peter J. Derrick πŸ“‚ Article πŸ“… 1990 πŸ› John Wiley and Sons 🌐 English βš– 858 KB

The reactions of ten metastable immonium ions of general structure R'R2C=NH+C4H9 (R' = H, R2 = CH, , C2H, ; R' = R2 = CH,) are reported and discussed. Elimination of C4H, is usually the dominant fragmentation pathway. This process gives rise to a Gaussian metastable peak; it is interpreted in terms

Microwave Spectra of the Methylpolyynes
✍ M.J. Travers; W. Chen; J.-U. Grabow; M.C. McCarthy; P. Thaddeus πŸ“‚ Article πŸ“… 1998 πŸ› Elsevier Science 🌐 English βš– 122 KB

Following the laboratory detection by Fourier transform microwave spectroscopy of the four new methylcyanopolyynes described in the accompanying paper by W. Chen et al. (J. Mol. Spectrosc. 1998), we detected two new methylpolyynes, CH3(C identical withC)4H and CH3(C identical withC)5H. The strongest

Vapour-liquid equilibria in the ternary
✍ G Trappehl; H Knapp πŸ“‚ Article πŸ“… 1988 πŸ› Elsevier Science 🌐 English βš– 434 KB

A systematic study has been performed with mixtures consisting of N 2, CH 4, C2H 6 and C3H 8 to investigate experimentally phase equilibria and caloric properties and to test the accuracy of thermodynamic correlations. This Paper reports more results of T-p-x-y measurements on ternary systems in the

Excess molar heat capacities CEp,m and e
✍ W. Mier; R.N. Lichtenthaler; A.H. Roux; J.-P.E. Grolier πŸ“‚ Article πŸ“… 1994 πŸ› Elsevier Science 🌐 English βš– 299 KB

Excess molar heat capacities and excess molar volumes of \(\left\{x_{1} \mathrm{CH}_{3}\left(\mathrm{CH}_{2}\right)_{3} \mathrm{CH}_{3}+\right.\) \(\left.x_{2} \mathrm{CH}_{3} \mathrm{C}\left(\mathrm{CH}_{3}\right)_{2} \mathrm{CH}_{2} \mathrm{CH}\left(\mathrm{CH}_{3}\right) \mathrm{CH}_{3}+x_{3} \ma