Abstract
Fire accidents are more likely to occur in tunnels with different curves, aspect ratios, and slopes due to the land’s geographical characteristics. A three-dimensional computational fluid dynamics code with curvilinear grids fitted to the body was used to simulate a variety of fire locations releasing heat at a rate of 5 MW–60 MW in a tunnel with a turning radius of 100 m–1500 m, an aspect ratio of 0.5–2, and a slope between – 10% and 10%. Using the Design of Experiments (DOE) method coupled with numerical simulations, 32 3D numerical models were constructed and a second-order critical velocity model was generated. Analysis of critical velocity was performed based on Response Surface Methodology (RSM) and multifactor curve plots were drawn for effective parameters. The results showed that the critical velocity was proportional to one-third power of the heat release rate. It was also observed that the critical velocity increased gradually as the fire source moved from the tunnel’s center to its walls. Furthermore, the critical velocity decreased with increasing the aspect ratio. Results showed that the critical velocity increased with increasing the tunnel turning radius. Moreover, tunnels with negative slopes have a higher critical velocity than horizontal tunnels without slopes. Finally, by defining the parameters in non-dimensional form, a new modified form was derived for critical velocity calculation (R2 = 0.98). A critical velocity of 1.24 m/s–5.21 m/s was calculated based on five parameter values in this study. Furthermore, other straight and curved tunnel models confirmed the formula’s predictions.
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Abbreviations
- ANOVA:
-
Analysis of variance
- CCD:
-
Central composite design
- DOE:
-
Design of experiment
- RSM:
-
Response surface method
- A:
-
Tunnel cross-section area \(({{\text{m}}}^{2})\)
- Cp :
-
Specific heat at constant pressure (J/kgK)
- AR:
-
Aspect ratio (dimensionless)
- g:
-
Gravity acceleration (m2/s)
- h:
-
Smoke layer thickness (m)
- H:
-
Tunnel height (m)
- HRR:
-
Heat release rate (MW)
- HRRC :
-
Convective part of the heat release rate (MW)
- HRR*:
-
Non-dimensional form of the heat release rate (dimensionless)
- \({{\text{HRR}}}_{{\text{a}}}^{*}\) :
-
Asymptotic \({{\text{HRR}}}^{*}\) (dimensionless)
- HD :
-
Tunnel hydraulic diameter (m)
- Lf :
-
Flame height (m)
- \({\dot{{\text{m}}}}_{{\text{s}}}\) :
-
Mass flux of smoke \(({\text{kg}}/{\text{s}})\)
- \({{\text{P}}}_{{\text{s}}}\) :
-
Static pressure (Pa)
- \({\Delta {\text{P}}}_{{\text{stack}}}\) :
-
Stack pressure (Pa)
- \({\Delta {\text{P}}}_{{\text{total}}}\) :
-
Total pressure difference (Pa)
- \({{\text{P}}}_{{\text{d}}}\) :
-
Dynamic pressure (Pa)
- \({{\text{Q}}}_{{\text{H}}}\) :
-
Heat of combustion (\({\text{MJ}}/{\text{kg}}\))
- R:
-
Tunnel radius (m)
- S:
-
Tunnel slope (%)
- \({{\text{T}}}_{0}\) :
-
Ambient air temperature (K)
- \({{\text{T}}}_{{\text{f}}}\) :
-
Gas temperature (K)
- \(\Delta {\text{T}}\) :
-
Temperature difference between the smoke layer and airflow (K)
- \({{\text{u}}}^{+}\) :
-
Non-dimensional tangential velocity (dimensionless)
- V:
-
Ventilation air velocity (m/s)
- \({{\text{V}}}_{{\text{C}}}\) :
-
Critical velocity (m/s)
- \({{\text{V}}}_{{\text{C}}0}\) :
-
Critical velocity of the horizontal tunnel (m/s)
- \({{\text{V}}}_{{\text{CS}}}\) :
-
Critical velocity of the slopped tunnel (m/s)
- \({{\text{V}}}_{{\text{CS}}}\) :
-
Critical velocity of the slopped tunnel (m/s)
- \({{\text{V}}}_{{\text{min}}}\) :
-
Minimum critical velocity (m/s)
- \({{\text{V}}}_{{\text{max}}}\) :
-
Maximum critical velocity (m/s)
- \({{\text{V}}}_{{\text{C}}}^{*}\) :
-
Non-dimensional form of the critical velocity (dimensionless)
- \({{\text{V}}}_{{\text{min}}}^{*}\) :
-
Non-dimensional minimum critical velocity (dimensionless)
- \({{\text{V}}}_{{\text{max}}}^{*}\) :
-
Non-dimensional maximum critical velocity (dimensionless)
- W:
-
Tunnel width (m)
- \({{\text{x}}}_{{\text{i}}}\) :
-
Variable factor
- \({{\text{x}}}_{{\text{j}}}\) :
-
Variable factor
- \({{\text{X}}}_{{\text{r}}}\) :
-
Radiation fraction (dimensionless)
- y:
-
Second-order model
- \(\Delta {\text{y}}\) :
-
Grid size (m)
- \({{\text{Y}}}_{{\text{s}}}\) :
-
Soot yield (%)
- \({{\text{y}}}^{+}\) :
-
Non-dimensional distance from the wall (dimensionless)
- \(\Delta\) :
-
Fire transverse location (dimensionless)
- \({\upbeta }_{0}\) :
-
Constant coefficient
- \({\upbeta }_{{\text{i}}}\) :
-
Linear coefficient
- \({\upbeta }_{{\text{ii}}}\) :
-
Second-order coefficient
- \({\upbeta }_{{\text{ij}}}\) :
-
Interaction coefficient
- \(\in\) :
-
Error term
- \(\uptheta\) :
-
Longitudinal inclination of a tunnel (degree)
- \({\uprho }_{0}\) :
-
Ambient air density \(({\text{kg}}/{{\text{m}}}^{3})\)
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Jafari, S., Farhanieh, B. & Afshin, H. Effects of Fire Parameters on Critical Velocity in Curved Tunnels: A Numerical Study and Response Surface Analysis. Fire Technol (2024). https://doi.org/10.1007/s10694-024-01548-2
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DOI: https://doi.org/10.1007/s10694-024-01548-2