On
19 November 2025 at 16:30 JA Said:
Interesting. I would like to have a good think about this but life does not allow it.
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This is complex and DO NOT compare it with the Otto or Brayton cycle.
JA
Werner, please keep us informed of your results.
First, I owe Werner an apology. My first answer told him stuff he already knows because I forgot his previous posts on the subject show he knows how to measure engines!
I’m in the same boat as JA. I’m interested in thermodynamics but don’t have the time to master it. And to be honest, my tiny brain is an obstacle!
Heat engines convert heat into useful power. Theory identifies 6 ways in which the working fluid can be expanded to do work:
- Adiabatic. Hot fluid expands and temperature drops rapidly. Work is delivered quickly, pulsed, not smooth,
- Iso-thermal. Hot fluid expanded such that temperature does not change. Does most work, but slowly.
- Iso-baric. Heat added to maintain constant pressure. Temperature does not change. Less efficient, less power, but constant, which is sometimes exploited. iso-baric is mostly used to add heat to the working fluid for an adiabatic or iso-thermal expansion in the next stage. Diesel engines.
- iso-choric. No work, temperature changes. Mostly used to add heat to the working fluid for an adiabatic or iso-thermal expansion in the next stage.
These expansions can be exploited by designers to maximise efficiency, or power, or torque, or smoothness. And, in a practical engine, to minimise pollution, shocks, excessive temperature, resonances, maintenance and rough running. Ignition is a major factor, as are many other practical considerations. Steam is not an Ideal gas!
Practical cycles include:
- Carnot – sets the upper limit on heat engine efficiency. Although the Victorians put massive effort into building steam and IC engines using the Carnot cycle, it’s impractical. Valuable theory.
- Otto – spark ignition engines. Variations include Miller and Atkinson.
- Diesel – compression ignition engines
- Brayton – jet engines and turbines
- Stirling and Ericson – gas engines
- Rankine – vapour engines Steam engines
Model steam engines should implement the Rankine Cycle. They sort of do, in that their proportions are derived from full-size prototypes, and they produce Rankine-like indicator diagrams. As far as I know, no-one has built a model engine explicitly designed and built to a perfect Rankine cycle. May not be worth the effort because small engines are grossly inefficient due to scale imposed friction and heat losses.
Compressed air does not perform well in a Rankine Cycle engine – a steam engine’s proportions and valve events aren’t optimised to produce the most appropriate adiabatic / iso-thermal expansions. Compressed air works well-enough for testing, but the engine won’t get the best out of it, and, compared with steam, there isn’t much energy in air. Enough heat in it to turn the engine over, but power output is low. How low depends on practical unknowns: possibly the proportions and valve events in a model are so off Rankine that compressed air works better! The only way to find out is to measure it by putting it on a dynamometer and taking indicator diagrams. Indicator diagrams graph pressure vs volume as they change during the stroke, and the shape of the loop shows how close, or not, the engine is to it’s design cycle.
Practical example. In WW2, British Agents were parachuted into occupied Europe. Their radios used thermionic valve that guzzled electricity. A serious problem when operating covertly from a wood! One way was to charge lead-acid accumulators with a hand-cranked or bicycle driven dynamo, both exhausting hard-work. Petrol generators need hard to obtain fuel and were noisy. Stuart-Turner were asked to provide a small steam engine and boiler, also inconveniently heavy, but ran on water and windfall wood. For obvious reasons, compressed air is unsuitable! Compressed air is great in the workshop though. Air-tools could be steam-powered, but…
Dave