Here is a continued discussion of how to calculate steam engine horsepower.
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LOL, that's a good one. Still, you were able to use the first piece for something? I thimpfks NASA's little problem occurred before the space station stuff. it wasd when the Apollo projects were active (me thimpfks.)I seem to recall that the first docking stations in space where precision machined and polished surfaces, and when they docked, they stuck together like superglue.
I think that is when they started coating the mating surfaces with teflon.
I will have to look this up, but I am sure it is true.
I had a similar story when I made the green twin engine.
I had a LOT of bronze boat shaft, and so I thought "This is perfect for bearings", never having made an engine before.
The boat shaft machined like a dream, and the bearings came out great..........but when I assembled the engine, it would not rotate.
I loosened the bearings a bit, added lots of oil, and still, very poor rotation.
Removed the bearings, reamed them oversize, and still, it was like I was using glue instead of oil.
I discovered the property that some metals have called "stiction", and I discovered that while boat shaft bronze is awesome stuff, it is not bearing bronze by any means.
The second set of bearings I made using certified bearing bronze.
Who would have known ?
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One of the reasons I start with the carnot cycle its the best you can ever do for efficiency. And all the other factors can be ignored if you know the heat energy going in and the work coming out of the cycle. That is not to say knowing the other factors has no value because you can work to improve those numbers if you know what they are. I have several older papers on calculating the efficiency of GE steam turbines and the paper is filled with equations. So in some cases more detail is good. I will go back give Hall's paper a read.I know the concept of Carnot efficiency, but have never seen it as really useful in the context of a steam engine, where you have combustion losses, exhaust heat losses, fluid friction losses, exhaust losses, back pressure, mechanical friction, internal leakage, condensation losses etc.
Certainly back in the day, "build one and test it" was the method used to derive output and efficiency or steam consumption for a given power. I was only suggesting that in this day and age it is possible to calculate things from scratch, but if you look at the maths in Bill Hall's paper most folk will probably not want to. For those with a curious mind, Bill Hall sets out the various factors involved very well.
Martin
The mean effective pressure is the area enclosed by the indicator diagram divided by the stroke. Here is an example
Indicator diagram
While the pressure at the start of the stroke might be near to line pressure, as the expansion proceeds pressure drops away quite quickly. You also have fluid friction in ports and passages which tends to round off the corners of the indicator diagram. Then on top of that you have exhaust back pressure which is pushing the piston the "other way". So the MEP is always a lot less than inlet pressure.
All the friction losses increase rapidly with rpm (everything goes faster so friction losses get bigger) then MEP drops away even more. It can all be calculated to a reasonable degree of accuracy, but needs a time step spreadsheet that calculates everything by the fraction of a degree. There is a good paper by Prof Bill Hall on how to calculate it from zip here:
Prof Bill Hall paper
Martin
I read professor Halls paper and found it interesting. He mentioned in the first paragraph the actual fired btu to the drawbar power which is actually a heat rate for power stations. He also quietly mentioned the efficiency was way below the maximum but did not emphasize that. So he obviously looked at analysis from a carnot cycle but I was not able to determine what the high and low temperature was used. But thats not what he was doing. Apparently he also left out more complex details to make the paper easier to read based on his comments.I know the concept of Carnot efficiency, but have never seen it as really useful in the context of a steam engine, where you have combustion losses, exhaust heat losses, fluid friction losses, exhaust losses, back pressure, mechanical friction, internal leakage, condensation losses etc.
Certainly back in the day, "build one and test it" was the method used to derive output and efficiency or steam consumption for a given power. I was only suggesting that in this day and age it is possible to calculate things from scratch, but if you look at the maths in Bill Hall's paper most folk will probably not want to. For those with a curious mind, Bill Hall sets out the various factors involved very well.
Martin
I agree a simple solution is always a good answer. And probably just as accurate given accounting for errors which can occur in gages and instruments.If you actually have an engine, a simple Prony brake with a scale will work fine. If heat disipation is an issue, spray water on it.
Lohring Miller
https://en.wikipedia.org/wiki/Prony_brake
Thank you ever so much - - - - now to reading and digesting and hopefully understanding!!!The mean effective pressure is the area enclosed by the indicator diagram divided by the stroke. Here is an example
Indicator diagram
While the pressure at the start of the stroke might be near to line pressure, as the expansion proceeds pressure drops away quite quickly. You also have fluid friction in ports and passages which tends to round off the corners of the indicator diagram. Then on top of that you have exhaust back pressure which is pushing the piston the "other way". So the MEP is always a lot less than inlet pressure.
All the friction losses increase rapidly with rpm (everything goes faster so friction losses get bigger) then MEP drops away even more. It can all be calculated to a reasonable degree of accuracy, but needs a time step spreadsheet that calculates everything by the fraction of a degree. There is a good paper by Prof Bill Hall on how to calculate it from zip here:
Prof Bill Hall paper
Martin
I've welded brand new AN aircraft fittings together just by spinning them on by hand while chatting. It wasn't like galling and torque was mostly from the inertial spinning. The threads had welded together at atom level and removal left two cylinders. From then on I learned having an interface as simple as natural oil from handling was enough to keep it from happening.I seem to recall that the first docking stations in space where precision machined and polished surfaces, and when they docked, they stuck together like superglue.
I think that is when they started coating the mating surfaces with teflon.
Ah, as I was looking for info on Charles Porter, this HMEM thread poppt up. As I had replied to it already, but re-read it I found I wanted to reply to this part. We all know the approximate workings of a capacitor, that is, how it temporarily stores an electric charge, and we all know how that is very much like a water reservoir or dam stores water, so I wish to add a point, that is, that a storage bulb (it has two names but don't recall either at the moment), near the input of the steam to the valves would act the same way, and thus overcome some of friction losses Martin is writing of. I don't see these enough but some members have written short bits on them.The mean effective pressure is the area enclosed by the indicator diagram divided by the stroke. Here is an example
Indicator diagram
While the pressure at the start of the stroke might be near to line pressure, as the expansion proceeds pressure drops away quite quickly. You also have fluid friction in ports and passages which tends to round off the corners of the indicator diagram. Then on top of that you have exhaust back pressure which is pushing the piston the "other way". So the MEP is always a lot less than inlet pressure.
All the friction losses increase rapidly with rpm (everything goes faster so friction losses get bigger) then MEP drops away even more. It can all be calculated to a reasonable degree of accuracy, but needs a time step spreadsheet that calculates everything by the fraction of a degree. There is a good paper by Prof Bill Hall on how to calculate it from zip here:
Prof Bill Hall paper
Martin
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