1.20 Characteristic speed power curves
If the mean effective pressure (mep) and the mechanical efficiency of an engine remained constant as the speed increased, then both the indicated and brake horsepower would increase in direct proportion to the speed, and the characteristic curves of the engine would be of the simple form shown in fig. 1.5, in which the line marked 'bmep' is the product of indicated mean effective pressure (imep) and mechanical efficiency, and is known as
brake mean effective pressure (bmep). Theoretically there would be no limit to the horsepower obtainable from the engine, as any required figure could be obtained by a proportional increase in speed. It is, of course, hardly necessary to point out that in practice a limit is imposed by the high stresses and bearing loads set up by the inertia of the reciprocating parts, which would ultimately lead to fracture or bearing seizure.
Apart from this question of mechanical failure, however, there are reasons which cause the characteristic curves to vary from the simple straight lines of fig. 1.5, and which result in a point of maximum brake horsepower being reached at a certain speed which depends on the individual characteristics of the engine.
Characteristic curves of an early four-cylinder engine of 76.2 mm bore and 120.65 mm stroke are given in fig. 1.6. The straight radial lines tangential to the actual power curves correspond to the power lines in fig. 1.5, but the indicated and brake mean pressures do not, as was previously assumed, remain constant as the speed increases.
On examining these curves it will be seen first of all that the mep is not constant. It should be noted that full throttle conditions are assumed - that is, the state of affairs for maximum power at any given speed.
At low speeds the imep is less than its maximum value owing partly to carburation effects, and partly to the valve timing being designed for a moderately high speed; it reaches its maximum value at about 1800 rev/min, and thereafter decreases more and more rapidly as the speed rises. This falling off at high speeds is due almost entirely to the lower volumetric efficiency, or less complete filling of the cylinder consequent on the greater drop of pressure absorbed in forcing the gases at high speed through the induction passages and valve ports.
When the mep falls at the same rate as the speed rises, the horsepower remains constant, and when the mep falls still more rapidly the horsepower will actually decrease as the speed rises. This falling off is even more marked when the bmep is considered, for the mechanical efficiency decreases with increase of speed, owing to the greater friction losses. The net result is that the bhp curve departs from the ideal straight line more rapidly than does the ihp curve.
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If a suitable scale is applied, the bmep curve becomes a 'torque' curve for the engine that is, it represents the value, at different speeds, of the mean torque developed at the clutch under full throttle conditions - [...]