- •5. Physical Properties
- •5.1 Solubilities
- •Table 5.1 Solubility of Gases in Water
- •5.2 Vapor Pressures
- •Table 5.8 Vapor Pressures of Various Inorganic Compounds
- •5.3 Boiling Points
- •Table 5.12 Ternary Azeotropic Mixtures
- •5.4 Freezing Mixtures
- •5.5 Density and Specific Gravity
- •Table 5.14 Density of Mercury and Water
- •5.5.1 Density of Moist Air
- •Table 5.17 Dielectric Constant (Permittivity) and Dipole Moment of Various Organic Substances
- •5.6.1 Refractive Index
- •5.6.2 Surface Tension
- •5.6.3 Dipole Moments
- •5.6.4 Dielectric Constants
- •5.6.5 Viscosity
- •Table 5.22 Aqueous Sucrose Solutions
- •5.7 Combustible Mixtures
- •Table 5.23 Properties of Combustible Mixtures in Air
- •5.8 Thermal Conductivity
- •Table 5.26 Thermal Conductivity of Various Solids
- •5.9 Miscellany
- •Table 5.29 Van der Waals’ Constants for Gases
- •5.9.1 Some Physical Chemistry Equations for Gases
|
|
|
|
|
|
|
|
PHYSICAL |
PROPERTIES |
|
|
|
|
|
|
|
|
|
|
|
|
|
5.135 |
||||||||
5.6.1 |
Refractive Index |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
||
The refractive index |
n is the ratio of the velocity of light in a particular substance to the velocity of |
||||||||||||||||||||||||||||||
light in vacuum. Values reported refer to the ratio of the velocity in air to that in the substance |
|
|
|||||||||||||||||||||||||||||
saturated with air. Usually the yellow sodium doublet lines are used; they have a weighted mean of |
|
|
|||||||||||||||||||||||||||||
589.26 nm and are symbolized by |
|
|
D |
|
. When only a single refractive index is available, approximate |
||||||||||||||||||||||||||
values over a small temperature range may be calculated using a mean value of 0.000 45 per degree |
|
|
|||||||||||||||||||||||||||||
for dn |
/dt, and |
remembering that |
decreasesn Dwith an |
increase in |
temperature. If a transition point |
|
|
||||||||||||||||||||||||
lies within the temperature range, extrapolation is not reliable. |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
||||||||||||||||
The |
specific refraction |
r D |
is given by the Lorentz and Lorenz equation, |
|
|
|
|
||||||||||||||||||||||||
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
n |
D2 |
1 |
1 |
|
|
|
|
|
|
|
||||||
|
|
|
|
|
|
|
|
|
|
|
R D |
|
|
|
|
|
|
|
|
· |
|
|
|
|
|
|
|
||||
|
|
|
|
|
|
|
|
|
|
n |
D2 |
2 |
|
|
|
|
|
||||||||||||||
where is the density at the same temperature as the refractive index, and is independent of tem- |
|
|
|||||||||||||||||||||||||||||
perature and pressure. The molar refraction is equal to the specific refraction multiplied by the |
|
|
|||||||||||||||||||||||||||||
molecular weight. It is a more or less additive property of the groups or elements comprising the |
|
|
|||||||||||||||||||||||||||||
compound. A set of atomic refractions is given in Table 5.19; an extensive discussion will be found |
|
|
|||||||||||||||||||||||||||||
in Bauer, Fajans, and Lewin, in |
Physical Methods |
of |
Organic Chemistry, |
|
|
3d ed., A. Weissberger |
|||||||||||||||||||||||||
(ed.), vol. 1, part II, chap. 28, Wiley-Interscience, New York, 1960. |
|
|
|
|
|||||||||||||||||||||||||||
The empirical Eykman equation |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
||
|
|
|
|
|
|
|
|
n |
D2 |
|
1 |
|
|
|
|
1 |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
· |
|
constant |
|
|
|
|
||||||||||||||
|
|
|
|
|
|
|
|
n D |
0.4 |
|
|
|
|
||||||||||||||||||
offers a more accurate means for checking the accuracy of experimental densities and refractive |
|
|
|||||||||||||||||||||||||||||
indices, and for calculating one from the other, than does the Lorentz and Lorenz equation. |
|
|
|||||||||||||||||||||||||||||
The refractive index of moist air |
can be calculated from |
the |
expression |
|
|
|
|
|
|
|
|
|
|
|
|
|
|||||||||||||||
|
|
|
|
|
103.49 |
|
|
|
177.4 |
|
|
|
86.26 |
5748 |
|
|
|||||||||||||||
|
|
(n 1) 10 6 |
|
|
|
|
|
p 1 |
|
|
|
|
|
p 2 |
|
|
|
1 T |
|
|
p 3 |
||||||||||
|
|
|
|
T |
|
|
|
T |
|
|
|
T |
|
|
|||||||||||||||||
where p 1 is the partial pressure of dry air (in mmHg), |
|
|
|
|
|
|
|
|
|
|
p 2 |
|
is the partial pressure of carbon dioxide (in |
||||||||||||||||||
mmHg), |
p 3 is the partial pressure of water vapor (in mmHg), and |
|
|
|
|
|
|
|
|
|
T is the temperature (in kelvins). |
||||||||||||||||||||
Example: |
1-Propynyl acetate |
has |
|
|
|
n D |
|
1and.4187 |
|
|
|
density |
at0.209982 |
|
C; the molecular |
||||||||||||||||
weight is 98.102. From the Lorentz and Lorenz equation, |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|||||||||||
|
|
|
|
r D |
(1.4187) 2 |
1 |
|
· |
|
1 |
|
|
|
0.2528 |
|
|
|||||||||||||||
|
|
|
|
(1.4187) |
2 |
2 |
|
|
|
|
|
|
|
|
|||||||||||||||||
|
|
|
|
|
|
0.9982 |
|
|
|
|
|
|
|
||||||||||||||||||
The molar |
refraction is |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Mr D |
(98.102)(0.2528) |
|
|
|
|
24.80 |
|
|
|
|
|||||||||||||||||
From the atomic and group refractions in Table 5.19, the molar refraction is computed as follows: |
|
|
|||||||||||||||||||||||||||||
|
|
|
|
6 H |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
6.600 |
|
|
|
|
||||||
|
|
|
|
5 C |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
12.090 |
|
|
|
|
||||||||
|
|
|
|
1 C |
#C |
|
|
|
|
|
|
|
|
|
|
|
|
|
2.398 |
|
|
|
|
||||||||
|
|
|
|
1 O(ether) |
|
|
|
|
|
|
|
|
|
|
|
|
|
1.643 |
|
|
|
|
|||||||||
|
|
|
|
1 O(carbonyl) |
|
|
|
|
|
|
|
|
|
2.211 |
|
|
|
|
|||||||||||||
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|||||
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Mr |
D |
24.942 |
|
|
|
|