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Module13 External gamma dose assessment from building materials according to IAEA SSG-32 DTU-COST-RILEM DOCTORAL COURSE, TECHNICAL UNIVERSITY OF DENMARK, LYNGBY, DENMARK, 17/08/2016 “The project leading to this application has received funding from the European Union’s Horizon 2020 research and innovation programme under the Marie Sklodowska-Curie grant agreement No 701932” By-BM Project H2020-MSCA-IF-2015 Research Fellow Geopolymer Team, School of Natural and Built Environment Queen’s University Belfast (QUB) z. [email protected] Dr Zoltan Sas

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Page 1: External gamma dose assessment from building materials ...bybmproject.com/wp-content/uploads/2018/04/Z_SAS_module_13.pdf · Module13 External gamma dose assessment from building materials

Module13External gamma dose assessment from

building materials according to IAEA SSG-32

DTU-COST-RILEM DOCTORAL COURSE, TECHNICAL UNIVERSITY OF DENMARK, LYNGBY, DENMARK, 17/08/2016

“The project leading to this application has received funding from the European Union’s Horizon 2020research and innovation programme under the Marie Sklodowska-Curie grant agreement No 701932”

By-BM Project H2020-MSCA-IF-2015 Research Fellow

Geopolymer Team, School of Natural and Built Environment

Queen’s University Belfast (QUB)

z. [email protected]

Dr Zoltan Sas

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Electromagnetic radiation from

the core

No chare, no mass

High penetration (energy

dependant)

Not decay just a follwing effect

Discrete energy of the energy

nievaus

Usually, it the gamma radiation is

generated right after the decays

Gamma radiation

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Gamma spectra of NORM sample

Red mud sample from Ajka

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Photoeffect

Total enertgy of

the photon

imparted to theelectron

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Compton scattering 100 keV < Eg < 2MeV

The photon imparts energy but

not the total!

Energy of the scattered photon is

lower after scattering and the

direction also changes

The difference is the kinetic

energy of the Compton electron

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Pair production Eg > 1.02 MeV

The photon iteracts with

electromagnetic field of the atom

The total energy is imarted

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Interaction of gamma radiation with matter

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Gamma radiation is the main source of

external indoor exposure on residents

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Introduction of dose assessement method

This module of the training course about dose assessments

provides examples relating to massive concrete structures (e.g.

apartment blocks) and for a smaller, simpler type of structure

such as those widely found in the rural areas of developing

countries

A calcualtion is based on of the approach of Markkanen

presented for calculating dose due to external gamma radiation

from BMs

The results are given in tabular form as specific dose rates

This allows the most typical dose assessments to be made without

computer calculations

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Introduction of dose assessement method

The method is based on calculating the dose rate for a

rectangular building constructed of BM of uniform density

and containing radionuclides of uniform activity

concentration.

The calculation covers situations in which the radionuclides

are distributed in two layers of separate BMs with different

densities and activity concentrations;

e.g.: concrete walls covered with a thin layer of another

material such as tiles

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Introduction of dose assessement method

The reference level of 1 mSv/a used for BMs is defined as due to the ‘excess

exposure’ caused by these materials above the exposure due to normal

background levels of radiation

The effects of doors and windows will lower the dose

rate by only a minor amount and so for simplicity

doors and windows are not considered in the

calculation

In many cases, BMs themselves provide significant

shielding against gamma radiation from the soil in the

terrestrial background

In the case of massive concrete structures, the

shielding is almost complete

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Introduction of dose assessement method

The basic approach in determining the ‘excess exposure’ is as follows:

The total exposure due to the BM and the

background levels is calculated, after allowance for

the shielding provided by the BM against gamma

radiation in the terrestrial background

The exposure to gamma radiation in the terrestrial

background is then subtracted

The result for comparison with the reference level is

referred to as the ‘excess exposure’

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Introduction of dose assessement method

The world population weighted average dose

rate of 60 nGy/h is assumed for gamma radiation

in the terrestrial background (reported in

UNSCEAR2000 Annex B)

The possible shielding effect of BMs for cosmic

radiation is considered to be small, and therefore

exposure to cosmic radiation is not considered in

the assessments

The gamma dose rate is calculated in the middle

of the standard sized room shown in Figure

Longer sidewall

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Introduction of dose assessement method

The total dose rate indoors is calculated by

summing the separately calculated dose

rates due to walls, floor and ceiling given in

Table VI–1 of IAEA SSG-32

A conversion factor of 0.7 Sv/Gy is used for

converting the absorbed dose in air to an

effective dose [UNSCEAR1993] (for adults)

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Introduction of dose assessement method

Risica et al. have carried out a sensitivity analysis concerning the effects of

changes in the parameters for the room on the dose in the room and found

the following results:

The variation in the dose rate in air in relation to the position in the room was found

to be limited to approximately 10% at a distance of up to 1 m from the walls.

The maximum variation in the dose rate obtained was 6% from the calculation for a

room with a volume of 60 m3

The absorbed dose rate in air was calculated as a

function of room dimensions for a fixed height of 2.8

m and various widths and lengths of the room

ranging from 2 m to 10 m were used, in both

rectangular and square shapes.

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Introduction of dose assessement method

The absorbed dose rate in air in the room was calculated

as a function of the wall, floor and ceiling thickness

It was found that up to a thickness of 0.4 m, increasing

the thickness increases the radiation dose rate, whereas

when the thickness is greater than 0.4 m, self-absorption

in the material makes the effect of a further increase in

thickness negligible

It can therefore be concluded that the variation in the dose rate in the model

room is not significantly affected for room sizes ranging from 12 m2 to 100 m2

for a fixed room height of 2.8 m, or for variations in the wall thickness

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First steps

Data collection: Ra-226; Th-232; K-40

(Bq/kg), Density (kg/m3), Thickness (m)

Calculate Mass per unit Area (M/A) of

wall, ceiling or floor material (kg/m2)

Select the closest value from the 1st

column TABLE VI–1.

Multiple the dose conversion factor

with activity concentrations

Summarize them in function of the

number of the walls, covers, etc

To get effective dose use 0.7 Sv/Gy

dose conversion factor

To get annual excess multiple the dose

rate considering the occupancy

factor

Ra-226 Th-232 K-40

W1 - - - - - - - -

W2 - - - - - - - -

Floor - - - - - - - -

Ceiling - - - - - - - -

Tile_W1 - - - - - - -

Tile_W2 - - - - - - -

Tile_Floor - - - - - - -

Tile_Celiling - - - - - - -

Roundup

with Tile

Roundup

without

Tile

Activity concentration Density

(kg/m3)

Thickness

(m)

M/A

(kg/m2)

Exposure to gamma radiation in a concrete room with tiles on

the walls

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First steps

Data collection: Ra-226; Th-232; K-40

(Bq/kg), Density (kg/m3), Thickness (m)

Calculate Mass per unit Area (M/A) of

wall, ceiling or floor material (kg/m2)

Select the closest value from the 1st

column TABLE VI–1.

Multiple the dose conversion factor

with activity concentrations

Summarize them in function of the

number of the walls, covers, etc

To get effective dose use 0.7 Sv/Gy

dose conversion factor

To get annual excess multiple the

dose rate considering the occupancy

factor

Ra-226 Th-232 K-40 Ra-226 Th-232 K-40

w1

Longer sidewall:

12.0×2.8 m

0 0 0 0 95 110 8

25 9 10 0.73 87 100 7.3

50 18 21 1.5 80 94 6.7

100 35 40 2.8 65 77 5.6

150 50 56 3.9 52 62 4.6

200 61 70 4.9 40 50 3.8

300 79 91 6.4 24 31 2.5

500 96 110 8.1 8 12 1

-

0 0 0 0 32 37 2.7

25 2.7 3.1 0.22 30 35 2.5

50 5.5 6.2 0.44 28 32 2.3

100 11 12 0.85 22 27 2

150 15 18 1.2 19 23 1.7

200 20 22 1.6 16 19 1.4

300 26 30 2.1 10 13 1

500 33 38 2.7 3.7 5.4 0.45

0 0 0 0 350 420 30

25 46 52 3.7 310 370 27

50 90 100 7.1 270 330 24

100 160 190 13 200 250 18150 220 250 18 150 180 14200 260 300 21 110 140 11300 310 360 26 56 78 6.3500 350 420 30 15 27 2.2

Floor or Ceiling:

12.0×7.0 m

Wall, ceiling or floor material

(top layer)

0.2 m thick concrete behind the

wall, ceiling or floor material

(pGy/h per Bq/kg) (pGy/h per Bq/kg)

(pGy/h per Bq/kg) (pGy/h per Bq/kg)

w2

Smaller sidewal:

7.0×2.8 m

Wall, ceiling or floor material

(top layer)

0.2 m thick concrete behind the

wall, ceiling or floor material

(pGy/h per Bq/kg) (pGy/h per Bq/kg)

Mass per unit

area of wall,

ceiling or floor

material (kg/m2)

Radionuclide

Wall, ceiling or floor material

(top layer)

0.2 m thick concrete behind the

wall, ceiling or floor material

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First steps

Data collection: Ra-226; Th-232; K-40

(Bq/kg), Density (kg/m3), Thickness (m)

Calculate Mass per unit Area (M/A) of

wall, ceiling or floor material (kg/m2)

Select the closest value from the 1st

column TABLE VI–1.

Multiple the dose conversion factor

with activity concentrations

Summarize them in function of the

number of the walls, covers, etc

To get effective dose use 0.7 Sv/Gy

dose conversion factor

To get annual excess multiple the dose

rate considering the occupancy

factor

w1 0 0 0 0 0 0 0

w2 0 0 0 0 0 0 0

Floor 0 0 0 0 0 0 0

Ceiling 0 0 0 0 0 0 0

w1_Tile 0 0 0 0

w2_Tile 0 0 0 0

F_Tile 0 0 0 0

C_Tile 0 0 0 0

100

80

60 0.00

0 00.00 0.00 0.00

0.00 0.00 0.00

0.00 0.00

Adult Children Infant

0

Σ D_rate

(nGy/h)-BG

Excess

E_D_rate

(nSv/h)

Occupancy

(%)

Annual effective excess dose mSv/y

Ra-226 Th-232 K-40 Dose rate

(µGy/h)

Σ D_rate

(nGy/h)(pGy/h per Bq/kg)

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Calculation examples

Check Annex VI of IAEA SSG-32 on page 75

Work in pairs with the help of excel on the basis of the guide

P1 Example 1: Exposure to gamma radiation in a concrete room where the

concentrations of Ra-226 and Th-232 are slightly above average

P2 Example 4: Exposure to gamma radiation in a room where lightweight walls

are made of materials with an elevated concentration of Ra-226

P3 Example 5: Exposure to gamma radiation in a room where the concrete walls

are made of material with an elevated concentration of Ra-226

After finish discuss the results

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Calculation examples

Check Annex VI of IAEA SSG-32 on page 75

Work in pairs with the help of excel on the basis of the guide

P1 Example 1: Exposure to gamma radiation in a concrete room where the concentrations of Ra-226 and Th-232 are slightly above average

P2 Example 4: Exposure to gamma radiation in a room where lightweight wallsare made of materials with an elevated concentration of Ra-226

P3 Example 5: Exposure to gamma radiation in a room where the concrete walls are made of material with an elevated concentration of Ra-226

Discuss the results

Solve Example 3: Work together

Every participant should search litrature about Ra-226; Th-232, K-40 activityconcentration in BMs

Make you own calculation

Use the prepared excel sheet in case of your future publication

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Comparison of RP-112 and IAEA SSG-32

on the example of By-BM Database

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By-BM database

This study is based on the continuously growing database of

the By-BM (H2020-MSCA-IF-2015) project.

The aim of this project to characterize the mechanical and

radiological parameters of constituents and prepared By-BM

geopolymers made from industrial by-products.

This project is strongly connected to, and provides information

to the NORM (naturally occurring radioactive material)

database of COST TU 1301 NORM4Building Action.

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By-BM database unified selection criteria

Only individually reported sample information about the Ra-226, Th-232 and

K-40 were obtained by gamma spectrometry was used

Average results of certain materials were used only if the investigated

material originated from same site, e.g. quarries, mines, reservoirs.

In the case of commercial building materials the brand and the type of the

samples had to be clearly mentioned in the reference to fulfil selection

criteria.

In several cases the U-238 activity concentration values were published. In

that cases the reported data was imported into the database only if the

results were obtained from the Rn-222 progenies (Bi-214, Pb-214) to avoid the

disequilibrium in the decay chain

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By-BM database unified selection criteria Generally, to limit gamma exposure originated from building materials the widely used

I-index – defined in RP112 – is applied. The I-index can be calculated by the followingequation:

Where CRa-226, CTh-232, CK-40 are the Ra-226, Th-232 and K-40 activity concentrations inBq/kg.

The calculation method the I-index based on the model of Markkanen with fixedparameters of concrete building (density and thickness of the walls are 2350 kg/m3, 20cm, respectively)

MARKKANEN, M., Radiation Dose Assessments for Materials with Elevated Natural Radioactivity, Publication STUK-B-STO 32, Finnish Centre for Radiation and NuclearSafety, Helsinki (1995).

The I-index value of 1.0 can be used as a conservative screening tool for identifyingmaterials that during their use would cause doses exceeding the reference level (1mSv/y excess in addition to outdoor exposure) in the case of bulk amount inbuilt.

In the European Union to control the gamma exposure originated from buildingmaterials the I-index is recommended for the member states to screen them.

kgBq

C

kgBq

C

kgBq

CI KThRa

/3000/200/300

40232226

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By-BM database unified selection criteria

The Council Directive allows the dilution and mixing of construction materials (I-

index<1.0), which makes possible the mixing of NORM by-products with low activity

level raw materials.

In the case of the calculation of dose needs to take into account other factors such

as density, thickness of the material as well as factors relating to the type of building

and the intended use of the material (bulk or superficial) to get precise dose

estimation of residents. The density and the thickness of modelled concrete room are

a constant parameters.

In the case of the International Atomic Energy Agency (IAEA) released No. SSG-32

(Specific Safety Guide) the simplified calculation method is based on the same

model of Markkanen but the thickness and the density of the building material are

taken into consideration during the calculation.

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By-BM database

By-BM database contains

individual data about Ra-226, Th-

232, K-40 activity concentration of

30 different materials (23 building

materials, 7 by-products

Altogether 431 by-products and

1095 building materials and raw

materials were collected from 48

countries.

The worldwide distribution and

the number of data are illustrated

on Figure

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By-BM database Material

name

Number

of

samples

Density Material

type Material

name

Number

of

samples

Density Material

type

kg/m3 BM/BP kg/m3 BM/BP

Aggregate 9 1900 BM Serizzo 5 2650 BM

Basalt 3 3000 BM Sienites 5 2700 BM

Brick 243 1900 BM Silstone 1 2350 BM

Cement 87 1500 BM Slate 1 2650 BM

Ceramics 94 2400 BM Tile,

asbestos 4 1750 BM

Concrete 63 2350 BM Travertine 9 2300 BM

Gas

concrete 37 700 BM Tuff 10 2100 BM

Granite 297 2600 BM Volcanic 7 1800 BM

Gypsum 66 865 BM Bottom ash 59 700 BP

Limestone 16 2600 BM Fly ash 145 720 BP

Marbles 72 2550 BM Manganese

clay 44 2800 BP

Pumice 3 650 BM Phosphogyp

sum 45 1500 BP

Rock 29 2300 BM Red mud 92 1600 BP

Sand 19 1500 BM Steel slag 41 2600 BP

Sandstone 14 2323 BM Residue of

TiO2 5 4300 BP

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Results

In case of the building materials the natural isotope content

varied widely (Ra-226: <DL-27851 Bq/kg; Th-232: <DL-906

Bq/kg, K-40: <DL-17922 Bq/kg), more so than the by-products

(Ra-226: 7-3152 Bq/kg; Th-232: <DL-1350 Bq/kg, K-40: <DL-3001

Bq/kg).

But the mean value of Ra-226, Th-232 and K-40 content of

reported by-products were 2.52, 2.35 and 0.39 times higher in

case of the by-products than the building materials,

respectively.

This is the reason why the radionuclide content cannot be

ignored since the by-products can cause increased

radiological risk.

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Density considertion on calculated dose rate

Overestimation without density

consideration of absorbed dose

Absorbed dose rates of BMs calculated

with different methods in the function

of I-indexes

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Results

In this study the absorbed gamma dose rate of a model

room with 20 cm thickness with various density were

calculated applied with dose conversion factors of RP-112

without density consideration and the IAEA No. SSG-32.

The data about Ra-226, Th-232 and K-40 activity

concentration of the building materials were collected from

worldwide scientific reported sources.

The I-indexes of the building materials were also calculated

and compared with the absorbed gamma dose rates of the 2different calculation methods.

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Conclusion

The absorbed gamma dose rates results were compared and

clearly proved that without density consideration the calculated

dose rate significantly higher in the case of low density buildingmaterials

Under 1000 kg/m3 even 60-70% higher dose rate can be estimated.

This is the reason why with density consideration the calculated I-

indexes belong to lower dose rate which clearly proves the

overestimation of I-index in connection with generated dose rate

It means the I-index provides a conservative and superficial

approximation.

In the case of building materials with low density e.g. commonly

used perforated bricks, which can make significant overestimation

and unnecessary restriction in the case of certain low density

building materials

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“The project leading to this application has received funding from the European Union’s Horizon 2020

research and innovation programme under the Marie Sklodowska-Curie grant agreement No 701932”