Thank you all for your feedback. Dealing with the responses in turn:
Paul,
I would be pleased to see any test results that you can obtain – tests are like gold dust!
I agree that coal consumption is basically a function of air flow. I wondered whether to discuss that in the article, but decided against it. However, I am convinced that rather than consider grate loading, we should probably be looking at air flow per unit grate area and this then dictates a combustion rate PROVIDED CONDITIONS ARE STEADY STATE – that is that the fire thickness is adjusted until it is not changing at a steady air flow.
I also agree that model traction engines tend to run at a lower grate loading than rail locos – generally, there is simply not the load on them (I have a 4" scale Burrell, which I rally). Having said that, the loading on 2" scale engines on a wet rally field can be massive. My friend's 2" Fowler can be "roaring away", while my 4" machine is having a leisurely time of it.
I am not convinced that all the difference between road and rail grate loadings is down to draughting. I agree that the base of a TE chimney is not great for free gas passages. However, the tall gently tapering chimney is a massive improvement in draughting over most rail locos (except tall chimney narrow gauge outline machines). I have been doing some work on draughting and have more planned, but the height and gentle expansion of the chimney is an important factor in effective draughting.
With regard to un-burnt fuel, you may not see evidence. From full size practice, about 4% of it will end up in the ashpan with the ash. Of the remainder most is ejected as fine (ish) particles which is the dirt that adorns most steam engines. Another "work in progress" is playing with the Navier Stokes equation to see if I can predict fuel loss on the basis that particles below a certain size will be blown through the fire by the draught. If you are working at relatively low grate loadings, then un-burnt fuel loss will be significantly lower anyway.
I have also been looking at full size practice and they generally recognise two limits to grate loading:
1) Grate limit – the point at which the curve of evaporation rate against grate loading has zero gradient – i.e. putting more coal on does not make any more steam. It should be possible to predict this with my program.
2) Front end limit – the point at which flow in the blast nozzle achieves sonic velocity. Thereafter, attempts to increase throughput result in rapidly increasing back pressure on the cylinders. It will be almost impossible to reach in a scale model where velocities are all scaled, but the working fluid sonic velocity remains constant.
Paul has also drawn my attention to an error in my calculation of heat loss from the boiler casing, which will be somewhat high in the calculation. Fortunately, it is a small part of the whole picture, so is not a major blow. Nevertheless, something to be corrected in the next issue – yes I am working on an upgrade.
J. Hancock
Yes, part of correcting the current lagging loss calculation will allow me to include that.
Richardandtracy
The calculation of "Available steam volume for power" depends on a curve fit of Bill Hall's test results of condensation loss on a 5" gauge cylinder (Speedy, actually). When you consider the effect of scale, the surface available for condensation changes as the square of scale, but the total volume of steam obviously varies as the cube. Hence, the condensation losses must be heavily dependent on scale. Hence my warning.
I have noodled around a bit to try and calculate a scale effect from first principles. Not happy with it yet, but that bit of work is "resting" – not dead.
In between all this, I am trying to build a model.
Thank you all for your interest.
Martin