ISSN : 0970 - 020X, ONLINE ISSN : 2231-5039
     FacebookTwitterLinkedinMendeley

Incorporation of Nuclear Wastes in LIP and Uranium Containing LIP Glasses

A. Ghosh1, G. Hazra2, P. Mitra3 and T. Das1,*

1Dept. of Chemistry, The University of Burdwan, Burdwan  713 104, India 2Dept. of Chemistry, Kalna College, The University of Burdwan, Burdwan 713409 ,India.

3Dept. of Physics, The University of Burdwan, Burdwan   713 104, India

DOI : http://dx.doi.org/10.13005/ojc/300111

Article Publishing History
Article Received on : December 12, 2013
Article Accepted on : January 19, 2014
Article Published : 29 Mar 2014
Article Metrics
ABSTRACT:

Glasses in lead-iron phosphate (LIP) system loaded with simulated nuclear waste, were melted in the temperature range750-950oC. Some of the LIP glasses were mixed with uranium salt. The pH determinations of the leachate solution at normal temperature show some interesting trends. Leaching study of these glasses with a maximum time period of 300 hrs. were conducted under Soxhlet distillation condition with distilled water. Weight losses and residual activities by ‘Radiotracer technique’ were followed with respect to cumulative time period of leaching. For some LIP-glass samples containing uranium the leach rates as calculated from BET surface area measurements. They were in the range 8.2 x 10–4 to 1.8 x 10–3 g.m-2.hr-1 at 90°C. DTA endotherms occur at ~400oC and ~900oC for the LIP glasses. FTIR studies show absorptions at ~532, ~1025, ~1620-1640, ~2365 and ~3440-3490 cm–1. SEM of some selected glasses was reported. The variation of different properties was explained in terms of the changes in the ionic potentials of the different modifier ions. The model structure of glasses has been considered taking the dual role of and as glass formers/ modifiers which ultimately has an effect on the chemical durability of these glasses.

KEYWORDS:

future; development; nuclearpower plants Glass offers .

Download this article as: 

Copy the following to cite this article:

Ghosh A, Hazra G, Mitra P, Das T. Incorporation of Nuclear Wastes in LIP and Uranium Containing LIP Glasses. Orient J Chem 2014;30(1)


Copy the following to cite this URL:

Ghosh A, Hazra G, Mitra P, Das T. Incorporation of Nuclear Wastes in LIP and Uranium Containing LIP Glasses. Orient J Chem 2014;30(1). Available from: http://www.orientjchem.org/?p=2533


Introduction

The future development of nuclear energy depends largely on the success of programmes and management of radioactive wastes generated at various stages of the nuclear fuel cycle. A nuclear (radioactive) waste is any material that contains or is contaminated with radionuclides at concentrations greater than a certain safe (permissible) level. Radioactive wastes are generated from the various sources such as nuclear power plants, medical isotope applications, defence, communication systems and atomic industries. The fission products with the usual fuel materials viz., U, Pu, and Th contain about 35 elements with 200 different isotopes. Besides the fission products, the waste contains unrecovered U, Pu, corrosion products like Fe, Co, Ni, Al, Na and the anions NO3 and SO42–. The corrosion products come from the stainless steel process vessels, which are attacked by acid solution [1]. Glass offers a medium for waste containment since it has the ability to dissolve most of the elements of the periodic table. The fission product constituents thus become a part and parcel of the glass structure as compared to any other mechanical entrapment. Glass can be considered as a truly ‘secular’ matrix, imbibing in one melt all the elements contained in the waste. This results in a permanent and irreversible fixation of the nuclides in the various matrix. Glass has very high leach resistance, i.e., it does not dissolve easily in water. High leach resistance is one of the most desirable properties of the solid matrix used to immobilize the fission product. It is the leach resistance value which dictates the selection of glass as a nuclear waste glass [2]. Since these glasses are to be stored for several thousand years under such conditions before the radioactivity dies down, corrosion study of such glasses under varying environmental conditions is helpful in understanding the durability and fission product release from such glasses. Since millions of curies of activities will be stored in such glasses emanating huge amount of radiation, it will be useful to see the effect of radiation on leachability. Lead iron phosphate glasses have several advantages such as lower aqueous corrosion rate, lower processing temperature, etc [3].  In addition, these glasses did not vitrify upto 550oC. Lead iron phosphate glasses (LIP) are a potential candidate for immobilization of high level commercial and defence radioactive waste with leach rate 102 – 103 times lower than the leach rate of a comparable borosilicate waste glass [4]. The composition of the nuclear wastes used in the present work is shown in Table 1.

Table 1 Compositional details of simulated low and intermediate level radioactive liquid waste

 

Sr. No. Properties Low level radioactive liquid waste Intermediate level radioactive liquid waste
1 PH 8-9 9-13
2 CsNO3 (milimoles/L) 6.56´10-6 8.39´10-4
3 Sr(NO3)2 (milimoles/L) 2´10-6 2.4´10-5
4 RuCl3 (milimoles/L) 2´10-9 2.93´10-7
5 NaNO3 (moles/L) 1´10-2 2
6 Na2CO3 (moles/L) 5´10-2
7 CaCl2 (moles/L) 2´10-3
8 NaOH (moles/L) Traces for adjustment of pH 5´10-3

 

Experimental

Preparation of glass batches and melting operation

The glass batches used in the present work were prepared from the ingredients like quartz powder (AR grade, Oxford laboratory reagent) as source of silica, Borax (AR grade, RANKEM), PbO (AR grade, Dipak laboratories), BaO (AR grade, Boroyne), CeO2 (AR grade, Hi Media), SrO2 (AR grade, Aldrich), uranyl acetate (AR grade, BDH) and Fe2O3 (AR grade, Dipak laboratories). As source of lead, two ingredients were tried, viz., PbO and Pb3O4. The ingredients were dried and taken in a alumina crucibles and fired in a muffle furnace fitted with programmer in the range 750 – 1000°C for soaking periods of 30 min – 60 min in air. The oxides SiO2, B2O3 and P2O5 act as the glass former while PbO act as intermediates and BaO, SrO2,CeO2 and Fe2O3 act as modifiers. The compositions used in the present work are shown in Table 2. The selection was based on that supplied by Nuclear Recycle Group (BARC) and also from some predetermined compositions [5] after reviewing of earlier works in reference to the corresponding ternary diagrams. Some of the LIP glasses [LIP 8 – LIP 10] were composed by taking uranyl acetate directly into itself since U is active and by measuring the net counts per sec (cps),  the leaching characteristics can be traced by ‘radiotracer technique’ with the help of a Geiger-Muller counter. For the pH determination of the leachate solution, the bulk glass was powdered to 0.3 – 0.425 mm size. One (1) gm of the glass powder was taken in a beaker with 40 ml  distilled water. And it was stirred with a magnetic stirrer for 2 minutes. The pH of the liquid was determined by a pH meter (Systronics digital pH meter, Model 335). Such measurements of pH were carried out at regular intervals of 1 hr., 2 hr., 3 hr., 4 hr. and 5 hr.

Figure: 1 Soxhlet apparatus Figure: 1 Soxhlet apparatus

Click here to View Figure

 

respectively. The mixture was stirred after each 15 minutes. For U-containing LIP glasses, the leachate extract after each operation of leaching for varying time intervals was subjected to pH measurement. For leaching studies, the glass samples were crushed to 300 – 425 mesh taken in a nylon net. Then 0.5 gm of each sample glass was vapor distilled in Soxhlet apparatus with a round bottom flask (500 ml. capacity) fitted with a condenser [6]. The distillation was carried out for varying period of time up to a maximum of 300 hr. The heating was done in a heating mantle. The arrangement is shown in figure 1. The weight loss after each run of leaching was measured by a four-decimal electronic balance (Satorius) and was converted into % wt. loss.  In order to find the leach rates, BET surface area of the U-containing LIP glasses were determined under liquid nitrogen temperature [7]. For LIP glasses, the leaching study was augmented by noting the cps after each interval of time from its residual activity of α and/or β with the help of a G–M counter (Nucleonix, Hyderabad, India).  To obtain information about the thermal characteristics of LIP glasses, Differential thermal analyzer [Perkin-Elmer Diamond TG/DT analyzer] was employed in the range 30 – 900°C under N2 atmosphere, with a rate of 5°C/min using α-Al2O3 asreference. Higher temperatures were deliberately omitted since melting point of such glasses is close to it. FTIR spectrum of the glasses LIP 8 – LIP 10 was recorded by a spectrometer [Perkin-Elmer FTIR model RXL spectrometer] using KBr pellet. SEM image of some glasses were recorded in a Scanning electron microscope [S-530, Hitachi, Japan].

Table  2 Different Glass Compositions prepared (wt %)

 

Glass

SiO2

PbO

BaO

Fe2O3

CeO2

SrO2

P2O5

Uranyl acetate

LIP3

49(Pb3O4)

8

10

33

  LIP4

52.4

7.9

6.5

33.2

LIP5

49(Pb3O4)

8

10

33

LIP6

49(Pb3O4)

8

5

5

33

LIP7

49(Pb3O4)

10

8

33

LIP8

52.4

7.9

33.2

6.5

LIP9

51.4

7.9

10

33.2

7.5

 LIP10

45.8

7.0

30.2

7.0

 

Results and Discussion

Table 3 shows the melting temperature and time of melting of different glass compositions obtained in the present work. X-ray diffraction study showed that the products to be amorphous. In melting operation, the temperature and time of meting are the principal factors to be monitored. In the present work we could melt the glass at much lower temperature (750-950oC) with a soaking period of 30 min -1 hr which were earlier reported to be melted not below 10000 C. The melting temperature of the glass LIP4 was found to be appreciably lower (750oC) in comparison to other glasses [10]. It may be mentioned that in case of LIP4, the modifier oxide is PbO while for others it is Pb3O4 [11]. The variation in melting points is due to mixed effect of different modifier ions, the exact trend being difficult to

 

 Figure: 2 Plot of pH vs Time for BS and  LIP glasses Figure: 2 Plot of pH vs Time for BS and  LIP glasses

Click here to View Figure

 

speculate. Considering that the glass will be utilized to incorporate nuclear waste with some of the fission fragment like RuO which is highly volatile, the lower the glass processing temperature the better will be the utility of the glass melt. The effect of different modifier ions like , , and  on the melting points and time of melting is quite evident. The results of pH studies are shown in figure 2. Figure shows the plot of variation of pH against time (in hour) for different glass systems. The curve for LIP 7 runs lowest. The slightly increasing trend in the pH values may be due to the mixed oxide of phosphate system. The observed pH values are in good agreement with the equilibrium pH values of glass system having composition close to present work [5]. The result can be explained considering the following equilibrium in the aqueous system:

Vol30_No1_Incor_Ghosh_F1

Table 3 Melting Temperature (°C) and Time of Melting of different glass compositions

 

Glass

M. P. (± 2oC)

Time( mins)

LIP3

950

30

LIP4

750

30

LIP5

900

30

LIP6

900

30

LIP7

950

30

LIP8

900

60

LIP9

900

60

LIP10

950

60

 

 

the extent of which (i.e., the forward or  the reverse direction) is influenced by the different modifier ions released during the leaching of the glass sample. The ionic radii (Å) of the different modifier ions in our case are Pb2+ (1.33), Ba2+(1.35),Fe3+ (0.69), Ce4+(1.18) and Sr4+ (1.13). The corresponding ionic potential increases as Ba2+ (1.48) < Pb2+ (1.5) < Sr4+  (1.54) <Fe3+  (3.39) <Ce4+ (4.69).  Now greater the ionic potential of , more it will attract  ions to form the corresponding hydroxides . This formation of hydroxide shifts the dissociation of in the forward direction releasing more number of ion in the medium. Thus the resulting solution will increasingly become acidic with lowering value of pH. The LIP 8 glass contains uranyl acetate (7.0 wt%). Since U can act as a good glass former, the resulting glass does not dissociate and the pH value flattens out at a value just below 6.75. Leaching operation was done under Soxhlet distillation condition. For glasses not containing uranium, the results of % wt. losses at each stage (time in hr.) were taken. For U-containing glasses the wt. loss data was further accompanied from the results of ‘radiotracer technique’ (cps vs. cumulative time). Figure 3 shows the corresponding plots. It is observed that with increasing cumulative time, the net cps (alpha or beta) is decreasing in an exponential way signifying that with increasing leaching time, the release of uranium along with other constituents becomes slower and slower until getting stopped.

Figure: 3 Net CPS vs. Cumulative time for (o) LIP8, (∆) LIP 9 and (▼) LIP10 Figure: 3 Net CPS vs. Cumulative time for (o) LIP8, (∆) LIP 9 and (▼) LIP10

Click here to View Figure

 

Vol30_No1_Incor_Ghosh_F2

Thus the glass becomes resistant to leaching and is a better choice for the disposal of nuclear waste compared.  In case of LIP9 glass, a similar type of plot is obtained. The exponential decay must not be confused with the decay of U238, the present isotope present in the system, since its half life period is too high (~108 years) to be reflected in such decay. The leach rates (LR) for LIP8 and LIP9 after leaching are  determined from BET surface area analysis. These are 1.8×10-3 g.m-2.hr-1 and 8.2×10-4 g.m-2.hr-1 respectively. The leach rate (LR) were measured by weight loss according to the relationship where and are the initial and final sample weights respectively,  is the  BET surface area of the sample and  is the time exposed to the leachant. These rates as compared to other borosilicate a system is 1000 times lower (13) and thus LIP glasses have much improved chemical durability. This is due to  content and structural role of , which strengthens the cross bonding between the polyophosphate chains. Percent weight loss studies show a distinct decrease in the % wt.  loss value with extended  period of time of leaching signifying that the extent of leaching die down with time (Figure 4). It is observed that the %   wt. loss decreases in the order

(LIP 10) > (LIP 8) > (LIP  9)

 

Figure: 4 Percent wt. loss vs. Cumulative time Figure: 4 Percent wt. loss vs. Cumulative time

Click here to View Figure

 

In case of the glass LIP9, CeO2 is present which is not present in LIP8 and LIP10 other. Thus the role of Ce as binder modifier is evident.

Figure 5shows the DTA study of U-containing LIP9 glass and Figure 6 shows the same for LIP10 glass. The thermograms of the above glass samples were taken in the

 

Figure: 5 DTA Thermogram of  LIP 9 Figure: 5 DTA Thermogram of  LIP 9

Click here to View Figure

 

range 30 – 900°C. The endotherm at ~400oC is due to the peak crystallization temperature . This corresponds to the transition temperature of the base glass. The peak at ~900oC corresponds to the liquidus temperature (TL) which corresponds to the melting of the crystalline phase. Figure 7 and Figure 8 shows the FTIR spectrum of LIP 9 and LIP 10 glasses respectively. Major stretches are observed at ~532, ~1025, ~1620-1640, ~2365 and ~3440-3490 cm-1 respectively.

 

http://www.orientjchem.org/wp-content/uploads/2014/04/Vol30_No1_Incor_Ghosh_Figure6.jpg Figure: 6 DTA Thermogram of  LIP 10

Click here to View Figure

 

The IR stretch at ~532 cm-1 may be related to the to phosphate motion (P–O bending vibration) [15], the one at ~1025 cm-1  is related to the symmetry stretch of non-bridging  oxygen [16]. The stretch at ~2365 cm-1 stretch is related to P-OH stretching [17] and the one in the range 3440-3490 cm-1 is related to the OH stretching (phosphate glass absorbs moisture from  atmosphere). Figure 9 shows the SEM images of some selected glass systems. The pictures reveals homogeneous nature of that the glasses formed.

 

Figure: 7 FTIR Spectrum of  LIP 9 Figure: 7 FTIR Spectrum of  LIP 9

Click here to View Figure

 

Figure: 8 FTIR Spectrum of  LIP 10 Figure: 8 FTIR Spectrum of  LIP 10

Click here to View Figure

 

Figure: 9 SEM Photomicrograph of (a) LIP7 and (b) LIP10 glass Figure: 9 SEM Photomicrograph of (a) LIP7 and (b) LIP10 glass

Click here to View Figure

 

Conclusion

The combination of lead phosphate glasses with various types of simulated nuclear waste showed that it is possible to have a waste-form with corrosion rate 1000 times less than that of a comparable borosilicate glass. The addition of iron to lead phosphate glass was found to increase the chemical durability of the glass and to suppress the tendency for crystallization on cooling and reheating. The durability test shows that the alkaline earth oxides BaO and SrO decrease the durability while PbO improves the corrosion resistance. LIP glasses have several distinct advantages: (i) Solidified forms have dissolution rates in water about several orders lower than comparable borosilicate formulations.  The addition of iron to lead phosphate glass was found to dramatically increase chemical durability of the glass ( by a factor of about 104 for  9 wt % iron oxide addition), (ii) a processing temperature that is 100° to 250°C lower. Effect of modifier ions on melting temperature is evident in the present work and (iii) a much lower melt viscosity in the temperature range from 750° to 950°C. Most significantly, the lead-iron phosphate waste form can be processed using a technology similar to that developed for borosilicate nuclear waste glasses.

Acknowledgements

Discussions with Dr. J. Mukerji and Dr. A. S. Sanyal, retired Scientists, CGCRI, Kolkata, is duly acknowledged. The help rendered by Dr.  N. Dutta, Bankura Unnayani Institute of Engg., W.B., in setting the Soxhlet system is acknowledged. Financial assistance by DSA (Chemistry) and CAS (Physics) and state funded fellowship provided to one Research Fellow (A. G.) is also acknowledged.

References

  1. Mukerji J., Sanyal A. S., Glass Technol., 45, 117 (2004).
  2. Day D. E.,  Atm. Environ., 35, 5169 (2001).
  3. Sales B. C.,  Boatner L. A., Science, 226, 45 (1984).
  4. Day D. E.,  Chandra S. R., Kim C. W., Annual Report for DOE FG07-96ER45618. University of Missouri-Rolla, Rolla, MO (USA): 2002 June.
  5. Malik P. P., Hajra G., Mitra P., Das T., Prog. in Th. and Appl. Phys., 1, 01 (2013).
  6. Sanyal A. S., Mukerji J., J. Scientific & Industrial Res.,  33, 436 (1974).
  7. Yanagi T., Yoshizoe M., Nakatsuka N., J. Nuclear Sc. and Technol., 25,  661 (1988).
  8. Reis S. T., Martinelli J. R., “J. Non-Cryst. Solids., 274, 241 (1999).
  9. Islam M. M., Holand D.,  Scales C. R., Phys. Chem. Glasses – European J. Glass Sc. and Technol B., 49, 229 (2008).
  10. Hazra G., Das T.,  Mitra P., “Role of lead as modifier on the properties of lead iron phosphate glasses”, Proc. of Nuclear and Radiation Chem.; 2011 Feb 22-26; Vishakhapatnam (India). p. 449-450.
  11. Jana S., Karmakar B., Kundu P., Mat. Sc. Pol., 25, 1127 (2007).
  12. Fang X., Ray C. S., Milankovic A. M., Day D. E., J. Non-Cryst. Solids, 283, 162 (2001).
  13. Yanagi T., Yoshizoe T., Kuramoto K., J. Nucl. Sc. and Technol., 26, 948 (1989).
  14. Shih P. Y., Mat. Chem. Phys., 84,  151 (2004).
  15. Hudgens J., Brow R. K., Tallatant D. R., Martin S. W., J. Non-Cryst. Solids, 223, 21 (1998).
  16. Doweidar H., Moustafa Y. M., El-Egili K., Abbas I., Vibrational Spectros., 37, 91 (2007).
  17. Brow R. K., Tallant D. R., Myers S. T., Phifer C. C., J. Non-Cryst. Solids, 191, 45 (1995).


Creative Commons License
This work is licensed under a Creative Commons Attribution 4.0 International License.