ABSTRACT
The accidental or intentional crash upon structures of Nuclear Power Plant (NPP) by an aircraft cause the fuel spreading followed by a fireball formation. This fireball is large enough to engulf the entire NPP and radiates a large amount of heat. This engulfment may lead to a local rise in temperature, which causes the spallation of concrete structure and fatalities to the human being. This may affect the integrity of NPP structures and has safety implications. The building structures influence the spatial evolution of fireball due to the generation of large turbulent structures, which further increases the local temperature. The evolution of fireball following fuel dispersion due to the aircraft crash upon an NPP is presented in this article. Numerical simulation to study the effect of fireball on the target NPP structure and its surrounding has been performed using a three-dimensional computational fluid dynamics (CFD) code. This analysis is used to study the evolution of fireball and thermal hazard associated with the radiated heat. It is found that some parts of fireball energy go as heat input to containment and the remaining portion is dissipated to the atmosphere by convection and radiation.
Abbreviations
CCPS: Centre for Chemical Process Safety; CID: Controlled Impact Demonstration; CFD: Computation Fluid Dynamics; EDC: Eddy Dissipation Concept; FAA: Federal Aviation Administration; FDS: Fire Dynamic Simulator; FVDOM: Finite Volume Discrete Ordinate Method; GAMG: Geometric Algebraic Multi-Grid; HRR: Heat Release Rate; IAEA: International Atomic Energy Agency; NIST: National Institute of Standards and Technology; NPP: Nuclear Power Plant; NTSB: National Transport Safety Board; OpenFOAM: Open Field Operation And Manipulation; PBiCG: Preconditioned Bi-Conjugated Gradient; PISO: Pressure Implicit with Splitting of Operator; SMD: Sauter Mean Diameter; TNO: The Netherlands Organization of applied scientific research; VTT: Technical Research Centre of Finland; WTC: World Trade Centre
Nomenclature
Ad | = | surface area of droplet |
Cd | = | drag coefficient |
Cp | = | specific heat capacity (kJ kg−1 K−1) |
D | = | diffusion coefficient |
DFB | = | fireball diameter (m) |
hFB | = | lifting height (m) |
h | = | convection coefficient (w/m2K−1) |
hs | = | sensible enthalpy (kJ/kg) |
ΔHc | = | Heat of combustion (kJ mol−1) |
H°(T) | = | absolute enthalpy (kJ/kg) |
Hv | = | latent heat of vaporization |
I | = | radiation intensity (W sr−1) |
k | = | turbulent kinetic energy (m2 s−2) |
L | = | distance from the target |
M | = | mass of fuel (kg) |
| = | radius vector |
= | direction vector | |
Srad | = | source term for thermal radiation |
| = | scattering vector |
S | = | path length (m) |
T | = | time (s) |
Δt | = | integration time step |
Φ | = | scattering phase function |
= | spatial angle (sr) | |
Xv | = | vapor mole fraction |
Y | = | mass fraction |
Subscript
a | = | ambient |
d | = | Droplet |
fuel | = | Fuel |
FB | = | Fireball |
h | = | Enthalpy |
k | = | Species |
n | = | Number |
lift | = | Lifting |
max | = | maximum |
mix | = | Mixing |
ox | = | Oxidizer |
in | = | Inlet |
t | = | turbulent |
Greek Symbols
Ω | = | reaction rate (mol L−1 s−1) |
Α | = | absorption coefficient |
β | = | evaporation parameter |
γ* | = | mass fraction |
Ε | = | dissipation rate |
µ | = | dynamic viscosity (N s m-2) |
η | = | refractive index |
τ | = | transmissivity |
= | droplet relaxation time | |
τmix | = | turbulent mixing |
Ρ | = | density (kg m−3) |
Σ | = | Stefan-Boltzmann constant (W m−2 K−4) |
σs | = | scattering coefficient |
χR | = | radiative heat fraction |
χ | = | fraction of fine structure which may react |
Non-Dimensional Numbers
Bi | = | Biot Number |
BM | = | Splading Number |
Nu | = | Nusselt Number |
Pr | = | Prandtl Number |
Re | = | Reynolds Number |
Sc | = | Schmidt Number |
Sh | = | Sherwood Number |
Superscripts
“-” | = | Spatial filter |
“~” | = | Favre filter |
st | = | Stokes flow |
Disclosure statement
No potential conflict of interest was reported by the authors.