Paul:  Your and my last were also to the stove list, so I re-insert the list 


On Aug 17, 2013, at 8:06 PM, Paul Olivier <[email protected]> wrote:

> See comments below.
> 
> 
> On Sun, Aug 18, 2013 at 8:03 AM, Ronal W. Larson <[email protected]> 
> wrote:
> Paul and List:
> 
>     Three comments/questions:
> 
>     1.  The gas analysis from Belonio was apparently at 1000C in the hot 
> char, but you believe you are closer to 500 C?
> 
> This 1000 C is not the temperature of the gas that exits the reactor. It is 
> the process temperature in the zone where C combines with O2 to form CO2. 
> This reaction supplies the heat for the endothermic reactions that follow. 
> These endothermic reactions cool down the gas as it exits the reactor. The 
> temperature of the gas as it exits the reactor (and prior to combustion) 
> reaches as high 500 C. This we were able to measure.
        {RWL1:   I am comfortable with the 500 C number, but I remain concerned 
that 1000 C may be too high for the (or most) pyrolysis from max temps.  
Numbers I recall seeing with thermocouple readings have never been that high.

> 
>     2.  Is there any way to know what the air equivalency ratio is as you are 
> operating?  even if you are above or below the optimum (of 0.3)?   I guess 
> this is determined by the CO measurements, but I haven't seen any data for 
> either TLUDs or rockets on that.
> 
> If too much oxygen is supplied to the process as is the case of an air 
> equivalency ratio of 0.6, the amount of carbon monoxide produced can drop by 
> over 50% and the amount of H2 produced can drop by almost 60%. The reactor 
> will heat up to dangerously high levels. We can try to correlate the specific 
> rate of solids consumption to the flow of primary air to determine the 
> equivalency ratio. But I have never done this.
           [RWL2:  I hope that they will jump into this dialog if they have 
seen anything on this ratio in tests or literature.  I am still unsure what 
"equivalency" means,  does it include excess air concepts?
>  
> 
>     3.  Some reading this exchange may not realize that you light the 
> pyrolysis gases before adding the burner assembly,
> 
> Before adding the burner assembly, I do not light the gases. I am merely 
> lighting the biomass. When the biomass lights, a large flame rises out of the 
> reactor.
      [RWL3:  This is what most TLUD users live with  (and same for rockets).  
A tall diffusion flame

> When the burner is placed on the reactor, this large flame within the reactor 
> must go out. There should never be open flames within the reactor, otherwise 
> I get burner holes that do not support a flame.
>  
> then you drop the fan speed to extinguish the interior burning and can then 
> relight the 80 flame lets.  
> 
> Yes. At this point, I do not "relight" but "light" the burner holes for the 
> first time.
       [RWL4.  This was point I was making- because only you and Belonio are 
doing this  (a top surface with lots of small holes - that seems to work very 
well), I think.
>  
> Other than Belonio,  I don't know anyone else doing this.
> 
> I am totally confused. How then do they get the open flames within the 
> reactor to go out?
>       [RWL5.  They are "happy" with the flame as is.  For one thing, the 
> "chimney" they are using provides draft that you (with a fan) don't need.
>  
> In your final sentence, people may not realize that your flamelets are still 
> diffusion type, not premixed.   I know no-one getting premixed flames,  
> either rockets or TLUDs.
> 
> This morning I will test a 250 unit with a secondary air pipe that runs from 
> the reactor grate at the bottom of the reactor into the burner at the top. 
> This pipe is situated fully inside the reactor. This burner has 50% more 
> burner holes than a normal burner to account for the added flow. If this 
> works, this will be true premix burner.
         [RWL:  I look forward to hearing (actually I did hear - and not so 
good, for reasons we have discussed - which I will let you report).      Ron
> 
> Thanks.
> Paul
> 
> 
> On Aug 17, 2013, at 5:54 PM, Paul Olivier <[email protected]> wrote:
> 
>> It is challenging to try to understand what happens in a char-making TLUD. 
>> My exposure to stoves has been entirely limited to the work of Belonio, both 
>> from a practical and theoretical side. On the theoretical side, the 
>> following is what I have gleaned from Belonio with the help of a young 
>> engineer from the University of Delft. I throw this out to the list with 
>> great trepidation, since I have only been working on this reflection for 
>> about a week.
>> 
>> Temperature is very important, and it is generated as C reacts with O2 
>> giving rise to CO2 (initial combustion that supplies heat to the process). 
>> The O2 is supplied from the primary air and from the H2O within the biomass. 
>> The temperature has to be high enough to optimize the endothermic reactions 
>> that take place within the process. The endothermic reactions are the water 
>> gas reaction (C combines with H2O to form CO and H2) and the Boudouard 
>> reaction (C combines with CO2 and to form CO).  If the temperature is high 
>> enough, C will not combine with H2 to form methane. If the temperature is 
>> high enough, there will be little tar and oil formation. The goal is to 
>> create a high percentage of CO and H2. 
>> 
>> Then there is the moisture content of the biomass. A moisture content of 10% 
>> is ideal. If there is too much water in the biomass, water is transformed 
>> from a liquid to a gas within the process, and the process temperature is 
>> lowered. Also if there is too much water, the water gas shift reaction is 
>> favored giving rise to CO2 and H2. So if the moisture content increases 
>> beyond what is optimal, there is less CO, more CO2 and more H2O in the gas. 
>> 
>> Then there is the amount of oxygen being supplied to the process. If too 
>> much oxygen is supplied, the amount of CO and H2 decreases, and the amount 
>> of CO2 and H2O increases. Excess oxygen burns up CO and H2 within the 
>> reactor. This translates into a big inefficiency, since the heat generated 
>> here is generally quite far away from the bottom of the pot. Part of the 
>> oxygen comes from the water, and the rest from the primary flow of air. An 
>> air equivalency ratio of 0.3 is ideal. 
>> 
>> But air must be supplied uniformly up through through the biomass. 
>> Channeling (too much air in some places and not enough in other places) 
>> severely disrupts the entire process. In such a case, the concept of an 
>> ideal air equivalency ratio becomes somewhat meaningless. Some people design 
>> TLUD stoves that handle all types of biomass. But I only know of about 4 or 
>> 5 types of biomass that are sufficiently uniform to be run through a TLUD in 
>> their raw state. Everything else has to be prepared (splitting, cutting, 
>> chipping or pelletizing) to be rendered sufficiently uniform. Of all forms 
>> of preparation, pelletizing appears to be the best.
>> 
>> If rice hulls are processed at 1000 C, at an equivalency ratio of of 0.3 and 
>> at a moisture content of 10%, the gas content consists of 26.1% CO, 20.6% 
>> H2, 0% CH4, 6.6% CO2 and 8.6% H20 (numbers from Belonio). This adds up to 
>> 61.9% of the total gas. The remainder is mostly N2. 
>> 
>> The presence of CO2 and H2O in the gas gives rise to a dirty gas. In a stove 
>> test, it would be interesting to measure the CO2 and H2O content of the gas 
>> prior to combustion at the burner. If CO is intimately mixed with CO2 and 
>> H2O, the combustion of CO at the burner is compromised.
>> 
>> When the gas is burned at the burner, heat is generated by the combustion of 
>> CO and H2. Air is about 21% oxygen and 79% nitrogen, and it takes 
>> considerably less oxygen to burn CO and H2 than other more complex forms of 
>> gas such as methane, propane or butane. The molar ratio of air to gas to 
>> burn the CO and H2 in the above proportions is roughly 1.11 mol/mol. The 
>> mixing ratio of air to gas by volume is roughly 0.42 m3/m3. Also if the gas 
>> prior to combustion has a temperature in excess of 500 C, this facilitates 
>> the combustion of CO and H2. If anyone would like to see these calculations, 
>> I will supply the spreadsheet off-list.
>> 
>> This might explain why the Belonio burner with the burner housing I added to 
>> it functions reasonably well in spite of the fact that the premixing of air 
>> and gas does not take place. So little secondary air is required, the gas is 
>> hot, and the mixing takes place all along the periphery of the two off-set 
>> rings of burner holes. As the gas exits the 80 burner holes, it does so 
>> under mild pressure and sucks in air from the burner housing.
>> http://www.youtube.com/watch?v=84qDsbBO9p8
>> 
>> I have seen several rice hull gasifiers where gas exits through one large 
>> burner hole in the middle of the burner. This produces a single flame with a 
>> long diffusion tail, and the transfer of heat to the pot under such 
>> conditions cannot be optimal.
>> 
>> So in conclusion, the process temperature within the reactor should be 
>> higher than 700 C, the moisture content of the biomass should be less than 
>> 12%, the air equivalency ratio should be about 0.3, the biomass should be 
>> sufficiently uniform, the temperature of the gas prior to combustion should 
>> be in the range of about 500 C, the gas prior to combustion should contain 
>> little CO2 and H2O, and the mixing of secondary air with gas should as 
>> thorough as possible.
>> 
>> Thanks.
>> Paul Olivier
>> 
>> 
>> 
>> 
>> On Sun, Aug 18, 2013 at 12:19 AM, Ronal W. Larson 
>> <[email protected]> wrote:
>> 
>> http://www.et.byu.edu/~tom/classes/733/ReadingMaterial/Jenkins-Baxter.pdf
>> 
>> "Stoichiometric air fuel ratios …………..for biomass they are 4 to 7,"
>> 
>> I have seen "6" a lot, and the inverse (fuel to air weights) would be 17%
>> 
>> 
>> On Aug 17, 2013, at 5:49 AM, Alex English <[email protected]> wrote:
>> 
>> 
>>> Ron, Paul,
>>> Below; Paul refers to 'equivalency ratio'. This would be the amount of 
>>> primary (under fuel air)
>> 
>>          [RWL:  Alex,  thanks  _ I wasn't thinking this way.  For your 
>> moving grate design, this term  "under fuel air" makes sense.  But for 
>> TLUDs,   I believe the term "under" makes less sense, as all the O2 is used 
>> up at the pyrolysis front, regardless of its magnitude in volume per unit 
>> time.  Since it would seem that CO needs about half the oxygen as CO2  
>> (except some O2 is coming from the biomass and we have to account for H2 
>> going to H2O), maybe a number near half  (meaning the 30% and 60% numbers 
>> below) makes sense.  Or, maybe Paul's definition of equivalency ratio 
>> includes excess air - not stoichiometric air.  Paul - do you have a cite we 
>> can go to?
>> 
>>> divided by the theoretical amount of air (stoichiometric) for complete 
>>> combustion of that fuel. Then he speaks of CO2, CO and H2 production and 
>>> syngas quality and variable fuel moisture contents.  It would be nice to 
>>> see data that would correlate to his instance #2. I have yet to see "Syn" 
>>> gas composition measurements from a TLUD.  "process temperature might be 
>>> below 500C" Where does this number come from?
>>> 
>>       [RWL:  I am going to stay away from this, due to press of other 
>> business.  The above cite with Tom Miles as co-author might have some of 
>> this.   I think the 500 C term means at the pyrolysis front.  Would you go 
>> higher?
>> 
>>> "A lot of CO is emitted by the stove" 
>>> Here he refers to CO that fails to be combusted in the burner portion of a 
>>> stove making it sound like it is a consequence of conditions that occur in 
>>> the fuel bed. "Syn"gas quality does affect burner performance but burner 
>>> parameters also affect stack CO emissions.
>>>      [RWL:  Maybe,  but I think Paul is repeating what I heard often at the 
>>> Stove Camp.    All the stoves burning char (not done in TLUDs usually) 
>>> suffer from very high CO production.  (emphasis added below in Paul's 
>>> comment).
>> 
>> 
>>> Instance #3 seems plausible.
>>>        [RWL:  Agreed.  but there should be a paper to see the details and 
>>> definitions.]      Whew -  this is a good topic - but I need something more 
>>> to read.   Thanks to both Paul and Alex.      Ron
>>> 
>>> 
>>> Alex
>>> 
>>> 
>>> 
>>> 
>>> 
>>> 
>>> 
>>> 
>>> 
>>> Paul writes;
>>> 
>>> Ron,
>>> 
>>> One should look at a stove according to what it is designed to use as fuel. 
>>> Let us look, for example, at stoves that process rice hulls. 
>>> 
>>> In a first instance, the stove might simply burn rice hulls. Here we are 
>>> talking about direct combustion where an air equivalency ratio situates 
>>> close to 1. Such a stove will produce a lot of CO2 and H2O as well as 
>>> relatively high levels of CO. The fuel for such a stove is rice hulls.
>>> 
>>> In a second instance, the air equivalency ratio might be 0.6, the process 
>>> temperature might be below 500 C, the moisture of the biomass might be 20% 
>>> or more, and too much secondary air might be applied to the combustion of a 
>>> dirty syngas containing a lot of CO2 and H2O. Since the production of CO 
>>> and H2 is suboptimal, it might make sense in this instance to burn the char 
>>> in order to maximize the production of energy. But unfortunately burning 
>>> the char has serious problems: a lot of CO is emitted by the stove, and 
>>> heat is generated far below the pot. If the char is burned within this 
>>> second stove, the fuel for such a stove is rice hulls.
>>> 
>>> In a third instance, the air equivalency ratio situates close to 0.3, the 
>>> process temperature rises above 800 C, the moisture content of the biomass 
>>> situates at 10%, and the supply of secondary air is kept low, but still 
>>> adequate, to achieve total combustion of the syngas. Here the production of 
>>> CO and H2 is optimized, the temperature of the syngas prior to combustion 
>>> at the burner reaches as high as 500 C, and not too much secondary air is 
>>> mixed in with the syngas. In this instance, up to 30% of the weight of the 
>>> rice hulls would still remain as biochar. But it would make no sense to 
>>> burn this biochar, since the production and combustion of the syngas were 
>>> optimized.
>>> 
>>>> 
>>> 
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>> 
>> 
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>> 
>> 
>> 
>> -- 
>> Paul A. Olivier PhD
>> 26/5 Phu Dong Thien Vuong
>> Dalat
>> Vietnam
>> 
>> Louisiana telephone: 1-337-447-4124 (rings Vietnam)
>> Mobile: 090-694-1573 (in Vietnam)
>> Skype address: Xpolivier
>> http://www.esrla.com/
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> 
> 
> 
> 
> -- 
> Paul A. Olivier PhD
> 26/5 Phu Dong Thien Vuong
> Dalat
> Vietnam
> 
> Louisiana telephone: 1-337-447-4124 (rings Vietnam)
> Mobile: 090-694-1573 (in Vietnam)
> Skype address: Xpolivier
> http://www.esrla.com/

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