Low Temperature Stirling Engines



Theory 6 - Pressurization of ideal Stirling cycle engines

Optimally buffered engines

When increasing by a factor K the mean pressure of optimally buffered ideal cycle engine we increase by a factor K the number of gas molecules in the workspace.

According to equation presented in chapter 5, the output shaft work is also increased by a factor K. Optimally buffered engines means that the buffer pressure is also increased by a factor K (to be equal to internal mean pressure).

This linear relationship between shaft output and mean pressure keeps true for non-ideal optimally buffered engines.

Engines buffered from bellow

By definition engines of that kind have a workspace pressure that is always higher then buffer pressure. This kind of engines are not advantageous from a theoretical point of view (optimally buffered engines are better) but could be advantageous to solve technical issues (to avoid large external pressure vessels, to prevent lubricant migration etc...)

stirling cycle bfb

Starting from equation of chapter 3, the mechanical efficiency of such engines Emeca_ideal_bfb (buffered from below) is:

 mechanical efficiency bfb

The condition for the engine to run is

condition bfb engine

Resolving this equivalence gives the following condition for engines buffered from bellow:

condition bfb engine 2

For the very worst case (Pbuffer=0) this condition reduces to E2 >= τ

The output work for each cycle is:

bfb output work per cycle






Theory index

Theory 1 - Generic schematic
Theory 2 - Buffer pressure
Theory 3 - Mechanism effectiveness
Theory 4 - Optimal buffer pressure of the ideal Stirling Cycle
Theory 5 - Output work of engines with ideal Stirling cycle
Theory 6 - Pressurization of ideal Stirling cycle engines
Theory 7 - Crossley cycles engines
Theory 8 - Various losses in real engines





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