Marc, Matt etal 

Two problems I see with your analysis. 

First is minor - Your equation 1 show a linear variation with temperature, 
whereas it should show a 4th power. But you were using the proper fourth power 
in your Excel spread sheet - so this was just a typo. 

More serious is your assumption that the metal portion of the mesh is 10%. This 
is appropriate only for a very few mesh per inch and fine wire. My guess is 
that Paul's mesh could be more like 30-40% - which will change your conclusion 
a great deal. See pages like: 

http://www.twpinc.com/wire-mesh/TWPCAT_12/p_014X014S0170W48T 

So this is to ask Paul Olivier for a visual check on what he was using in his 
particular strainer. A manufacturer and model number would be helpful, if 
available 

Conversely, I worry about assuming the mesh was as high as 750 degrees - based 
on the color in Paul's photo. But I am used (vaguely - long time ago) to 
looking at solid materials through a peep hole in ceramic kilns. The openness 
of the mesh must affect our visual color/temperature calibrations. Anyone up on 
that? 

I'd like to know more about the maximum possible kiln power level - by knowing 
the amount of rice husk consumed per unit time (same as question asked by 
Crispin, I think). From this we can start to compute the convective heat 
transfer coefficient. In other words, what part of the output energy was not 
getting into the cookpot? I think we can assume a larger portion of the 
radiative energy was captured than of the convective. 

Also the amount of water evaporated should be easy to measure rather than 
guesstimate. I also would feel better running longer and using the weight 
evaporated for these energy capture-power computations. 

Ron 

----- Original Message -----
From: "Marc Pare" <[email protected]> 
To: "Discussion of biomass cooking stoves" <[email protected]> 
Sent: Saturday, March 17, 2012 6:30:50 AM 
Subject: [Stoves] Radiation Analysis for Gasifier 


Hi all, 


First a short story, then a presentation of some analysis I've been working on 
the last week (with the help of Crispin and Matt Redmond). You can skip the 
story, if you like. 


the story 
My friend Isaac from Tech tells of his most traumatic experience training to be 
an engineer: "We were giving a presentation on a design of a hybrid vehicle. 
The professor asks us why we choose one particular motor over another. 'Oh, it 
was bigger, so we figured it would be better.' The professor stopped them 
there. Stood up, turned to the class, and yelled: "ENGINEERS QUANTIFY!" 


the results 
In the spirit of Isaac's legendary professor, I sought to provide some clarity 
to the speculation of radiative heat transfer and improved cook stoves by doing 
some simple analysis. 


The setup was simple: what is the theoretical upper bound on contribution to 
heat transfer by the "dome-shaped emitter" described over the last week. 


It turns out that the dome-shaped emitter has negligible impact on the heat 
transfer . Further testing supported this conclusion, but I figured it was 
worth showing how we were able to show with theory that the dome-shaped thing 
was not important. 


The results place the upper bound on power from the emitter at 0.301 kW vs. the 
power required to boil water at 1.65 kW . 
This means that even at 100% efficiency, the emitter will only improve your 
thermal performance by about 20%. (not the reported 100% improvement) 


I attached a pdf explaining the theory and a spreadsheet of the calculation. 
You can also get them here: 
http://notwandering.com/radiation.php 



thanks 
Matt Redmond for a first pass on the spreadsheet 
Crispin for quadruple-checking the spreadsheet and adding improved water 
boiling numbers 




feedback is welcome. there is always the chance that there are mistakes! 


Best, 
Marc Paré 
B.S. Mechanical Engineering 
Georgia Institute of Technology | Université de Technologie de Compiègne 

my cv, etc. | http://notwandering.com 



On Sat, Mar 17, 2012 at 2:05 PM, Crispin Pemberton-Pigott < 
[email protected] > wrote: 





Great! 



Marc you are doing us a great service. Simply by collecting the little 
spreadsheets circulated here, one can gain a good education in stove design. 



The volunteer’s efforts are always rewarded. 



Many thanks 

Crispin 




+++++++ 



# I appeal to Marc not to hide his light under a bushel. These discussion also 
need numbers and methods so the reality of things becomes widespread. 




Write-up is coming :) 


Putting in some effort so that it's a useful resource for folks in the future. 


Marc Paré 
B.S. Mechanical Engineering 
Georgia Institute of Technology | Université de Technologie de Compiègne 

my cv, etc. | http://notwandering.com 




On Sat, Mar 17, 2012 at 1:55 PM, Crispin Pemberton-Pigott < 
[email protected] > wrote: 


Dear Alexis and Paul 



Thanks so much for the very open discussion and open design of the burners. 
Alexis, when we met in Thailand you mentioned that you have switched to a 
premixed flame and if you recall we did talk a bit about the top end of the 
version of the stove you demonstrated. 



Is it correct that you are now using a premixed flame? I have been in extensive 
conversation with Paul O about the burner for some time and it seems at present 
to be a blend of premixing with secondary air and as Paul says, some tertiary 
air for the final burnout. 



The difference in performance that Paul mentioned and which got some much 
discussion going about heat transfer from the hot dome could have at least 
three quite different origins and there is a lot of merit in tracking down the 
difference. The first might be that the structure under the pot on Paul’s 
present configuration is much more closed than the one I saw in Thailand. That 
could account for all the difference in the boiling time. A second possibility 
is the reduction in excess air either through the burner where flames are 
present or between the flames and the final departure of the pot and stove 
structure, by which I mean the outer ring. Until the hot gases leave the pot 
and vent into the room, the air present in that gas stream is technically part 
of the combustor. If there is a lot of cold air entering the region under the 
pot, then it is counted as excess air in the heat exchanger. 



Paul, thanks for putting the pictures of the development work you are doing. It 
is helpful for those who would like to work on stoves with minimal equipment to 
see how things work and what has been tried. It saves a lot of reinventing. 



With regard to the heat transfer from a radiant dome, Marc has been doing some 
calculations which I hope he will post here when he is confident in the method. 
That should settle the question as to whether or not a large increase in 
performance can be obtained by changing hot, relatively non-IR radiant gas into 
IR emitted from a wide gauze surface. 



It is well worth remembering that because a flame is pale blue in the visible 
range, that does not tell us what it is emitting in the IR which is invisible 
to human eyes. Looking through a translucent flame is not really a measure of 
emissions of heat. If you point an IR gun at a flame it will register a high 
temperature, even if it is as inaccurate as an unshielded thermocouple. 



I agree with the others that the discussion about heat transfer has been a good 
exploration of the subject. I appeal to Marc not to hide his light under a 
bushel. These discussion also need numbers and methods so the reality of things 
becomes widespread. 



Regards 

Crispin 




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