I don't think you need a "for dummies" version, Gunnar! :0) Let's define two
versions of "engine braking", since I think this is where the confusion in this
thread is coming from:
1. The race car driver's seat-of-the-pants version: Engine braking is how
quickly you slow down when you let off the throttle, regardless of what caused
it (minus aerodynamic drag effects).
2. The engineer's version: Engine braking is the "torque" the engine makes
when you let off the throttle, and is seperate from the acceleration. In this
definition, inertia is not part of the equation at all, so it's irrelevant.
According to "the engineer's version", it would have no effect on engine
braking, however, you think in terms of the "race car driver's version" of
engine braking, as most people probaby do. There's nothing wrong with that, of
course, it's intuitively quite right once you're behind the wheel :0)
So... According to the race car driver's version, a heavier flywheel would do
just the opposite of what you said; it would *decrease* engine braking. Why?
Suppose at 5000 rpm (or whatever speed) we shut the throttles. The engine
makes (wild guess) negative 50 lbs-feet of torque (trying to slow the
car/engine down, the opposite of making power). The engine's inertia with the
normal flywheel is 5 (another wild guess).
The engine's acceleration when you shut the throttle would be:
Acceleration = Torque/inertia
= -50lbs*feet / 5
= -10 radians/sec/sec
= 95 Rpm's/sec
If we put a flywheel that had twice as much inertia (either it was heavier, or
bigger, or a combination of the two), the inertia is 10. The acceleration
would be:
Acceleration = Torque/inertia
= -50lbs*feet / 10
= -5 radians/sec/sec
= 47 Rpm's/sec
Exactly 1/2 of what you had before. So you'd wind up with less engine braking
(according to "the race car driver's definition").
This is somewhat misleading though, because it appears that we've got 1/2 the
engine braking with the heavier flywheel, so if you let off the throttle, you'd
expect the car to slow down about 1/2 as quickly. This doesn't happen though;
this "inertia" effect is rather small compared to what's happening at the
wheels. I'll spare you the math on that part though.
The "engineer's" definition (I know I'm repeating myself here in different
posts and you got it by now) says that the -50lbs*feet _IS_ the engine braking.
This didn't change from one flywheel to the next, so neither did the engine
braking.
Again, neither definition is really wrong imo, it's just a matter of how you
want to define engine braking. Ruud, Jonny, and Collin prefer the "engineer's"
definition though.
Todd Wasson
---
Performance Simulations
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