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1, this gives: Ps Xs CPs CGs=0 Xs=Xi+Xr-l=l FLOW TO THE ATMOSPHERE (B) OPEN END OUTFLOW Hence, Xr=2-Xi. 6) For compression waves, as Xi> 1 and Xr Naturally, this table contains only the broadest of classifications and could be expanded into many sub-sets, each with a known band of attainment of brake mean effective pressure. Therefore, it is possible to insert this data into Eq. 1, and for a given engine total swept volume, SV, at a rotation rate, RPS, determine the power output, BPR. It is quite clear that this might produce some optimistic predictions of engine performance, say, by assuming a BMEP of 10 bar for a single-cylinder spark-ignition engine of 500 cc capacity running at an improbable speed of 20,000 rpm. In the measurement of hydrocarbons, either by a NDIR (non-dispersive infrared) device or by a FID (flame ionization detector), the readings are quoted as ppm hexane, or ppm methane, respectively. Therefore Prog. 4 contains, in the appropriate equations, the molecular weights for hexane, CH„, or methane, CH„. 15) and in that case, in the relevant equation in Prog. 85. The same holds true for nitrogen oxide emission, and in Prog. 4 it is assumed that it is to be NO and so the molecular weight for NO, 30, is employed.