JOURNAL of the JAPANESE SOCIETY of AGRICULTURAL MACHINERY
Online ISSN : 1884-6025
Print ISSN : 0285-2543
ISSN-L : 0285-2543
Combustion Characteristics of Husk Charcoal
Hiroshi SHIMIZUToshinori KIMURAYoshio NISHIYAMATsutomu TERUI
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JOURNAL FREE ACCESS

1982 Volume 44 Issue 1 Pages 79-84

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Abstract

The authors developed a new device for the purpose of studying the combustion of various husk charcoal and experiments were conducted to obtain the relations between combustion and specific air flow rate G. The results were as follows.
1. Maximum combustion temperature Tp was related to specific air flow rate G. The value for Tp yielded the highest value of 1350°C when G was 0.56Nm3/min. kg. In order to decrease the value for Tp, in was required that the vales for G was sufficiently smaller than 0.56Nm3/min. kg. The suction aeration was the most recommended method to realize such condition.
2. The value for Tp was hardly related to the carbon ratio φ of the husk charcoal. The values Tp for moistened materials became slightly smaller than those of dried materials. The critical specific air flow rates Gp were nearly equal to 0.56Nm3/min kg for all experimental conditions.
3. Combustion propagation velocity was expressed as a power function of specific air flow rate G. Theoretical flame temperatures Tth which were calculated for boundless bed had a linear correlation to specific air flow rates G. If the specific air flow rate G increased. the steep increase was shown for both combustion propagation velocity Vf and maximum combustion temperature Tp, which might give an explosive combustion and a dangerously high temperature.
4. An exponential correlation was observed between theoretial excess air ratio m calculated from eq. (2) and specific air flow rate G. The values for m considering boundless bed approached 1.0 asymptotically, while more practical values for Mth which were calculated from using θf′ instead of θf in Fig. 2 took the value 2.0. When m took the value 1.0, the calculated value for Tth was 2550°C.
5. Theoretical flame temperature Tth′ was determined from the combustion propagation velocity Vf′ which was obtained by more practical combustion time θf′ The relation between the theoretical flame temperature Tth and the specific air flow rate G was similar to the relation between the observed maximum temperature Tp and the specific air flow rate G.
6. The deviations of Vf from the regression curve had a slight positive correlation as to the bulk densities ρ of the husk charcoal. So the bulk density ρ did not have a significant effect on the combustion characteristics of husk charcoal.

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