Guest
When it comes to converting one form of energy one way to mechanical
work only a Pelton wheel can approach an electric motor's 95+%
efficiency.
In sharp contrast all single cycle high compression ratio ICE small
enough to be hauled down a road tops off at 40% efficiency with
vehicle size spark ignition ICE generally running below 30%. That's a
well tuned engine running on it's "sweet spot" rpm.
Why can't anyone do much about the sorry efficiency of 99.9% of the
prime movers on the planet?
Far and away the biggest problem comes from the basic thermocycles of
adiabatic engines, i. e., gas turbines (Brayton/Joule/Ericsson I),
diesel (Diesel) and spark ignition (Otto).
The machinery dictates the processes and the shape of the thermocycle
and even the idealized [read: fantasy] adiabatic cycle doesn't fill a
Carnot or other isothermalized parallelogram cycle -- the
thermodynamic limit of heat engines -- very well. Materials
temperature limits reduce the Carnot limit below 100%, so maybe a
little over 50% Carnot for most ideal adiabatic cycles.
The real cycle, however, looks more like a paramecium. The nice
sharply defined corners of the ideal have been rounded reducing
efficiency still more.
Toss in incomplete combustion and other parasitical losses and
electric motors start to look pretty.
Bret Cahill
work only a Pelton wheel can approach an electric motor's 95+%
efficiency.
In sharp contrast all single cycle high compression ratio ICE small
enough to be hauled down a road tops off at 40% efficiency with
vehicle size spark ignition ICE generally running below 30%. That's a
well tuned engine running on it's "sweet spot" rpm.
Why can't anyone do much about the sorry efficiency of 99.9% of the
prime movers on the planet?
Far and away the biggest problem comes from the basic thermocycles of
adiabatic engines, i. e., gas turbines (Brayton/Joule/Ericsson I),
diesel (Diesel) and spark ignition (Otto).
The machinery dictates the processes and the shape of the thermocycle
and even the idealized [read: fantasy] adiabatic cycle doesn't fill a
Carnot or other isothermalized parallelogram cycle -- the
thermodynamic limit of heat engines -- very well. Materials
temperature limits reduce the Carnot limit below 100%, so maybe a
little over 50% Carnot for most ideal adiabatic cycles.
The real cycle, however, looks more like a paramecium. The nice
sharply defined corners of the ideal have been rounded reducing
efficiency still more.
Toss in incomplete combustion and other parasitical losses and
electric motors start to look pretty.
Bret Cahill