The value of the index of refraction can be calculated using chemical and
physical property data if these values are missing.
The relationship between chemical composition, density, and refractive index
was proposed as a means of examining gasses and solutions (Gladstone,
Dale(1863), Phil. Trans, 153, 317). This relationship is as follows:
KP = (n - 1) / d = constant
Where
n = mean index of refraction
D = density
constant = Gladstone-Dale constant
The practice of using the Gladstone-Dale relationship to minerals only gives
an approximation because of the effects that different crystal systems have on
the anisotropy of the crystal lattice and the resultant values of n (index of
refraction). The value of KP may be estimated from the
value of Kc, the value of the Gladstone-Dale constant
derived from the chemical composition.
KC = SUM OF (k1p1/100 + k2p2/100...
+ knpn/100). The Gladstone-Dale constant estimated
from chemical analysis
Where kc = Gladstone-Dale constant of chemical phase "n" kp = Percentage of the chemical phase "n"
Birefringence is an optical property possessed by a material which has more
than one index of refraction. This anisotropy in the index of refraction is
dependant on the crystallographic projection and can be calculated as follows:
Uniaxial Minerals: Birefringence = abs(NO - NE).
Biaxial Minerals: Birefringence = NZ - NX.
Birefringence can also be estimated from a color interference chart for
colors observed under crossed polarizers on a petrographic microscope. The
interference color chart is from Bloss, 1962, fig. 8-17. Click on the image for
a larger picture.
Dispersion is defined as the separation of a ray or beam of
white light into its component colors. The common example is the separation due
to a glass prism into the colors of the rainbow. Dispersion can be measured by
calculating the index of refraction at different wavelengths. High dispersion
materials separate the colors more effectively then low dispersion materials.
High dispersion provides the "fire" in gemstones. Low dispersion materials are
desirable in optical lenses.
In the special case of biaxial minerals, dispersion is
noted by the color fringing in acute bisectrix figures using a petrographic
microscope. This fringing is due to the variation of the refractive indices of
α, β, and γ (Nx, Ny, Nz) with respect to wavelength. The net result is the
variation of 2V
angle with wavelength. This is represented by the relative position of
2Vr for
red light and 2Vv for
violet light on the opposite ends of the visible spectrum. This is
shortened to r and
v.
When 2Vr is
less than
2Vv then it is noted as
r < v.
When 2Vr is
greater than
2Vv then it is noted as
r > v.
Modifiers to r versus
v include: none for no noticeable dispersion weak for weak dispersion moderate for moderate dispersion strong for strong dispersion extreme for maximum dispersion
Other References to Optical Data
Search the Mineralogy Database
Example Subject Searches
Example:biaxial1.7* finds all biaxial
minerals with the lowest index of refraction 1.7 to 1.79. Example:biaxial1.7* bire=0.015* pleochroism
"pale blue" finds all biaxial minerals with the lowest index of refraction
from 1.7 to 1.799, a birefringence of 0.0150 to 10159 and a pale blue
pleochroism. Example:uniaxial1.6* finds all uniaxial
minerals with the lowest index of refraction 1.6 to 1.69. Example:isotropic1.5* finds all
isotropic minerals with the lowest index of refraction 1.5 to 1.59.