logo

Thermoluminescence Study of Quartz Minerals

 Abstract:

The present paper reports the thermoluminescence(TL)study of Quartz minerals collected from the ceramic tiles manufacturing unit, Morbi, Gujarat. The natural thermoluminescence (NTL) as well as artificial thermoluminescence (ATL+NTL), by giving a 15Gy beta dose, was recorded for the collected sample.Then after Quartz mineral is  annealed and quenched from 250oC,4500C and 6500C temperature and irradiated by 25Gy beta dose   from Sr-90 beta source and then the  thermoluminescence was recorded. The TL results are very interesting regarding purity of the mineral.

Keywords: Thermoluminescence, Quartz minerals, Ceramic technology
                    ATL- Artificial Thermoluminescence , NTL- Natural Thermoluminescence.

Introduction:

Many natural mineral are used to manufacture floor tiles for household floorings. The demand of a variety of flooring materials has lead to develop various types of ceramic tiles. In India the ceramic industry is one of the fastest growing industries, more then 200 manufacturing units of ceramic tiles, vitrified tiles and sanitary wares are situated at Morbi (Rajkot District, Gujarat state, India). Many natural minerals are used as the raw materials for the manufacturing ceramic wares. The minerals used in manufacturing the ceramic tiles are Quartz, Feldspar, Zircon, Talc, Frit-O, Frit-T, Aluminium oxide, Sodium trypoly phosphate China clay, Bikaner clay, etc. Most of the minerals are from mines in Gujarat and few are from Rajasthan state and imported from Russia. The phenomenon of TL has been studied by many investigators. The thermoluminescence (TL) study in geology, particularly for natural minerals, is an important research tool.  The TL study of minerals commonly used in ceramic tiles industry, such as Quartz gives better understanding about their properties. The systematic study of TL of such minerals is helpful to solve the basic raw materials quality problem the ceramic tiles industries.

 Quartz:

gr12

The purest natural crystalline form of silica is quartz, containing more than 99.95% SiO2. The other abundant sources of silica are the acid igneous rocks, sands, sandstones and quartzite containing varying amounts of impurities. In all these raw materials SiO2 exists in the form of µ-quartz. Flint, which is a mixture of chalcedony and quartz, is also used as a source of silica in some countries.

     

Under optical microscope, quartz is identified by its colorless, nonpleochroic habit in plane polarized light; shape is commonly anhedral, often found as perfect euhedral crystal. It does not show any cleavage, but some conchoidal fractures are observed within the grains. Anisotropic under cross polarized light, quartz shows first order interference color which is highly variable (grey, yellow etc.). It gives adulatory or patchy extinction which is one of the most characteristic features of Quartz especially in metamorphic rocks. Refractive index is low, slightly higher than Canada balsam (1.55), the outline being feebly visible in plane polarized light. Quartz grains often show numerous tiny vitreous inclusions of other minerals. Quartz is distinguished from alkali Feldspar by its positive relief in balsam, lack of alteration and cleavage. Quartz lacks the multiple twinning of most Feldspar and differs from the untwined oligoclase by uniaxial figure and lack of cleavage.

Uses :  

Quartz is widely used in the manufacture of soda-lime-silica glass and white wares. Quartzite containing about 98% SiO2 are used for the manufacture of silica bricks, used in steel making furnaces, specially at the roof of an acid open-hearth, checkers, converter etc. They are also used in coke-ovens and the roof of glass tank furnace. For refractory use, the combined Al2O3 and TiO2 should be < 2.5% and for superior qualities < 1%. With Na2O and K2O < 0.1% CaO <  0.3% and MgO < 0.1%, quartzite are considered to be of suitable quality.

The pure, untwined, clear and transparent quartz crystals possess piezo-electric properties and are used in telecommunication. Quartz is also the source of element silicon, used in the manufacture of non-oxide ceramics (e.g. SiC, Si3N4) and ferro-silicon.

Chemical Composition of Quartz:

Source

Constituents (%)

Quartz

SiO2

Al2O3

Fe2O3

TiO2

CaO

MgO

K2O

Na2O

LOI

Nizamabad, A.P.

99.75

0.15

0.02

-

-

-

-

-

-

Hyderabad, A.P.

99.96

-

0.02

-

-

-

-

-

-

Gujarat

99.40

0.06

0.04

-

0.09

tr.

-

-

.22

Tura, Meghalaya

99.12

0.21

0.36

0.01

-

-

-

-

-

Jaipur, Rajasthan

98.11

0.41

0.22

tr

0.68

tr.

0.07

0.15

.19

Hyderabad (Sanatnagar)

99.13

0.12

0.13

0.07

0.09

tr.

0.10

0.06

.19

 Experimental method:

Thermal Annealing Treatment:

Thermal annealing for the specimen was carried out in the muffle furnace. The laboratory muffle furnace has temperature range up to 1200oC and the size of chamber for sample heating was 22cm ´ 10cm ´ 10cm. The temperature was maintained with ±1oC accuracy using a temperature controller, which supplied required current to the furnace. Power supply of 230V was provided to the furnace. A silica crucible containing a powdered form of virgin specimens was kept in the furnace at required annealing temperature for desired time. After completion of annealing duration the specimens were rapidly air-quenched to room temperature by withdrawing the Alumina crucible on to a ceramic block. Such material or specimens are called “annealed and quenched” or “thermally pre-treated specimen”.

gr13

(High temperature Furnace and taking out the sample from high temperature furnace)

Beta-Radiation Source

gr14

 

gr15

                (TL Set-Up)                                         (Kanthal strip&Sr-90 Beta source)
The natural Quartz minerals used in manufacturing   ceramic tiles are collected from the industry. Most of the materials used for the TL analysis were indigenous ones and a few were imported minerals. TL of Quartz mineral was recorded using TL set-up supplied by Nucleonix Systems, Hyderabad [1]. Irradiation was carried using Sr-90 beta source. Equal quantities of samples (5 mg) were used for the analysis.
 Results and discussion :  

(4.2)TL Study of Quartz:

gr16

Fig 1.1 is the TL of 5mg of weighed powder was taken to record TL glow curve of Quartz (NTL) without any pre heat treatment and irradiation. The glow curve exhibit one hump like glow peak at temperature at 3320C.  There is no good TL is observed.
Fig.1.2 shows TL glow curve of Quartz irradiated with beta dose of 25 Gy using Sr90. Here one peak occurs at temperature 1100Cand intensity of 1.83au here little TL is recorded. It is noted that after irradiation one trap developed and released carrier during the TL measurement.

Fig1.3                                                         Fig.1.4

gr17

Fig. 1.3 is the TL glow curve of Quartz annealed and quenched from  2500C and given a beta dose of 25 Gy using  Sr-9o beta source TL  glow curve of 250oC AQ sample of Quartz exhibits  one well resolved peak around 109oC.

Fig. 1.4 is the TL glow curve of Quartz annealed and quenched from  4500C and given a beta dose of 25 Gy using  Sr-9o beta source. TL glow curve of 450oC AQ sample of Quartz exhibits  one well resolved and isolated TL peak  with high intensity around 100oC.  This peak is interesting TL peak in  dosimetric point of view. Fig. 1.5 is the TL glow curve of Quartz annealed and quenched from  6000C and given a beta dose of 25Gy using  Sr-9o beta source.   TL  glow curve of 650oC AQ sample of Quartz exhibits  one well resolved and isolated TL peak  with high intensity around 102oC.  This peak is interesting TL peak in dosimetric point of view.

gr18

Table1:


Sr.No.

Temperature oC
 AQ

Peak Temperature
oC

Peak Intensity (Arb.Unit)

1

Natural

332

3.11

2

Beta Irriated

110

1.83

3

2500C+ Beta(15Gy)

109

0.98

4

4500C+ Beta(15Gy)

100

100

5

6500C+ Beta(15Gy)

102

69

Table-1 shows the peak temperature and peak intensity of Quartz at different annealing and quenching temperature irradiated with beta source of 15Gy by Sr90 .

gr19

Fig. 1.10 shows the TGA of Quartz from the TGA it is clear that variation seen in phase between temperature range 4000C and 8000C

gr20

Fig. 1.11 shows the X RD pattern of Quartz it is clearly matches with the standard peaks observed at 26.66, 20.88, 50.18 and 60 o are major peaks of standard quartz sample. 

Conclusion:

  • The natural TL [NTL] observed in both the minerals under study as well as NTL+ATLfollowed by the TL observed from annealed and quenched form 2500C and 450oC and 650oC followed by beta irritation leads to the conclusions this may be due to traps formed due to irradiation as well as heat treatment subjected  to the mineral.
  • The TL study of mineral Quartz sample treated with different annealing and quenching temperature at 2500C, 4500C,and 6500C  irradiated with beta source given a dose of 15Gy by Sr90  gives remarkable result. The maximum TL intensity exhibits by the sample when it treated with AQ 4000C and irradiated with beta source by giving a dose of 25Gy,at this point peak temperature is recorded 1000C and intensity of 100au,the peak at 1000C temperature is well resolved and it is important for study of TL dosimetric point of view.
  • The systemic study may be more useful in checking the purity of the raw materials which in turn leads to improving the quality of ceramic tiles in ceramic industries. Further studies are in progress.

REFERENCES :

  1. K.V.R. Murthy and  J.N. Reddy Thermoluminescence basic theory application and experiment , Feb.2008, Pub. Nucleonix, Hyderabad.
  2. K V R Murthy , Y S Patel , A S Sai Prasad, V Natarajan , A G Page , 2003 Radiation Measurements 36  483.                                                                                                
  3.   K V R Murthy, S P Pallavi, R Ghildiyal, M C Parmar , Y S Patel ,  V Ravi Kuma, A S Sai Prasad V Natarajan , A G Page , 2006 Radiation  Prot. Dosim. 120 238.
  4.  K V R  Murthy , S P Pallavi , R Ghildiyal ,  Y S Patel ,A S Sai Prasad , D Elangovan, 2006 Radiation  Prot. Dosim. 119  350.
  5. S W S Mckeever , 1985 Thermoluminescence of Solids, Cambridge University Press, Cambridge,  205.
  6. Blasse , 1994 Luminescent Materials, Springer, Berlin  93.
  7. M J Aitken , 1974 Physics and Archaeology) Oxford, U.K.: Oxford Univ. Press.
  8. S W S McKeever , M S Akselrod  and B G Markey , 1996  Radiation .Prot. Dosim. 65 267.
  9. S.Kumar, Source Book of Ceramic, 19
  10. A study of ceramic India .in Global era by -S.N Ramsariya , research paper 2003
  11. Alien M. Alper , High temperature Oxides-part -1 – academic press , new York , 1970
  12. F.H Nortion, refractories , 3rd Edn.- Megraw Hill Book Co. Inc, 1949
  13. Jan – Hlavac The Technology of Glass & Ceramics - An Introduction,
  14. Elsevier Scientific Publishing, Co. New York, 1938
  15. S.K. Guha, Ceramic raw Materials of India – A Directory , Indian, Institute of Ceramics, 1928
  16. W.D Kngery, Introduction to ceramics , - John Wiley & sons, Inc, New York, 1960
  17. D.K  Banerjee , Mineral Resources of India, - The World press Pvt. Ltd , Kolkatta, 1992
  18. Indian Minerals Hand Book,- Indian Bureau of Mines , 1998 &1999
  19. M.J Aitken – Thermo. Lumi. Dating ,1985
  20. P.L Soni . Mohan Katyal – Text Book of  Inorganic Chemistry, 2007
  21. K.V.R Murthy , L.H.H Prasad, T.R. Joshi – Thermo. Lumi and it ‘s Applications, Tata Mccrraw – Hill Publishing Company Limited New Delhi, 1992
  22. K.V.R Murthy , V. Natarojan, M.D Shastri -  Lumilnscence &  it ‘s Applications February, 2009
  23. R. Debnath , H.K. Kundu , M.D. Shastri, K.V.R Murthy – Luminscence & it ‘s Applications February -21-2009
  24. K. Mahesh, P.S Weng – C. Furetta – Thermmo. Luni. India Solids And It ‘s Application , 1971
  25. D . J Mc Dougall – Thermo . Lumi . of  Geological Materials, Academic press , London & New York , 1984
  26. Y.H Gandhi, “Thermoluminescence and allied studies of synthetic quartz and its application”, Ph.D. Thesis, pp83, 1995.
  27. Mckeever and Yang, “Point defects and the pre-dose effect in quartz”, Radiation Protection Dosimetry, vol-33, No 1/4, pp27-30, 1990.
  28. R.Chen and Mckeever, “Sensitization of TL in synthetic quartz- heat treatment and radiation effects”, Journal of Luminescence, 48 and 49, pp 833-837, 1991.
  29. H.C.Mandavia,K.V.R.Murthy, Euration Chemico technical Journal, Volume-13, November 1-2,2012,ISSN-1502-3920
  30. H.C.Mandavia,K.V.R.Murthy KCG,Multydisciplinary e-Joural, year-1,essue- 1,October-november-2012,ISSN-2279-0268
  31. H.C.Mandavia,K.V.R.Murthy ,International Journal of Luminescence and Application,Volume-1(11),ISSN2277-6362,p129 to 132 ,8/6/2012
  32. H.C.Mandavia,K.V.R.Murthy , International Journal of Luminescence and 
    Application, Volume-2(1),ISSN-2277-6362,page-15 to 18,9/8/12

*************************************************** 

AUTHOR INFORMATION:

H.C.Mandavia
Shri M. M. Science College,Morbi

Dr. K.V.R.Murthy
Applied Physics Department, M.S.University of Baroda, Baroda

Dr.R.U.Purohit
Joint Director ,Commissioner of Higher Eduction,Gujarat,Gandhinagar

Previous index next
Copyright © 2012 - 2024 KCG. All Rights Reserved.   |   Powered By : Knowledge Consortium of Gujarat

Home  |   Archive  |   Advisory Committee  |   Contact us