Abstract
Indoor radon (222Rn) was surveyed in a total of 141 individual houses and apartments used precalibrated passive PicoRad Detectors. The radon activity in the soil gas around the dwellings was simultaneously measured. The arithmetic mean values of indoor radon concentrations for detached houses, old buildings (up to four-stories), prefabricated blocks of flats (mostly five stories) and high-rise residential buildings (10-stories) were:, 70.9; 46.5; 38.4, and 56.6 Bq m−3, respectively. The average arithmetic mean value for all measured rooms equals 51.8 Bq m−3. The calculated average effective dose from indoor radon for the local population was equal to 2.2 mSv.
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Introduction
Large scale epidemiological case–control studies with subsequent individual data analysis from 13 European teams showed a linear growth of the cumulative risk of death from lung cancer with an increase in indoor radon concentration [1]. For the practical implementation of a radon protection strategy, the International Commission on Radiological Protection (ICRP) recommended an integrated approach for protection against radon exposure in all buildings, irrespective of their purpose or the status of their occupants. It also introduced an upper value of the derived reference level of 300 Bq m−3 for 222Rn in dwellings [2]. A similar approach was proposed in the EU (European Union) Commission’s recommendations. Under the national action plan, Member States should promote action to identify dwellings with radon concentrations (as an annual average) exceeding this reference level [3]. Moreover, the Commission strongly encourages national authorities to set a national derived radon reference level as low as reasonably achievable in the range of 100–300 Bq m−3.
However, due to new epidemiological findings and the application of dosimetric models, the ICRP now suggests using nominal probability coefficients for radon exposure that are larger by a factor of almost 2 than in the former ICRP and UNSCEAR recommendations [4]. This approach leads to the doubling of the risk per unit exposure as a result of it also doubling the dose coefficients from 9 × 10−6 to 16.8 × 10−6 mSv Bq−1 h−1 m3. Thus, an identical radon exposure situation with the new dose coefficients would result in a doubling of doses compared with the former values. This has serious conceptual implications and is still being discussed [5].
Moreover, taking into account the new dose conversion factor for an annual indoor occupancy of 7000 h and an equilibrium factor of 0.4 for radon daughters, one can easily calculate annual effective doses for inhalation of radon daughters by members of public as being equal to 5.2 mSv and 15.6 mSv for indoor radon concentrations of 100 Bq/m3 and 300 Bq/m3, respectively. This range of doses can be compared with that of the 5–10 mSv year−1 range, recommended by the ICRP for the protection of aircraft crew occupationally exposed to cosmic radiation at typical flight altitudes of 8–12 km [6]. Although the EU Directive EU 2013/59/EUROATOM obligates its Member States to promote action to identify dwellings with radon concentrations (as an annual average) that exceed the reference level of 300 Bq m−3, the classification of the radon-prone areas should be reviewed, and the areas where the expected indoor radon concentration is around 100 Bq/m3 should also be included for intense survey actions.
There are several commonly used types of detectors to survey radon, for example, solid-state alpha track, activated charcoal adsorption, or active instrumental detectors [7]. To better estimate long term exposure (3 to 12 months) to 222Rn, the use of solid-state nuclear track detectors is recommended [8]. However, we previously proved that passive diffusion activated charcoal canister PicoRad detectors, which require only 24–48 h exposition, followed by 8 h radon elution to liquid scintillation solution, can also be used for the annual indoor radon inhalation dose assessment [9]. This method has been successfully used by us for large scale surveillance of indoor radon [10,11,12]. This method also allows correction for temperature fluctuations in the examined rooms, if necessary [13].
In our previous studies of the indoor radon concentrations in kindergarten and schools in Kalisz, we found that in more than 10% of the examined sites, the indoor radon activity concentration exceeded 100 Bq m−3, whereas the median value was a relatively low 31.5 Bq m−3 [14]. In the literature, one can find many papers dealing with the influence of various factors, including radon in sub-surface soil gas concentration and its transport to the higher floor levels, on indoor radon concentrations in residential buildings. Generally, so-called geogenic potential and building construction, including radium concentration in building materials and the radon exhalation rate from these materials, are recognized as major contributors to indoor radon levels [15]. Recently in Poland, a country-wide indoor radon survey was carried out, although it was limited mostly to small detached houses. Thus, the obtained average annual indoor radon concentration for the whole country of 160 Bq m−3 seems to be exaggerated [16], since it does not take into account fact that the almost 60% of the Polish population lives in towns where people predominantly live in prefabricated blocks or high-rise buildings.
The goal of this study was to extend the indoor radon survey to different types of building to evaluate residential radon activity concentration distributions and, consequently, to assess the radiological risk for the local population.
Experimental
Location description
Kalisz is the second-largest city in the Greater Poland region, after Poznan, with a population of around 1,08,000 and covering an area of 69.8 km2. The city is located on the east border of the Fore-Sudetic Monocline in the Prosna river valley with an elevation of 108 m above sea level. In the deeper layers of the soil in the city limits, the occurrence of Jurassic, Upper Cretaceous, Tertiary, and Quaternary deposits have been found. The average annual temperature is 8.4 °C, and the mean annual precipitation is about 511 mm. The urban space consists of a city center with buildings up to four stories that date from the beginning of the 20th century. They are surrounded by prefabricated blocks of flats and densely placed detached houses. Close to the city border, there are a few sites with the modern detached houses (see Fig. 1). The Arabic numbers denote the number of flats in a given area, where measurements were conducted.
Calculating radon entry into different types of buildings
Radon entry into a building greatly depends on the construction and building materials. For the model standard room, the resulting indoor radon concentration can be described by a linear differential equation [17]:
where: V—volume of the room (m3), Qo—airflow to the room (m3 h−1), Aa—radon concentration in the incoming air (Bq m−3), E—222Rn exhalation rate from the walls in (Bq h−1), λe—air escaping (exchange) rate (h−1), λd—222Rn decay constant = 7.5 × 10−3 (h−1) and A—indoor radon concentration in (Bq m−3). Substituting the total radon influx per one cubic meter of indoor air:
and for low ventilation rates: λe ≫ λd Eq. (1) becomes:
For the simplest situation, when the 222Rn influx is constant—R for a certain period and assuming that for t = 0 the starting indoor radon activity is equal to A0, one can get the following solution to Eq. (3):
If the equilibrium radon activity, Aeq, is settled in the room after a certain period, then dA/dt = 0 and from Eq. (3) one can get:
Substituting the expression Aeq = R/λe into Eq. (4) one can get finally:
where B = ln(1 − A0/Aeq) is assumed to be constant during the time of the experiment.
Therefore, checking (after complete ventilation of the room) the activity ingrowths from A0 to an equilibrium activity of Aeq as a function of time –t, one can get a radon in air exchange ratio-λe from the linear dependence of (6). Moreover, from Eq. (5), the total radon influx R- into the examined room can be calculated.
Such measurements can be performed by means of the Sarad EQF3220 device.
Indoor radon sampling and counting
Commercially available PicoRad plastic liquid scintillator vials with charcoal detectors were purchased from AccuStar (USA). According to the country-wide indoor radon survey, the average monthly indoor radon concentration values observed for Central Poland in March and April, as well as September and October, are very close to the annual average values [16] These data are close to those obtained for Northern Poland, where the correction coefficients were in the range of 0.9 to 1.15, except for March and three summer months—June, July, and August [18]. The vials were exposed for 48 h in 2017 and 2018 (except for the above mentioned months). The whole laboratory procedure, including the calibration of each set of PicoRad detectors was basically the same as those previously published [14]. The activities of the eluted 222Rn and its four short-living daughters were measured (at least 8 h from the beginning of elution) in the fixed channels of the liquid scintillation counter Beckman 3801 for 1 h each sample. The spectrum of radon and its daughters as well as the details of the optimal counting channel choice was reported elsewhere [19]. However in these experiments the average so –called calibration coefficient K was calculated from formula:
where ARn is the 222Rn activity concentration in (Bq m−3) and I- average of net activities of three PicoRad calibration vials (cpm) measured in optimal canal of the Beckman counter. Such calculated value of calibration coefficient equal to 1.43 ± 0.08 was used for the routine indoor radon concentration determinations.
The determination level- LO of the indoor radon activity concentration using Currie < s formula for a counting time of 3600 s and background in the optimal channel B = 14,5 cpm, was equal to 8 Bqm−3. A total relative standard deviation of the single indoor radon measurement for its concentration of 45 Bqm−3 (an average value for the Kalisz area), taking into account also the standard deviation of the calibration coefficient, didn’t exceed 7%.
The quality assurance of this method was confirmed with satisfactory results obtained during the country-wide interlaboratory radon in an air comparison experiments, organized in 2018 by the Central Laboratory of Radiological Protection in Warsaw, Poland.
Determination of radon in soil gas in the vicinity of detached houses
222Rn nuclide concentration in soil gas was determined in four points around each detached house site by the method described elsewhere [20]. The soil gas was removed on days without rain, usually at noon, by a typical hollow tube probe from 100 cm below ground level by 10 min sucking of about 3 dm3 gas and passed directly through 16 ml of water-immiscible liquid scintillator placed in standard 20 ml scintillation vials. The activity of absorbed radon nuclides was measured by the TRIATHLER device, and the 222Rn concentration in the soil gas was calculated on the basis of the previously described procedure [21].
Results and discussion
Radon entry rates for detached single-family houses
The linear dependence described by Eq. (6) for radon influx into two rooms in the same house is presented in Fig. 2.
The radon entry parameters were calculated based on the obtained linear relationships according to Eq. (6) for different rooms in detached houses (Table 1).
The low values of the radon entries (R < 10 Bq/m3 h−1) and resulting low indoor radon equilibrium concentrations (below 100 Bq m−3) were typical for houses with careful basement isolation finishing. However, comparing the indoor radon concentrations in the ground floor and first floor rooms (A0/A1) with corresponding radon entries (R0/R1) shows a lack of correlation. It indicates that a simple assumption that incoming air on the ground floor and first floor is characterized by the same radon concentration, Aa, is not valid. It is obvious since incoming soil gas with higher 222Rn concentration makes a substantial contribution in the ground level rooms, whereas for the first floor rooms, air from ground level rooms, as well as from outdoors, with low 222Rn concentration, is mostly transported. Nevertheless, the radon entry values in the ground level rooms calculated by the elaborated simplified method can be a valuable tool in predicting whether that particular house construction will be a “radon-resistant” solution or if it needs further basement sealing work.
The fluctuation of daily indoor radon concentrations in two rooms determined by 3-day consecutive exposition of PicoRad vials for 1 month
The PicoRad method, from its nature of 48 h exposition, gives a very good averaging of diurnal radon fluctuations in the examined rooms. The crucial problem for applying the PicoRad method for indoor radon evaluation is the relation between one single measurement using that method and the average monthly 222Rn concentration. Therefore, the PicoRad detectors were exposed continuously for 3 days in two rooms for 1 month. The fluctuations of the radon concentrations during this time are shown in Fig. 3.
The measured indoor radon concentrations for ground and first floor rooms were in the range of 76.5 to 105 Bq −3, with an arithmetic mean of 88 ± 9 Bq m−3, and 46 to 59 Bq m−3, with an arithmetic mean 53 ± 5 Bq/m3, respectively. As is evident from Fig. 3, all results were in the range of two standards deviations from the monthly mean values, and each single measurement was burdened with a relative deviation less than ± 20% of the monthly average value. Such an accuracy level is commonly accepted in radiological dose evaluations. Therefore, a single PicoRad method measurement can also be used for monthly evaluation of the indoor radon levels with reasonably accuracy.
Indoor radon distribution
Generally, there are four types of residential buildings in Kalisz:
-
Small detached houses; mostly are relatively new with up to two stories (ground and first floor)
-
Old, multifamily freestanding residential buildings, up to five stories, made of bricks
-
Five-story prefabricated block of flats
-
Ten-story high-rise buildings
Altogether, the indoor radon concentrations were measured in 141 rooms. The observed radon concentrations ranged between 10 Bq m−3 and 350 Bq m−3. The measurements in the detached houses involved the ground and first floors, while in the five-story prefabricated blocks, lower (0 ÷ 2 and and upper (3–5) stories, separately, in order to check for the possible influence of the subsurface soil gas penetration into the building. The distribution of indoor radon concentrations for three types of buildings, and finally for all rooms, are shown in Fig. 4. The calculated distribution parameters for each group of buildings are collected in Table 2.
As expected, higher indoor radon values were observed on the ground floors of the individual houses that were up to two stories. However, because of the high level of the result dispersion for this group, one can recognize that, according to the Student’s test, the arithmetic mean difference between the radon concentrations in the ground floor and first-floor rooms were statistically significant for the p-level equals to 0.1, only. It could confirm fact that radon in soil gas escaping to the basements of these houses is an important source of indoor radon in the small detached houses. However, for the five-story prefabricated blocks such a difference for the lower level and upper level flats was statistically insignificant. Moreover, comparing the indoor radon concentrations in detached houses with the radon concentration in the soil gas for the close vicinity of these houses showed only a very week, almost insignificant correlation (R2 = 0,1), as can be seen in Fig. 5.
Therefore, these results confirm the predominant effect of the building construction on the indoor radon concentrations in this type of buildings observed in the experiments.
On the other hand, the unexpected increased indoor radon levels in the high-rise blocks in comparison with those for the five-story prefabricated blocks can be explained by substantial input of radon exhalation from the different kinds of building materials, especially the so-called lightweight concrete used in high-rise building construction, which has ash as an additive. It has been proven that such building materials contain increased radium activity [22]. Elevated indoor radon levels have also been reported recently for high-rise blocks in Serbia [23].
The arithmetic mean values of indoor radon concentrations for this study are very close to those obtained previously for kindergartens and schools in the same city [14] or in the towns of Podlasie Province in Poland [18]. They also correspond to recently published indoor radon data for the city of Wroclaw in Poland [24]. However, for the annual effective dose calculation from Eq. (7), the median values of radon concentrations were taken
where DCF is the radon dose conversion factor for radon inhalation, DCF = 16.8 × 10−6 (mSv Bq−1 h−1 m3)]ARn is the median radon concentration of 46.4 Bq m−3t is the average annual indoor occupancy in hours, t = 7000 hF is the indoor radon daughters equilibrium factor, F = 0.4
The calculated average annual effective dose for adult inhabitants of Kalisz was equal to 2.2 mSv.
Conclusions
The results of the indoor radon survey in Kalisz, Poland performed using the PicoRad method show that the median values of indoor radon concentration ranged from 34.4 to 56.9 Bq m−3 for different types of residential buildings. The highest values were observed for ground floor rooms in detached houses, whereas the lowest were found in five-story prefabricated blocks. It is the type of building construction that is the major factor influencing the moderate values of indoor radon in this area This is confirmed by the almost negligible correlation between radon in soil gas and indoor radon levels in detached houses and the observed radon entries into these houses.
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Bem, H., Janiak, S. & Przybył, B. Survey of indoor radon (Rn-222) entry and concentrations in different types of building in Kalisz, Poland. J Radioanal Nucl Chem 326, 1299–1306 (2020). https://doi.org/10.1007/s10967-020-07394-0
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DOI: https://doi.org/10.1007/s10967-020-07394-0