-
16
-
-
67649231737
-
-
A. Gutberlet G. Schwaab O. Birer M. Masia A. Kaczmarek H. Forbert M. Havenith D. Marx Science 2009 324 1545 1548
-
(2009)
Science
, vol.324
, pp. 1545-1548
-
-
Gutberlet, A.1
Schwaab, G.2
Birer, O.3
Masia, M.4
Kaczmarek, A.5
Forbert, H.6
Havenith, M.7
Marx, D.8
-
34
-
-
79955423099
-
-
University of Wisconsin
-
S. Brastad, PhD Thesis, University of Wisconsin, 2010
-
(2010)
PhD Thesis
-
-
Brastad, S.1
-
37
-
-
12844249938
-
-
S. Ghosal J. C. Hemminger H. Bluhm B. S. Mun E. L. D. Hebenstreit G. Ketteler D. F. Olgetree F. G. Requejo M. Salmeron Science 2005 307 563 566
-
(2005)
Science
, vol.307
, pp. 563-566
-
-
Ghosal, S.1
Hemminger, J.C.2
Bluhm, H.3
Mun, B.S.4
Hebenstreit, E.L.D.5
Ketteler, G.6
Olgetree, D.F.7
Requejo, F.G.8
Salmeron, M.9
-
44
-
-
33751156923
-
-
Calculations from the aerosol inorganics model at The activity coefficient was estimated by extrapolating water activities from 1-14 M and 423-623 K to 212 K and then performing a Gibbs-Duhem calculation. For comparison, the activity coefficient for 8 m LiBr in water at 298 K is 8.6. See
-
K. S. Carslaw S. L. Clegg P. Brimblecombe J. Phys. Chem. 1995 99 11557
-
(1995)
J. Phys. Chem.
, vol.99
, pp. 11557
-
-
Carslaw, K.S.1
Clegg, S.L.2
Brimblecombe, P.3
-
47
-
-
0009034260
-
-
shows that the activity coefficient for a 3 m LiBr solution increases steadily as the temperature is lowered from 523 to 273 K
-
H. F. Holmes R. E. Mesmer J. Chem. Thermodyn. 1998 30 723
-
(1998)
J. Chem. Thermodyn.
, vol.30
, pp. 723
-
-
Holmes, H.F.1
Mesmer, R.E.2
-
53
-
-
0003527731
-
-
Oxford University Press, New York, The peak signal levels in Fig. 3b increase by a factor of 2.7, which is smaller than the 3.8 rise in vapor pressure. This smaller ratio may arise in part from changes in the angular distributions (not yet recorded) at 208 and 218 K and from broad deflections in the gas cloud above the solution
-
R. B. Bernstein, Chemical Dynamics via Molecular Beam and Laser Techniques, Oxford University Press, New York, 1982
-
(1982)
Chemical Dynamics Via Molecular Beam and Laser Techniques
-
-
Bernstein, R.B.1
-
57
-
-
38749092112
-
-
-1 is estimated from the 10-fold lower viscosity of the 212 K solution than the 1400 cP viscosity of pure glycerol at 292 K using the Stokes-Einstein relation
-
B. G. Perkins D. J. Nesbitt J. Phys. Chem. B 2008 112 507 519
-
(2008)
J. Phys. Chem. B
, vol.112
, pp. 507-519
-
-
Perkins, B.G.1
Nesbitt, D.J.2
-
58
-
-
33750250121
-
-
Multiplicative errors in the ion gauge readings alter the slopes in Fig. 8b but not the intercepts
-
D. A. King M. G. Wells Surf. Sci. 1972 29 454 482
-
(1972)
Surf. Sci.
, vol.29
, pp. 454-482
-
-
King, D.A.1
Wells, M.G.2
-
63
-
-
0000857883
-
-
+ and alkali cations from water to methanol is exothermic. See
-
M. J. Isakson G. O. Sitz J. Phys. Chem. A 1999 103 2044 2049
-
(1999)
J. Phys. Chem. A
, vol.103
, pp. 2044-2049
-
-
Isakson, M.J.1
Sitz, G.O.2
|