Gerald Morris
Senior Member
THIS is the greatest controllable variable we have aside from pump capacity for determining flow rate. A Word to the Wise from this is to be SURE and RETAIN some thermostatic control. I once pulled the thermostat on a 1955 Chevy Apache L6-296 engine during the most miserable summer of my life on the advice of an "elder" TO NO GOOD END. Why? NO CONTROL! That motor took a good half hour to warm up, assuring MUCH WASTED PETROL on short trips.The actual flow rate is throttled by the thermostat.
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The rate of heat transfer is proportional to the difference in temperature. (This can be shown from @Gerald Morris formula above. All other variables held constant, the rate of heat transfer Q is proportional to the temperature difference T2-T1.) ....
All combustion engines work best when the delta T is LARGE, as this assures that one then can have a HIGH POWER REACTION in the region of combustion. One must convey the exhaust heat away rapidly when so doing. Power after all is the measure of delta Q over delta t, (Joules/second --> Watts) which we aspire to translate mechanically into Newton * meters/second, where we rapidly accelerate, then simply work against sundry frictions of the road to maintain constant velocity. Thin cylinder walls help convey the heat away quickly, at the risk of rupture, et cetera.
To optimize cooling then really comes to flow rate, and finding the time it takes to remove exhaust heat. MUCH of this is linear, but I suspect not ALL of it. I'll look into this if I get the time, and let y'all know if I find any higher order stuff to optimize for.
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