![]() |
help with simplified cDA/cRR formula
I saw a coastdown calculator and wanted some help understanding it before I try and integrate it into the mpguino.
Basically you (or your computer) times a coastdown at high speed (say 55mph to 50mph) and another at low speed (say 7mph to 2mph) and put the speeds and times and weight in and it tells you your cDA and rolling resistance. But I'd like to understand what it is doing a little better. I appreciate that they have approximated things like pressure and temperature for the sake of simplification, but can anyone determine what the "6" on the cDA line represents or the "28.2" on the rr line actually is? The crux of it is: a1=(va1-vb1)/t1; a2=(va2-vb2)/t2; v1=(va1/2)+(vb1/2); v2=(va2/2)+(vb2/2); cDa=((6*m)*(a1-a2))/(v1*v1-v2*v2); rr=(28.2*(a2*v1*v1-a1*v2*v2))/(1000*(v1*v1-v2*v2)); abbreviations: a1: high speed deceleration a2: low speed deceleration v1: high speed average velocity KPH v2: low speed average velocity KPH cDA: coefficient of drag * area rr: Rolling resistance va1: high speed start KPH vb1: high speed end KPH va2: low speed start KPH vb2: low speed end KPH m: mass in Kilograms Other conversion factors 1 mile = 1.609344 KM 1 pound = 0.45359237 kilograms |
shameless bump (maybe this belongs in instrumentation?)
|
Quote:
In standard metric units (mks - metres/kilograms/seconds) there should be 2/1.2 in stead of "6" and 1/9.8 instead of "(28.2.../(1000...". So, re-written: cDa=((2*m)*(a1-a2))/((1.2)*(v1*v1-v2*v2)) rr=(a2*v1*v1-a1*v2*v2)/(9.8*(v1*v1-v2*v2)) From the (hand-derived) math: - the "2/1.2" is the reciprocal of the standard 0.5*'rho' ['rho' being the density of air @ 1.2 kg/m^3] - the 1/9.8 is the reciprocal of acceleration due to gravity [9.8m/s^2] As you have stated the speed units as km/h, there are factors of 3.6 (1 km/h = 1000 m / 3600 s = 1m/3.6s). So, used appropriately, one will achieve the original equations with the "6" and "28.2". And, as you have already suspected, the results will be an indication of real values but not absolute. I don't feel like doing the calculus to get the exact results - too time consuming and the external influences when taking the readings will not justify its precision! Also note that there is another component that is often overlooked: a 'viscous' drag - a velocity component in the equation: F = 'rho'/2*cDA*v^2 + cV*v + m*g*cF BTW = this is bringing back memories of my master's thesis... |
Thanx CO, it sounds like it might be good enough for our purposes then. I hope to take a lot of the timing/speed variables out of the equation by having the computer do all that, but I also didn't want to make the user jump through too many hoops about current temp/humidity/pressure/locust density/etc :)
|
Viscous Drag
Quote:
|
Quote:
In a spreadsheet that I have developed (its a beast!), I do include the viscous component - and guestimated it to be ~1 for a 2-wheel drive vehicle (where F(viscous) = cV*v (v in [m/s]). It could be ignored, but will have an influence on the standard pair of coast-down tests (high speed and low speed). Hint: (greater than) 3-speed coast down tests will show this minor factor (did this in uni many years ago w/ driveshaft torque measurement and data logger). This is notably small when compared to the other two inputs: eg. '90 Firefly: @ 25 m/s: F(friction) = 81.3N (cF = 0.010, m = 830kg) F(viscous) = 25.0N F(aero) = 236.3N (cD = 0.36, A = 1.75m^2) [Disclaimer: YMMV, above numbers may or may not simulate real life, ...] |
All times are GMT -4. The time now is 04:20 AM. |
Powered by vBulletin® Version 3.8.11
Copyright ©2000 - 2025, vBulletin Solutions Inc.
Content Relevant URLs by vBSEO 3.5.2
All content copyright EcoModder.com