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Rutile

Chemical Properties

Rutile has a chemical formula of TiO2, although it is in fact not purely titanium dioxide.  In reality there is a minimum of 94.0 % TiO2 in rutile and the rest is made up of impurities such as Fe, Ta, Nb, Cr, V and Sn.

As an oxide of titanium, rutile can thus be classified chemically as a metal oxide, but is more specifically a member of a small group of metal oxides known as the rutile group.

The Rutile Group

The rutile group also contains minerals such as Cassiterite (Tin Oxide), Plattnerite (Lead oxide), Pyrolusite (Manganese Oxide) and Stishovite (Silicon Oxide).  All members of the group have the formula MO2 and a 4/m 2/m 2/m symmetry (see Crystal Structure of Rutile).

Like rutile, the other members of the rutile group are often important ores of their respective metals.

 

Physical Properties

The table below shows physical constants and characteristics of rutile, including its optical properties.

Specific Gravity/Density (g/cm3)

4.2 – 4.3

Mohs Hardness at 20oC

6.5

Dielectric Constant

6.7

Birefringence

Maximum (0.285 – 0.296)

Luster

Submetallic to adamantine

Diaphaneity  

Opaque to translucent

Fracture

Concohidal to uneven

Steak

Pale Brown

Pleochroism

Weak to moderate

Refractive Index

- 2.60 to 2.89

Reflective Power

~21%

 

 

 

 

 

 

 

 

 

 

 

 

 

Looking at the table, we can see that with a Mohs Hardness of 6.5 at 20oC, rutile is a brittle material.  This coincides with its crystal structure (see Crystal Structure of Rutile). 

Optically, rutile is transparent in thin crystals otherwise it is found to be opaque.  It’s refractive index is relatively high, 2.60 – 2.89, giving it a greater sparkle than diamond.

 

Metaphysical Properties

On a slightly different note, some people believe that rutile has metaphysical properties.    It is said to one more forgiving towards both oneself and others, and to give a general sense of tranquillity.  Rutile is also said to stimulate one's problem solving capabilities by providing a more in-depth understanding of the details involved.

In the field of complimentary medicine, rutile is used to help strengthen the immune system and to help in the treatment of pulmonary and circulatory disorders.

 

 

 

Titanium Dioxide

As rutile has a defective crystal structure,  very little spectroscopic or thermo-chemical data has been collected for it.  However, for pure titanium dioxide of which a minimum of 94 % of rutile is made up, there is a reasonable amount.  Some of this data is shown below.

Gas Phase Thermochemistry Data

 

Quantity

Value

Units

Reference

Δfgas

-305.4324

kJ/mol

Chase, 1998

gas,1 bar

260.14

J/mol*K

Chase, 1998

 

Gas Phase Heat Capacity (Shomate Equation)

Cp° = A + B*t + C*t2 + D*t3 + E/t2
H° - H°
298.15= A*t + B*t2/2 + C*t3/3 + D*t4/4 - E/t + F -Δff,298
S° = A*ln(t) + B*t + C*t
2/2 + D*t3/3 - E/(2*t2) + G
    C
p = heat capacity (J/mol*K)
    H° = standard enthalpy (kJ/mol)
    Δ
f298.15 = enthalpy of formation at 298.15 K (kJ/mol)
    S° = standard entropy (J/mol*K)
    t = temperature (K) / 1000.  

Temperature (K)

4000. - 6000.

A

63.82818

B

-4.418178

C

1.080707

D

-0.058816

E

-5.216235

F

-336.0739

G

323.0094

ΔH°f,298 (kJ/mol)

-305.4324

Reference

Chase, 1998

 

Gas Phase Ion Energetics Data

Ionization energy determination

IE (eV)

Method

Reference

9.5 ± 0.5

EI

Balducci, Gigli, et al., 1985

9. ± 0.5

EI

Balducci, Gigli, et al., 1985, 2

10.4 ± 1.0

EI

Banon, Chatillon, et al., 1982

9.54 ± 0.10

EI

Hildenbrand, 1976

10.2 ± 0.2

EI

Rauh and Ackermann, 1974

11.56 ± 0.14

EI

Wu and Wahlbeck, 1972

8.5 ± 0.5

EI

Balducci, De Maria, et al., 1972

9. ± 0.2

EI

Mesnard, Uzan, et al., 1966

Appearance energy determinations

Ion

AE (eV)

Other Products

Method

Reference

OTi+

13.7 ± 0.5

O

EI

Banon, Chatillon, et al., 1982

Ti+

14.6 ± 0.5

O2

EI

Banon, Chatillon, et al., 1982

Ti+

20. ± 0.2

?

EI

Mesnard, Uzan, et al., 1966

TiO+

8. ± 0.5

O

EI

Mesnard, Uzan, et al., 1966

 

Vibrational and Electronic Spectra

 State: unknown

 Energy 
 (cm-1

Med.

 Transition 

 λmin (nm) 

 λmax (nm) 

 References

To = 18880

Ne

 

529

621

McIntyre, Thompson, et al., 1971

State:   a

Energy   (cm-1

 Med. 

 Trans. 

 λmin 
 (nm) 

 λmax 
 (nm) 

 References

To = 15800 ± 800

gas

 

 

 

Wu and Wang, 1997

State:   X 

Vib. 
Sym.

No.

Approx. 
 type of mode

cm-1

Med.

Method

References

a1

1

Sym. stretch

965     {T}

gas

IR

DeVore and Gallaher, 1983
Wu and Wang, 1997

 

1

Sym. stretch

962.0

Ne

IR

McIntyre, et al., 1971

 

1

Sym. stretch

946.9

Ar

IR

Chertihin and Andrews, 1995

b2

3

Asym. stretch

944

gas

IR

DeVore and Gallaher, 1983

 

3

Asym. stretch

934.8

Ne

IR

McIntyre, et al., 1971

 

3

Asym. stretch

917.1

Ar

IR

Chertihin and Andrews, 1995

Notes

T          Tentative assignment or approximate value.

To         Energy separation between the v = 0 levels of the excited and electronic ground states.

 

Infrared Spectrum of TiO2

 

Technique:

FT-IR Spectrum  

Phase:

Solid  

MF:

TiO2  

MW:

79.88  

MP:

1855  

BP:

2900  

X Axis

Wavenumber (cm-1)  

Y Axis

Absorbance  

   

 

 

 

Background Properties Crystal Structure Uses Resources

Copyright © 2001 Andrew P.L. Robinson