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Adsorption of gaseous iodine-131 at high temperatures by silver impregnated alumina

NUCLEAR CHEMISTRY, RADIOCHEMISTRY, RADIOPHARMACEUTICALS AND NUCLEAR MEDICINE

Adsorption of gaseous iodine-131 at high temperatures by silver impregnated alumina

CHENG Qing-Hui
LI Ze-Jun
CHU Tai-Wei
Nuclear Science and TechniquesVol.26, No.4Article number 040303Published in print 20 Aug 2015Available online 11 Aug 2015
35501

To prevent radioactive iodides from releasing into the environment in an accident of a nuclear power plant, silver-impregnated alumina (Ag/Al2O3) was fabricated, and its performance of radioactive iodine adsorption from high-temperature gas was tested. The silver loadings on alumina were obtained by ICP-OES and the texture properties of Ag/Al2O3 were characterized by N2 adsorption-desorption. The Ag/Al2O3 was of reduced specific surface (107.2 m2/g at 650 ℃). Crystalline phases of Ag/Al2O3 were confirmed through XRD characterization. After calcination at 650 ℃ for 2 h, the crystalline phase of Ag/Al2O3 changed. The 131I- removal efficiency of Ag/Al2O3 was tested at 100, 250, 350, 450 and 650 ℃, with good decontamination factor values for the radioactive iodine. Silver-impregnated alumina can be applied as adsorbents to remove radioactive iodine at high temperatures in nuclear accident.

Silver impregnated aluminaHigh temperatureRadioactive iodineAdsorptionDecontamination factor

I. INTRODUCTION

Nuclear energy has been exploited as an alternative to maintain energy sustainability for a half century, while environmental pollution caused by nuclear power plants (NPP) has become a worldwide concern [1, 2], especially in a sever accident of NPPs [3]. In March 2011, large amounts of nuclear dusts were released from Japan’s Fukushima Daiichi NPPs due to failure of cooling systems in a huge earthquake and tsunami. Due to their high mobility, the most dangerous nuclides released in an NPP disaster are gaseous 85Kr and 135Xe, and volatile 131I, 129I, 134Cs and 137Cs, with extensive radioactive hazard to the public [4, 5]. Among them, 131I (t1/2=8.02 d) is the most harmful radionuclide because of its large quantity of release in a nuclear disaster and relatively high activities, and its high accumulation in human thyroid and further damage to organs if ingested; whereas 129I, which decays in a half-life of 1.57×107 a and emits lower energy beta-rays, would do nearly no harm to people [6, 7]. In early stages of the Fukushima Daiichi NPP disaster, gaseous 131I released into the environment was estimated at 1.5×1017 Bq [8-10]. Therefore, how to remove 131I is an important research subject for safeguarding NPPs and the environment.

Great research efforts have been made to prepare adsorbents for 131I removal, such as carbon-based materials [11, 12, 13], silica gel [14, 15], polymer resin [16], titanium based materials [17-20], cyclodextrin [21], molecular sieves [22-24], etc. Also, impregnants have been exploited to improve performance of adsorbents for iodide removal, such as KI [25, 26], TEDA [27, 28] and silver salts [29]. However, most researchers focus mainly on iodide removal from water or gases at low temperatures. Given the fact that an NPP in lost-of-coolant accident is in high temperatures [4], preparation of materials for adsorbing radioactive iodides at high temperatures is meaningful [30].

Alumina is widely applied to manufacture ceramic materials and catalyst supports due to its good heat-resisting properties and large specific surface area [31-33]. In consideration of high affinity between silver and iodide, silver based alumina was exploited in this work as an adsorbent for radioactive iodine at high temperatures.

II. EXPERIMENTAL SECTION

A. Reagents and instruments

Potassium iodate (A.R.): Shantou West Long Chemical Co., Ltd; potassium iodide (A.R.): Beijing Tongguang Fine Chemicals Company; Na131I: HTA CO., Ltd.; L-(+)-tartaric acid (A.R.): Sinopharm Chemical Reagent Co., Ltd.; light petroleum (boiling range of 30–60 ℃, A.R.): Beijing Chemical Works; N2 (high purity): Beijing AP BAIF Gases Industry Co., Ltd.; nitrate silver (A.R.): Beijing Chemical Works; Alumina (neutral, 100–200 meshes): Sinopharm Chemical Reagent Co., Ltd.; nitric acid (A.R.): Shantou West Long Chemical Co., Ltd.

Tube furnace: Beijing Zhongshiyida Science and Technology Ltd.; KL-602 micro-injection pump: Beijing Kelly Med Co., Ltd.; D07-7B mass flow controller: Beijing Seven star Electronics Co., Ltd.; D08-1F flow displayer: Beijing Seven Star Electronics Co., Ltd.; XMT series digital display apparatus: Yuyao Jindian Instruments Co., Ltd.; quartz tube (Φ12 mm×620 mm): Beijing Haiqing Photoelectric Glass Instrument Co., Ltd.; ICP-OES (Prodigy): Leeman Labs; XRD (X’PERT-MRD): Phlips; injector (10 mL): Changzhou Yuekang Medical Appliance Co., Ltd.; ASAP2010 accelerated surface area and porosimetry analyzer: Micromeritics; 2470 WIZARD2 automatic gamma counter: Perkin Elmer; FH463A automatic scaler: Beijing Nuclear Instrument Factory; disposable plastic tube (WG, Φ10–12 mm×75 mm): Zhejiang Plasmed Medical Technology Co., Ltd.

B. Preparation of adsorbent

Silver based alumina was fabricated by the method of impregnation. Alumina was calcined at 450 ℃ for 2 h in a muffle furnace, and allowed to cool in a desiccator. Then, an appropriate amount of alumina was added into nitric silver solution in a light-shading flask at 80 ℃. After 24 h, the as-samples were spun to dry and placed in an oven at 120 ℃ for 2 h, before a 2-h calcination at 450 ℃ in the muffle furnace. Finally the adsorbent was prepared, and Ag/Al2O3 of different calcination temperatures are accordingly marked as "Ag/Al2O3 (T℃ / t h)", where T is calcination temperature and t is calcination time.

C. Silver loadings on alumina

Silver loadings on alumina were analyzed by inductively coupled plasma (ICP). Small amounts of the as-prepared Ag/Al2O3 were mixed with concentrated nitric acid in a flask for 24 h. The filtrate was gathered into a volumetric flask and the silver loadings were confirmed about 10 wt.%.

D. Characterization of adsorbents

Texture properties of the adsorbents were checked by the method of N2 adsorption and desorption on Micromeritics ASAP2010 analyzer. Adsorbents were degassed in advance at 300 ℃ for 2 h. Specific surface areas of adsorbents were measured by the BET method (Brunauer, Emmett and Teller); and the average pore volume was calculated by the BJH method (Barrett, Joyner and Halenda).

To confirm their crystalline phases and check their heat-resisting properties, Ag/Al2O3 of different temperatures were characterized by X-ray diffraction (D/max-2500/PC X-ray diffractometer, Rigaku, Japan), using Cu Kα (the XRD system was operated at 45 kV and 40 mA). The samples were scanned in 0.01 steps from 2θ = 10° to 80°, with the scan rate of 5min-1.

E. Adsorption of radioactive iodine
1. Effect of temperature

In this section, Ag/Al2O3 and Al2O3 were tested to evaluate their efficiency of 131I removal at 100, 250, 350, 450 and 650 ℃. Before the test, adsorbents were calcined at 450 ℃ for 2 h in the muffle furnace.

With trace amount of 131I, I2 was prepared using 2 mL of 2% KIO3 and 4 mL of 166 μg/mL KI (plus 1 mL Na131I), with 1 mL of 5% L-(+)-tartaric acid as acid medium. The I2 was dissolved in light petroleum. The 131I radioactivity in a test was 0.1–2.0 MBq.

The experimental apparatus (Fig. 1) consisted of the 131I-injection, heating and off gas purification sections. Radioactive iodine solution was injected by micro-injection pump in 2.5 mL/h of injection rate. High purity N2 at a flow rate of 35 mL/min was used as carrier gas. In the experiment, the adsorbents were laterally loaded in the tube center to adsorb 131I at different temperatures. A typical test with 1 g adsorbents in 5 mL light petroleum was done in 2 h. 13X (including Ag/13X zeolites, less than 40 meshes) and saturated NaOH solution were used to trap131I in the off gas [30]. After test, the spent adsorbents were imbedded in the disposable plastic tubes to detect radioactivity on the gamma counter. The decontamination factor were calculated by DF=(A+B)/B, where A is the radioactivity of spent adsorbents and B is the summation of radioactivities of the off gas purification columns. The DF values were normalized to DF/g.

Fig. 1.
Flow chart of the experiment.
pic
2. Effect of I2 concentration

To study whether I2 concentration would influence 131I-adsorbing performance of adsorbents, the KI concentration used as the source to produce iodine, was increased to 332 μg/mL, other details were the same as above.

3. Effect of N2 flow rate

Considering that the flow rate of carrier gas may affect 131I removal, N2 flow rates of 15–75 mL/min were used to measure the removal efficiency of adsorbents at 250 ℃. Other details were the same as above.

4. Effect of adsorption time

To check time-depenence of the interaction between Ag/Al2O3 and iodine, DF values in interaction durations of 30–180 min were measured at 100 ℃ and 450 ℃ under the N2 flow rate of 35 mL/min. Iodine (dissolved in light petroleum) produced by the KI (166 μg/mL, Na131I-included) was kept in a glass container. The amount of Ag/Al2O3 is about 1 g. As an example, the DF value of 30-min time point was measured as follows. Iodine dissolved in light petroleum was constantly injected by the micro-injection pump at 2.5 mL/h for 30 min, and radioactivity of the adsorbed 131I was measured to calculate the DF values.

III. RESULTS AND DISCUSSION

A. Adsorbents characterization
1. Texture properties of Ag/Al2O3

Texture properties of adsorbents and support were characterized by the method of N2 adsorption-desorption at 77 K. Figure 2 shows the N2 isotherms of alumina, Ag/Al2O3 (450 ℃/2 h) and Ag/Al2O3 (450 ℃/2 h + 650 ℃/2 h). The alumina maintained a mesoporous structure, which was in accordance with the calculation results by BJH method (average pore diameter of 4.5 nm). After loading silver on alumina, the Ag/Al2O3 (450 ℃/2 h) and Ag/Al2O3 (450 ℃/2 h + 650 ℃/2 h) were still of the mesoporous structure, with an average pore diameter of 5.2 and 6.4 nm (BJH method), showing a little increase after silver loading. An adsorption hysteresis occurred when the relative pressure (p/p0) reached to 1, i.e., all N2 isotherms were attributed to Type IV.

Fig. 2.
N2 adsorption-desorption isotherms of different adsorbents.
pic

As shown in Table 1, the Ag/Al2O3 samples were of relatively large specific surface area, being [per-mode=symbol]129.1 and 107.2 m2/g after 450 ℃/2 h and 650 ℃/2 h calcinations, respectively, though they were smaller than that of Al2O3.

TABLE 1.
Texture properties of Al2O3 and Ag/ Al2O3
Adsorbents SBET (m/g2)
Al2O3(450 ℃/2 h) 146.1
Ag/Al2O3(450 ℃/2 h) 129.1
Ag/ Al2O3 (450 ℃/2 h + 650 ℃/2 h) 107.2
Show more
2. XRD spectra of adsorbents

Silver impregnated alumina had the characteristic diffraction peaks of alumina from the XRD spectrum (Fig. 3), i.e., it maintained a stable structure after silver impregnated. To be specific, silver on alumina had nearly no effect on the alumina structure. In the XRD spectrum of Ag/Al2O3 after 450 ℃/2 h calcination, the diffraction peaks of silver particles can be seen clearly. For Ag/Al2O3 (450 ℃/2 h + 650 ℃/2 h), the crystalline phase of alumina changed, and the Ag diffraction peaks indicate sintering of the silver particles during the 2-h calcination at 650 ℃.

Fig. 3.
XRD spectra of Al2O3 and Ag/Al2O3.
pic
B. Adsorption of radioactive iodine
1. Effect of adsorption temperature on 131I-removal efficiency

The silver-impregnated alumina performs better in 131I-removal than alumina at the same temperatures under N2 flow rate of 35 mL/min. As shown in Fig. 4, the 131I-removal efficiencies of both Al2O3 and Ag/Al2O3 decrease with increasing temperature of adsorption. However, DF values of the silver-impregnated alumina were 806.9 at 450 ℃ and 306.7 at 650 ℃; while the DF values of alumina declined rapidly from 437.8(250 ℃) to 16.1(650 ℃).

Fig. 4.
(Color online) Adsorption of 131I at different temperatures by Al2O3 and Ag/Al2O3 under N2 flow rate of 35 mL/min.
pic

Despite its reduced specific surface area (107.2 m2/g for Ag/Al2O3, while 146.1 m2/g for alumina), Ag/Al2O3 has higher DF value, as the silver particles can react with iodine from high-temperature gas to form AgI.

2. Effect of I2 concentration on removal efficiency

I2 concentrations of 166 μg/mL and 332 μg/mL were used to study the I2 effect of dose on 131I-adsorbing performance of the Ag/Al2O3 at N2 flow rate of 35 mL/min. The results are shown in Fig. 5. The Ag/Al2O3 was of high 131I-removal efficiency at 350–650 ℃ under both the KI concentrations, though the Ag/Al2O3 at I2 concentrations of 166 μg/mL performed better at <300 ℃.

Fig. 5.
(Color online) Effect of I2 concentration on 131I-adsorbing performance of Ag/Al2O3 at N2 flow rate of 35 mL/min.
pic
3. Effect of N2 flow rate on 131I-removal efficiency

The effect of N2 flow rate on 131I-removal efficiency of adsorbents was carried out at 250 ℃, with N2 flow rate varying from 15 mL/min to 75 mL/min. As shown in Fig. 6, DF values changed little in the entire range of the N2 flow rate.

Fig. 6.
Effect of N2 flow rate on 131I-adsorbing performance of Ag/Al2O3 at 250 ℃.
pic
4. Effect of adsorption time

The interaction between Ag/Al2O3 and iodine was studied at 100 ℃ and 450 ℃ under N2 flow rate of 35 mL/min by measuring the 131I-removal efficiency in different durations of the adsorption (Fig. 7). The DF value of Ag/Al2O3 increased with time till 100 min, where it reached to a plateau. Therefore, the Ag/Al2O3 can achieve desirable result of 131I-removal in adsorption time of 100 min at N2 flow rate of 35 mL/min.

Fig. 7.
(Color online) I-131 adsorption kinetics curve of Ag/Al2O3 at 100 and 450 ℃ under N2 flow rate of 35 mL/min.
pic

IV. CONCLUSION

In this work, silver impregnated alumina was prepared and evaluated for its removal efficiencies of radioactive iodine at high temperatures (100, 250, 350, 450 and 650 ℃). The results suggested that: alumina would perform better for adsorption radioactive iodine at high temperatures after silver loaded; the differences of removal efficiencies among different flow rates of carrier gas were small. Silver impregnated alumina would be applied as adsorbents to remove radioactive iodine at high temperatures during nuclear accident.

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