Abstract
Alternative fuel has attracted large focus because of environmental issues. Laminar burning speed results of syngas/air/diluent, syngas/O2/He and GTL/air/diluent premixed flames have been reviewed. In this paper, syngas consists of hydrogen and carbon monoxide and GTL (gas to liquid) is a blend of 43% n-dodecane, 25% n-decane, and 32% iso-octane. The diluent with the same specific heat as the burned gases consists of 14% carbon dioxide and 86% nitrogen. Experiments were carried out using a cylindrical chamber to observe the flame images and to measure pressure rise. The pressure rise data have been used to calculate the laminar burning speed by an integral-based multi-shell thermodynamic model for the low stretch and smooth flames. Power-law correlations were developed for experimental burning speed results of syngas/air/diluent, syngas/O2/He and GTL/air/diluent mixtures over a wide range of equivalence ratios, temperatures, pressures, and diluent concentrations. Kinetics simulations calculated by 1-D steady-state flame code from CANTERA were compared with various experimental burning speed results. The measured burning speed values are very close to the simulation calculations.
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- \( A_{\text{b}} \) :
-
Burned gas area
- a :
-
Fitted constant
- b :
-
Fitted constant
- C :
-
Hydrogen percentage
- D :
-
Diluent concentration
- \( E_{\text{b}} \) :
-
Burned gas energy
- \( E_{\text{i}} \) :
-
Initial energy
- \( E_{\text{u}} \) :
-
Unburned gas energy
- \( E_{\text{eb}} \) :
-
Electrodes boundary energy defect
- \( E_{\text{ph}} \) :
-
Preheat zone energy defect
- \( E_{\text{wb}} \) :
-
Wall boundary energy defect
- \( e_{\text{b}} \) :
-
Burned gas specific energy
- \( e_{\text{u}} \) :
-
Unburned gas specific energy
- \( e_{\text{bs}} \) :
-
Isentropically compressed burned gas specific energy
- \( e_{\text{us}} \) :
-
Isentropically compressed unburned gas specific energy
- I :
-
Radiation intensity
- j :
-
Number of narrow bands
- \( k_{n} \) :
-
K-distribution absorption coefficient
- M :
-
Number of directions
- m :
-
Total mass
- \( m_{\text{b}} \) :
-
Burned gas mass
- \( m_{\text{u}} \) :
-
Unburned gas mass
- \( \dot{m}_{\text{b}} \) :
-
Mass burning rate
- N :
-
Number of Gaussian quadrature points
- P :
-
Mixture pressure
- \( P_{0} \) :
-
Reference pressure
- p :
-
Pressure
- \( p_{\text{i}} \) :
-
Initial pressure
- \( Q_{\text{e}} \) :
-
Energy loss to electrodes
- \( Q_{\text{r}} \) :
-
Radiation energy loss
- \( Q_{\text{w}} \) :
-
Energy loss to wall
- R :
-
Specific gas constant
- r :
-
Flame radius
- \( r_{\text{e}} \) :
-
Electrode radius
- \( S_{\text{u}} \) :
-
Laminar burning speed
- \( S_{\text{uo}} \) :
-
Reference laminar burning speed
- T :
-
Temperature
- \( T_{\text{b}} \) :
-
Burned gas temperature
- \( T_{\text{i}} \) :
-
Initial temperature
- \( T_{\text{u}} \) :
-
Unburned gas temperature
- \( T_{{{\text{u}}0}} \) :
-
Reference temperature
- t :
-
Time
- V :
-
Energy source volume
- \( V_{\text{b}} \) :
-
Burned gas volume
- \( V_{\text{c}} \) :
-
Chamber volume
- \( V_{\text{e}} \) :
-
Electrodes volume
- \( V_{\text{i}} \) :
-
Initial volume
- \( V_{\text{u}} \) :
-
Unburned gas volume
- \( V_{\text{eb}} \) :
-
Electrodes boundary displacement volume
- \( V_{\text{ph}} \) :
-
Preheat zone displacement volume
- \( V_{\text{wb}} \) :
-
Wall boundary displacement volume
- \( v_{\text{b}} \) :
-
Burned gas specific volume
- \( v_{\text{u}} \) :
-
Unburned gas specific volume
- \( v_{\text{bs}} \) :
-
Isentropically compressed burned gas specific volume
- \( v_{\text{us}} \) :
-
Isentropically compressed unburned gas specific volume
- \( x_{\text{b}} \) :
-
Burned gas mass fraction
- \( \dot{x}_{\text{b}} \) :
-
Rate of burned gas mass fraction
- \( \alpha \) :
-
Fitted constant
- \( \alpha_{0} \) :
-
Fitted constant
- \( \alpha_{1} \) :
-
Fitted constant
- \( \alpha_{2} \) :
-
Fitted constant
- \( \alpha_{3} \) :
-
Fitted constant
- \( \beta \) :
-
Fitted constant
- \( \beta_{0} \) :
-
Fitted constant
- \( \beta_{1} \) :
-
Fitted constant
- \( \beta_{2} \) :
-
Fitted constant
- \( \beta_{3} \) :
-
Fitted constant
- \( \gamma \) :
-
Fitted constant
- \( \gamma_{1} \) :
-
Fitted constant
- \( \gamma_{2} \) :
-
Fitted constant
- \( \theta \) :
-
Fitted constant
- \( \theta_{0} \) :
-
Fitted constant
- \( \theta_{1} \) :
-
Fitted constant
- \( \theta_{2} \) :
-
Fitted constant
- \( \theta_{3} \) :
-
Fitted constant
- \( \nu \) :
-
Wave number
- \( \rho_{\text{u}} \) :
-
Unburned gas density
- \( \phi \) :
-
Equivalence ratio
- \( \omega_{n} \) :
-
Weight function
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Wang, Z., Yu, G., Metghalchi, H. (2020). Laminar Burning Speed Study of Alternative Fuel Air Diluent Mixtures at High Pressures and Temperatures. In: Gupta, A., De, A., Aggarwal, S., Kushari, A., Runchal, A. (eds) Innovations in Sustainable Energy and Cleaner Environment. Green Energy and Technology. Springer, Singapore. https://doi.org/10.1007/978-981-13-9012-8_9
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