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Frontiers in Energy

ISSN 2095-1701

ISSN 2095-1698(Online)

CN 11-6017/TK

Postal Subscription Code 80-972

2018 Impact Factor: 1.701

Front. Energy    2021, Vol. 15 Issue (1) : 38-45    https://doi.org/10.1007/s11708-020-0692-1
RESEARCH ARTICLE
An experimental study on ignition of single coal particles at low oxygen concentrations
Wantao YANG, Yang ZHANG, Lilin HU, Junfu LYU, Hai ZHANG()
Key Laboratory for Thermal Science and Power Engineering of the Ministry of Education, Department of Energy and Power Engineering, Tsinghua University, Beijing 100084, China
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Abstract

An experimental study on the ignition of single coal particles at low oxygen concentrations ( XO2<21%) was conducted using a tube furnace. The surface temperature (Ts) and the center temperature (Tc) of the coal particles were obtained from the images taken by an infrared camera and thermocouples respectively. The ignition processes were recorded by a high-speed camera at different XO2 values and furnace temperatures Tw. Compared with literature experimental data obtained at a high XO2 value, the ignition delay time ti decreases more rapidly as XO2 increases at the low XO2 region. The responses of Ts and Tc to the variation of X O 2 are different: Ts decreases while Tc remains nearly constant with increasing XO2 at a low XO2 value. In addition, ti is less sensitive to Tw while the ignition temperature Ti is more sensitive to Tw at a low XO2 value than in air. Observations of the position of flame front evolution illustrate that the ignition of a coal particle may change from a homogeneous mode to a heterogeneous or combined ignition mode as XO2 decreases. At a low XO2 value, buoyancy plays a more significant role in sweeping away the released volatiles during the ignition process.

Keywords coal particles      low oxygen concentration      ignition      ignition temperature      ignition modes     
Corresponding Author(s): Hai ZHANG   
Online First Date: 08 September 2020    Issue Date: 19 March 2021
 Cite this article:   
Wantao YANG,Yang ZHANG,Lilin HU, et al. An experimental study on ignition of single coal particles at low oxygen concentrations[J]. Front. Energy, 2021, 15(1): 38-45.
 URL:  
https://academic.hep.com.cn/fie/EN/10.1007/s11708-020-0692-1
https://academic.hep.com.cn/fie/EN/Y2021/V15/I1/38
Fig.1  Schematic of experimental system.
Proximate analysis (air-dry basis)/(wt.%) Ultimate analysis (as received)/(wt.%)
Volatile matter Ash Moisture Fixed carbon Carbon Hydrogen Oxygen Nitrogen Sulfur
27.43 12.54 2.73 57.27 71.82 3.84 5.65 0.90 2.52
Tab.1  Properties of tested coal
Fig.2  Measurement of the center temperature of a single coal particle (dp ≈ 2 mm).
Fig.3  Typical images for temperature calibration.
Fig.4  Comparison of dimensionless ignition delay time t* (ti/ti,air) versus X O2 at a low X O 2 values of this paper with experimental data obtained at both low and high X O 2 values from references.
Fig.5  Ignition delay time (ti) versus furnace temperature (Tw) at different X O 2 values.
Fig.6  Comparison of dimensionless ignition temperature T* (Ti/Ti,air) versus XO2 with experimental results obtained at both low and high XO2 values from references.
Fig.7  Ignition temperature (Ti) versus furnace temperature (Tw) in air and low X O2 conditions.
Fig.8  Typical images of volatile flames at different times after ignition for DTC particles at low oxygen concentrations (X O 2) and different furnace temperatures (Tw) (dp ≈ 2 mm).
Fig.9  Dimensionless standoff distance (r*) at a low XO2 value and air at different furnace temperatures (Tw).
Fig.10  Ignition modes for single coal particle at different X O 2 values and furnace temperatures (Tw) (dp ≈ 2 mm).
B Spectral curves of beam splitter
C1 First constant of Planck radiation
C2 Second constant of Planck radiation
D Diameter/mm
DTC Datong coal
G Grayscale
ΔL Deviation between joint and particle center/mm
K Conversion coefficient of the optical system
R Radius/mm
r* Dimensionless standoff distance (x/rp)
T Temperature/K
T* Dimensionless temperature (Ti/Ti,air)
ΔT Temperature difference/K
wt Mass fraction
x Distance of flame front away from particle center/mm
X Molar fraction
τ Time/s
τ* Dimensionless time (τi/τi,air)
λ????? Wavelength/mm
ε Emissivity
σ Error/K
c Center
i Ignition
O2 Oxygen
p Particle
s Surface
w Wall
  
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