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Comparison of the rate of smoke generated from the combustion of biomass fuels by Dr. John Orrin
[top] [end]IntroductionSmoke has been defined as the products of burning organic materials in which small solid and liquid particles are also dispersed[1]. For communities that rely on open or three stone fires for cooking in poorly ventilated areas, smoke provides a threat due to its toxicity. This often results in smoke related illness[2].The amount of smoke generated is sensitive to a wide range of variables such as the orientation of the fuel on the stove, the size and geometry of the fuel, the temperature and the ventilation. The smoke chamber however allows the fuel alone to be examined under precisely defined and constant conditions[3]. When a fire is first started or when new fuel is introduced onto the fire, the fuel will be subject to non flaming (that is smouldering) combustion. If the fuel is carbon based, high levels of smoke are produced initially due to thermal pyrolysis and evolution of volatile matter. The combustion products with high boiling point condense as they mix with the cooler air and this produces a mist of minute droplets. These droplets combine together to give larger droplets of the order of 1mm that can then deposit on surfaces to give an oily residue[4]. When smoke is present in a room, the visibility is reduced because light is scattered and absorbed by the smoke particles. By measuring the visibility or optical density within the room, the amount of smoke can be measured. The optical density is defined as: (O.D.) = log10 ( Io/I ) Where: O.D. = Optical Density Io = initial intensity of light I = final intensity of light after passing through smoke If 50% of the light is absorbed by the smoke particles, then: Io =100 and I = 50 and the optical density = log10 (100/50) = 0.3. For an optical density per path length of smoke of 0.3, the visibility is about 4 metres5. For a smoke filled room that has been caused by a poorly vented stove, the visibility would be much higher than this value and the optical density lower. For example, a visibility of 10 metres and optical density per path length of smoke of about 0.1 might be typical values. [top] [end]Equipment Used For The Measurement Of Smoke
The sample of biomass fuel is first placed in a sample holder and the sample holder plus biomass fuel is weighed on a digital balance to three decimal places. The sample holder is then placed on the guide rails away from the radiant heat source. The door of the smoke chamber is shut and the software programme that controls the smoke chamber is started. The photo multiplier unit is calibrated so that 100% of the light passes across the smoke chamber (corresponding to no smoke). Drawing the biomass sample in front of the heat source then starts the test. As smoke is produced, the amount of light reaching the photo multiplier unit is reduced and the computer continuously records the results. When the light reaching the photo multiplier tube has been reduced by 30%, the test is stopped and the sample removed from the smoke chamber. The sample plus sample holder is again weighed and the amount of biomass fuel used is calculated. The test is then repeated for the next fuel. [top] [end]Results and Discussion
It was found that all the biomass fuels tested fall into one of three groups.
Fig. 6 shows the relationship between the average rate of mass loss of the biomass fuel and the time to produce smoke. Group 1 fuels produced smoke quickly with cardboard producing almost twice the same amount of smoke for a given mass loss as peanut shells. Group 2 fuels took much longer to produce smoke but had a much lower average rate of mass loss. Group 3 fuels (cardboard (wet) and Eucalyptus leaves) were outside the curve shown in Fig. 6 due to the high water content of these biomass fuels.
[top] [end]ConclusionsThe time required to produce a fixed quantity of smoke has been measured for a number of different biomass fuels. Each biomass fuel has been subject to the same radiant heat source and the same radiant intensity. This simulated the conditions whereby a fuel is first introduced onto a fire and produces smoke by non flaming (smouldering) combustion. The fuels were broadly classified into three groups. The first group (straw, hay, peanut shells and dry cardboard) had a low bulk density and would produce a large amount of smoke quickly if allowed to smoulder on an open fire. The second group (wood and chipboard) took much longer to produce the same amount of smoke for a given mass loss. The third group (wet cardboard and air dried Eucalyptus leaves) contained large amounts of water and took very much longer to produce a given amount of smoke again for a given mass loss. This last group would have produced large quantities of water vapour (not smoke) for a given mass loss. The results indicate the benefits of making briquettes of the fuel. Samples of briquettes could be tested using this equipment and the composition of the briquette varied to find the minimum rate of smoke production under non flaming (smouldering) conditions.[top] [end]Notes and References
[top] [end]Download the original article Comparison of the rate of smoke generated from the combustion of different biomass fuels by Dr. John Orrin (526 KB)[top] [end]Contents: Boiling Point 54 - Climate change and household energy
Categories: Boiling Point 54| Smoke | ||||||||||||||||
Page created:
02 February 2008; Last edited:
03 February 2008; Version: 0 | ||||||||||||||||
Pagename: BP54:RatesOfSmokeEmissions @HEDON: NYHA | ||||||||||||||||








Comparison of the rate of smoke generated from the combustion of different biomass fuels by Dr. John Orrin (526 KB)