Translate this page into:
Modeling of the Radiological Atmospheric Dispersion and Consequences of Hypothetical Nuclear Accident at an Coastal Site using MACCS2 Code
*Corresponding author: Dr. O.S. Ahmed, Department of Physics, College of Sciences, Qassium University, Saudi Arabia. o.abdeldaaem@qu.edu.sa
-
Received: ,
Accepted: ,
How to cite this article: Ahmed OS, Elbegawy H, Mohamed GY. Modeling of the Radiological Atmospheric Dispersion and Consequences of Hypothetical Nuclear Accident at an Coastal Site Using MACCS2 Code. J Qassim Univ Sci. 2026;1:127-34. doi: 10.25259/JQUS_22_2026
Abstract
Objectives
In order to determine the atmospheric diffusion coefficient (χ/Q) and assess the radiation dosage resulting from a hypothetical release of iodine-131 under stable atmospheric conditions (stability class E), this study will model the atmospheric diffusion of radioactive contaminants using the MACCS2 tool.
Material and Methods
The MACCS2 code was used to perform atmospheric diffusion simulations under atmospheric stability class E, examining how wind speed and distance from the emission point affected the relative air concentration. The diffusion coefficient (χ/Q) reached its maximum value of 3.67E−03 s/m3 at a wind speed of 0.5 m/s and a distance of 100 m. This value was entered into the Total Effective Dose Equivalent (TEDE) calculation. Four age groups were included in the study: adults who worked outside, adults who worked indoors or retired, children (10 years old), and (1 year old).
Results
The maximal effective dose (TEDE) of I-131 was found to be 9.38 E−07 TEDE for adults outside, 8.26 E−07 TEDE for adults indoors, 5.68 E−07 TEDE for children (10 years old), and 1.93 E−07 TEDE for newborns (1 year old) in stability class E at a wind speed of 0.5 m/s and a distance of 100 m. It was also demonstrated that as wind speed and distance increased, the concentration and dose levels decreased. The International Atomic Energy Agency’s recommended yearly occupational exposure limit of 2 E−02 TEDE was far below all computed values.
Conclusion
The results indicate that the hypothetical scenario for stable atmospheric condition (E) does not result in doses that are higher than those that are internationally permitted limits. The study underscores the importance of using the MACCS2 code in assessing radiological consequences and supporting control and safety decisions at nuclear facilities.
Keywords
Atmospheric dispersion (χ/Q)
Dispersion parameters of gaussian model (σ y
σ z)
Effective dose equivalent (TEDE)
I-131
MACCS2 code
INTRODUCTION
For calculating radioactive atmospheric dispersion.[1,2-12] and its effects, MACCS2 is a Gaussian plume model. Since the issuance of DOE-STD-3009-94, MACCS2 has primarily been used for deterministic consequence analysis in Department of Energy (DOE) applications. In nuclear facilities, safety control selection has been based on code results.[1,13-15] By utilizing either the instantaneous concentration
(Bq m-3 or g m-3) or time-integrated concentration (Bq s m-3 or g-s m-3). The dispersion of the atmosphere is typically represented in terms of χ/Q, where χ is the pollutant concentration in the air at a given downwind point (x, y, z).[16,17] Q can be either the pollutant’s overall source strength (in becquerels or grams) or its steady rate of discharge (in Bq s-1 or g s-1). The plume’s relative concentration since it moves windward from a discharge spot is denoted by χ/Q.
When determining the dose to an individual and the emergency response process,[18,19] the χ/Q is an important element that ultimately defines the type of safety controls required[13,14,20-22]. In many countries worldwide, numerical models are employed to calculate exposure for co-located workers when the facility’s aerodynamic impacts could affect the release. In building, the χ/Q value offers a conservative dispersion estimate; otherwise, the source term is an important tool in determining the dose to an individual.[13–27] As indicated in Table 1,[28] the source term used in the input data was determined by Maciej Lipka. For example,[28-31] assuming that the radionuclide source term for I-131 was 3.0E+6 Bq, the study was conducted. When a nuclear power plant accident occurs, a large amount of radioactive fission products is released from the core due to meltdown, polluting the environment.
| Nuclide | Activity [Bq] | Nuclide | Activity [Bq] |
|---|---|---|---|
| Br-83 | 1.2E+07 | Te-133m | 2.2E+04 |
| Kr-85m | 6.5E+08 | I-131 | 3.0E+06 |
| Kr-85 | 3.3E+09 | I-132 | 1.6E+08 |
| Kr-87 | 3.9E+11 | I-133 | 1.45E+06 |
| Kr-88 | 7.1E+11 | I-134 | 2.1E+08 |
| Sr-89 | 4.7E+07 | I-135 | 3.9E+07 |
| Sr-90 | 5.8E+07 | Xe-131m | 7.1E+11 |
| Ru-103 | 3.1E+04 | Xe-133m | 1.1E+12 |
| Ru-105 | 1.2E+01 | Xe-133 | 3.2E+09 |
| Ru-106 | 6.2E+03 | Xe-135m | 6.2E+11 |
| Te-131 m | 6.4E+04 | Xe-135 | 2.5E+10 |
| Te-131 | 6.8E+04 | Cs-134 | 1.4E+07 |
| Te-132 | 3.4E+04 | Cs-137 | 6.8E+07 |
| Total | 3.6E+12 |
MATERIAL & METHODS
a. The Gaussian distribution equation can be stated as:
Where:
X(x,y,z): Concentration of air (Bq m-3) at a point with coordinates x,y,z,
H: height of effective release (m)
Q: rate of release (Bq s-1)
x: distance downwind (m),
y: distance from the crosswind (m),
z: height in relation to the ground (m),
U: average speed of wind (m s-1),
σy, σz : factors for crosswind and vertical dispersion (m).
Dispersion variables of the Gaussian model σy, σz could be expressed as a function of downwind distance x and atmospheric stability (Apismon and Goddard, 1987) as in Equations (2) and Table 2:[32]
| Stability | σ y | σ z | ||
|---|---|---|---|---|
| a | b | C | d | |
| Very unstable | 1.46 | 0.71 | 0.01 | 1.54 |
| Unstable | 1.52 | 0.69 | 0.04 | 1.17 |
| Neutral | 1.36 | 0.67 | 0.09 | 0.95 |
| Stable | 0.79 | 0.70 | 0.40 | 0.67 |
Where:- a,b,c, and d depend on the atmospheric stability
Equation 1 calculates the atmospheric dispersion by taking into account atmospheric parameters, including hypothetical data for (temperature, wind direction, and wind speed). The plume’s size is determined by its Gaussian distribution in the horizontal and vertical planes, which is reliant on the atmosphere’s stability and the plume’s dispersion downwind from the release point in both horizontal and vertical directions [Figure 1]. Keep in mind that this calculation does not specifically include the downwind plume distance, x. Values for σy and σz are estimated as a function of downwind distance, x, and D.B. Turner’s implementation. The atmosphere’s stability. Alternatively, Equation (3) can be obtained by using the Gaussian plume equation (Equation 1), a plume centerline receptor, and a ground-level release (y = z = H = 0), assuming there is no building.[5] Using the coefficients of dispersion that were acquired by means of the Eimutis-Konicek parameterization once more,[32]

- Plume of Gaussian distribution and coordinate system source.
Where:
U: speed of wind, which reduces the plume’s intensity (m s-1);
σy: factor for crosswind dispersion (m).
σz: factor for vertical dispersion (m).
RESULTS AND DISCUSSION
For the E stability class, to make the calculation of χ/Q values, as wind speed increases, χ/Q decreases, as shown in Tables 3 and 4 and Figures 2 and 3, Where the value as shown in Table 3, Figure 2 at U=0.5 m s-1 the χ/Q = 3.67E-03 and at U= 6 m s-1 the χ/Q = 3.06E-04 and Table 4 and Figure 3 gives at U=0.5 the χ/Q = 1.42E-and at U= 6 m s-1 the χ/Q = 1.18E-04, this attributed to wind transports air more quickly as its speed increases, airborne particles or gases are more likely to mix and disperse, spreading the material over a bigger volume of air and decreasing its specific concentration., else shown as the distances increases, χ/Q decreases as in Table 3 and Figure 2,which show that at D=100 m, U=0.5 and 6 m s-1 the χ/Q = 3.67E-03 and 3.06E-04 respectively, while at D= 200 m, U= 0.5 and 6 m s-1 the χ/Q = 1.42E-03 and 1.18E-04 respectively, as shown in Table 4 and Figure 3, and it is noticeable that the value of χ/Q at 200 m is less than at 100 m, as shown in Figure 4, because when a gas or aerosol is released into the air, it starts to spread out; as it moves away from the source, the air volume increases, which means the concentration of the substance in any given volume of air decreases, because dilution and dispersion causes the relative air concentration of a substance to decrease as the distance from the source increases, as shown in Tables 5 and 6, Figure 5. For stability class E, the value of χ/Q at 100m at U=1.5 m s-1 is 3.67E-3, which is in agreement with 3.3E-3 s m-3 in NUREG-1140 and 3.5E-3 s m-3 in DOE-STD-1189-2008. [31]
| Wind Speed (m s-1) | Values of χ/Q (s m-3) at 100(m) |
|---|---|
| 0.5 | 3.67E-03 |
| 1 | 1.83E-03 |
| 1.5 | 1.22E-03 |
| 2 | 9.17E-04 |
| 2.5 | 7.34E-04 |
| 3 | 6.11E-04 |
| 3.5 | 5.24E-04 |
| 4 | 4.58E-04 |
| 4.5 | 4.08E-04 |
| 5 | 3.67E-04 |
| 5.5 | 3.33E-04 |
| 6 | 3.06E-04 |
| Wind Speed (m s-1) | Values of χ/Q (s m-1) at 200(m) |
|---|---|
| 0.5 | 1.42E-03 |
| 1 | 4.73E-04 |
| 1.5 | 4.73E-04 |
| 2 | 3.55E-04 |
| 2.5 | 2.84E-04 |
| 3 | 2.37E-04 |
| 3.5 | 2.03E-04 |
| 4 | 1.77E-04 |
| 4.5 | 1.58E-04 |
| 5 | 1.42E-04 |
| 5.5 | 1.29E-04 |
| 6 | 1.18E-04 |

- χ/Q against wind speed for stability class E at 100 m.

- χ/Q against wind speed for stability class E at 200 m.

- χ/Q versus wind speed for stability class E at 100 m and 200 m.
| Distance (D) m | Relative air concentration(s m-3) |
|---|---|
| 100 | 1.22E-03 |
| 200 | 4.73E-04 |
| 300 | 2.71E-04 |
| Distance (D) m | Relative air concentration (s m-3) |
|---|---|
| 100 | 3.67E-03 |
| 200 | 1.42E-03 |
| 300 | 8.14E-04 |

- χ/Q versus distance at U= 1.5 m s-1 for stability class E.
Figures 6-9 and Table 7 show The results for total effective dose (TEDE) of I- 131 in stability class E at 100,200 and 300 m at U= 1.5 m s-1, which reached about 3.13E-07, 1.2E-07 and 6.37E-08 for Adult (outdoor worker) & 2.7E-07, 1.06E-07 and 6.11E-8 for Adult (indoor worker (pensioner)) & 1.8E-07, 7.3E-08 & 4.2E-8 for (10 -year –old) and 6.4E-08, 2.5E-08, 1.43E-08 for (1 -year -old) respectively. The total effective dose (TEDE) decreased with increasing distances, which attributed to result of atmospheric dispersion factor, where dilution and dispersion cause the concentration of substance to decrease with

- Total effective dose as a function of distance for an adult (outdoor worker)of I-131at stability class E.

- Total effective dose as a function of distance for an adult (indoor worker (pensioner) of I-131 at stability class E.

- Total dose of effectiveness as a distance function for a ten-year-old of I-131 at stability class E.

- Total dose of effectiveness as a distance function for a one-year-old.
| Distances (m) | TEDE at Adult (outdoor workers) | TEDE at Adult (indoor workers or elderly) | TEDE at (ten years old) | TEDE at (one -year –old) |
|---|---|---|---|---|
| 100 | 3.12737E-07 | 2.75251E-07 | 1.8957E-07 | 6.44752E-08 |
| 200 | 1.20995E-07 | 1.06E-07 | 7.33429E-08 | 2.49449E-08 |
| 300 | 6.94261E-08 | 6.11045E-08 | 4.20836E-08 | 1.43132E-08 |
increasing distance from a source, and the length or intensity of exposure also reduces, resulting in a reduced total effective dose, else notice that the total effective dose decreases as wind speed increases as shown in Tables 7 and 8, Figures 10 and 11, This is because higher wind speeds enhance the dispersion and dilution of airborne radioactive materials, When stronger winds disperse radioactive particles over a greater area, the radioactive material is mixed with clean air more quickly, lowering its concentration at any one time and lowering the dose that people in the affected area get.
| Distances (m) | TEDE at Adult (outdoor workers) | TEDE at Adult (indoor workers or elderly) | TEDE at (ten years old) | TEDE at (one-year –old) |
|---|---|---|---|---|
| 100 | 9.38E-07 | 8.26E-07 | 5.6871E-07 | 1.93E-07 |
| 200 | 3.62985E-07 | 3.19E-07 | 2.20029E-07 | 7.48347E-08 |
| 300 | 2.08278E-07 | 1.83313E-07 | 1.26251E-07 | 4.29396E-08 |

- Total dose of effectiveness as a distance function for Adult (outdoor worker), Adult (indoor worker or elderly), (ten years old), and (one-year-old) of I-131at stability class E and wind speed 0.5 m.

- Total dose of effectiveness as a distance function for Adult (outdoor worker), Adult (indoor worker or elderly), (ten years old), and (one-year-old) of I-131at stability class E and wind speed 1.5 m.
Figure 10, Table 8 give the total dose of effectiveness as a distance function for Adult (outdoor worker), Adult (indoor worker or pensioner), (10-year-old), and (1-year-old) of I-131 at stability class E and wind speed 0.5 m s-1. The maximum TEDE of 9.38 E-07, 8.26 E-07, 5.68 E-07 and 1.9E-07 for Adult (worker outside), Adult (worker indoors), (Ten years old) and (One-year-old)at stability class E respectively at 100m from the release source, this value is less than IAEA for indoor worker ((occupational exposure limit of 2E-02 Sv per year).[31] It is evident from Figures 10 and 11 that the total effectiveness dose for an adult outdoor worker is greater than that for an adult indoor worker, an older adult, a 10-year-old, or a 1-year-old, which could be because the total effective dose of a substance can vary greatly depending on several factors, such as exposure time, physical activity, metabolic rate, and susceptibility. The adult outdoor worker usually has the largest total effective dose due to longer exposure time and higher activity levels (which result in greater inhalation), and perhaps increased pollution concentrations, The elderly and indoor workers have lower overall exposure and spend less time inexposed locations, which results in a lower total dose and younger children in particular have a faster respiratory rate in relation to their body size. However, because of their shorter exposure times and the environmental controls, they are still likely to receive a lower overall dose. Still, because of their susceptibility to poisons, even tiny amounts can have a big effect.
CONCLUSION
The χ/Q lowers as the wind speed rises and distances increase. For stability class E, χ/Q against wind speed is greater at 100 m than at 200 m. For stability class E, the value of χ/Q at 100m at U=0.5 m s-1 equals 3.67E-03,which is consistent with 3.3x10-3 s m-3 in NUREG-1140 and 3.5x10-3 s m-3 in DOE-STD-1189-2008.
At 100 meters from the release source, the maximum effective dose (TEDE) of I-131 for adults (outdoor workers), adults [indoor workers (pensioners)], and children aged 10 and 1, respectively, at stability class E is higher than at
At 200 meters, however, this value is lower than the IAEA occupational exposure limit for indoor workers (2E-02 Sv per year). Due to age and hours spent working, the total effective dose as a function of distance is higher for adults working outside and those working indoors (pensioners) at stability class E and wind speed of 0.5 m s-1.
Financial support and sponsorship
Nil.
Conflicts of interest
There are no conflicts of interest.
Use of artificial intelligence (AI)-assisted technology for manuscript preparation
The authors confirm that there was no use of artificial intelligence (AI)-assisted technology for assisting in the writing or editing of the manuscript, and no images were manipulated using AI.
REFERENCES
- Integration of safety into the design process. DOE-STD-1189-2008, U.S. department of energy, Washington, DC, 2008.
- Uncertainty study on atmospheric dispersion simulations using meteorological ensembles with a Monte Carlo approach, applied to the Fukushima nuclear accident. Atmos Environ: X. 2021;10:100112.
- [Google Scholar]
- Ranking uncertainties in atmospheric dispersion modelling following the accidental release of radioactive material. Radioprotection. 2020;55:S51-5.
- [CrossRef] [Google Scholar]
- Uncertainty-aware surrogate modeling for urban air pollutant dispersion prediction. Building Environ. 2025;267:112287.
- [Google Scholar]
- Atmospheric conditions and air quality assessment over NEOM, kingdom of Saudi Arabia. Atmos Environ. 2020;230:117489.
- [CrossRef] [Google Scholar]
- Radiological risk assessment of a proposed site for a generic VVER-1000 using HotSpot and InterRas codes. Prog Nucl Energy. 2020;120:103239.
- [CrossRef] [Google Scholar]
- Radioactive impact on Iran and the world from a postulated accident at Bushehr Nuclear power plant. Prog Nucl Energy. 2021;142:103991.
- [CrossRef] [Google Scholar]
- Application of probabilistic safety assessment (PSA) to the power reactor innovative small module (PRISM) Nucl Eng Technol. 2022;54:3324-35.
- [CrossRef] [Google Scholar]
- Drones application scenarios in a nuclear or radiological emergency. Kerntechnik. ;87:260-70.
- [CrossRef] [Google Scholar]
- Radiological consequences modelling for a land based operations environment. Def Sc J. 2021;71:470-5.
- [CrossRef] [Google Scholar]
- Revisiting atmospheric dispersion characteristics of multi-form tritium. SSRN Electron J 2022:1-26.
- [Google Scholar]
- Modeling of atmospheric dispersion and radiological dose consequences for a hypothetical accident in the perspective of Rooppur Nuclear power plant (RNPP) Nucl Eng Des. 2024;420:113022.
- [Google Scholar]
- Risk management program guidance for offsite consequence analysis, EPA 550-B99009, U.S. Environ Protection Agency 2009.
- MACCS2 computer code application guidance for documented safety analysis final report, DOE-EH-4.2.1.4, U.S. Department of Energy, Washington, D.C 2004.
- Code manual for MACCS2: Volume 1, user’s guide. Washington D.C, US: Nucl Regul Commission; 1998.
- Human respiratory tract model for radiological protection. ICRP publication 66. Annals of the ICRP 24. Oxford: International commission on radiological protection, Pergamon Press; 1994.
- Analysis and research of source term calculation. Beijing China: China Institute of Atomic Energy; 2004.
- Analysis of nuclear accident scenarios and emergency planning zones for a proposed advanced power reactor 1400 (APR1400) Nucl Eng Des. 2023;407:112275.
- [CrossRef] [Google Scholar]
- Evaluation of cancer risk after a release from a hypothetical nuclear reactor steam generator tube rupture accident (SGTR) Annals of Nuclear Energy. 2020;136:107023.
- [CrossRef] [Google Scholar]
- Final review of safety assessment issues at Savannah River Site. Pacific Northwest: Natl Lab; 2011.
- Quality assurance, DOE order 414.1D, U.S. Department of energy, Washington, D.C 2011.
- GENII Computer code application guidance for documented safety analysis final report, U.S. Department of energy, Washington, D.C 2004.
- Atmospheric relative concentrations for control room habitability assessments at nuclear power plants, regulatory guide 1.194. Washington D.C, US: Nucl Regul Commission; 2003.
- Deposition velocity methods for DOE site safety analyses, LLNL-TR654366, lawrence livermore national laboratory. U.S. Department of Energy; 2014.
- Chiddiq AB, Azad AA, Miah R. Radiological consequence assessment of a hypothetical accident at the rooppur nuclear power plant using hotspot simulation software ICCESD 2024
- Preparation guide for U.S. Department of energy nonreactor nuclear facility safety analysis reports, DOE-STD-3009-94, U.S. Department of Energy, Washington, D.C., Change Notice 2006.
- Derivations of continuous functions for the lateral and vertical atmospheric dispersion coefficients. Atmos Environ. 1972;6:857-63.
- [CrossRef] [PubMed] [Google Scholar]
- ICRP 1964. International commission on radiological protection, Recommendations of the international commission on radiological protection, ICRP Publication 6 (Pergamon Press, New York)
- “Source term estimation for the MARIA research reactor and model of atmospheric dispersion of radionuclides with dry deposition. Nukleonika. 2020;65:173-179.
- [Google Scholar]
- A regulatory analysis on emergency preparedness for fuel cycle and other radioactive material licenses, NUREG-1140, U.S. Washington, D.C: Nucl Regul Commission; 1988.
- Combining short-range dispersion simulations with fine-scale meteorological ensembles: Probabilistic indicators and evaluation during a Kr-85 field campaign. Atmos Chem Phys. 2022;22:15793-15816.
- [Google Scholar]
- Impacts of air pollution: General relationships and site dependence. Atmospheric Environ. 1996;30:3331-47.
- [CrossRef] [Google Scholar]
