Mechanical Efficiency of Heat Engines

Appendix C: Derivation of Schmidt Gamma Equations

The following derivation supplies the equations needed for Chapter 10 and follows the nomenclature described there.

VOLUME AND PRESSURE FUNCTIONS

The instantaneous volume of gas in the hot and cold spaces of the engine are


and


The instantaneous total engine volume V is then


In terms of the total swept volume V T = V 1 + V 2 = V 1(1 + ?) of the piston and displacer,


By the assumptions made, instantaneous pressure within the engine is


where m is the total mass of gas captive within the engine and R is its ideal gas constant. Putting the expressions obtained above for V H and V C in the denominator of the last expression gives the following expression for the instantaneous pressure:


The factor in the brackets in the denominator can be written in the following form:


where


Let


The analysis is limited to ? in the range 0 < ? < ?. Then B > 0, and A is positive or negative according to whether ?/(1 ? ?) > cos ? or not. Corresponding to whether A is positive or negative, ? will be in Quadrant I or II. With ? thus defined,


where


Therefore,


It is easily seen then that


Then the root mean cycle pressure can be written as


It can be checked that this is the exact same expression that...

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