MaxRaceSoftware
Automotive
- Nov 24, 2001
- 291
Ivymike...i should have posted this article 1st ..but i just found it
..from SuperFlow concerning what we are discussing
Fuel Flow When Accelerating
You only have to run a few tests on an accelerating engine with your SuperFlow Dynamometer system to discover that the power output and the air-fuel ratio change with the speed of acceleration. An understanding of fuel flow within the engine can shed light on these changes. What happens to fuel delivery when the engine is accelerating? How does fuel flow differ when the engine is running at steady speed?
When an engine is running at a steady speed, fuel is mixed with air and travels down the port as spray flow. Some of the fuel is vaporized and behaves exactly as air does. Other fuel remains in droplet form. These un-vaporized fuel droplets will partially coat the walls of the ports as a result of turns and general turbulence. This will create a slow moving flow along the wall which ranges from .010" to .020", (.25 to.5mm), thick. Moving much more slowly than the spray flow, this fuel moves down the port and breaks off at the valve, where it enters the cylinder as additional spray droplets. When the engine is running at a steady speed, the wall flow and the spray flow reach a point of equilibrium, delivering the desired air-fuel ratio to the cylinder. When the engine speed changes suddenly, as during acceleration from 4,000 rpm to 5,000 rpm, the spray flow rushes to the new equilibrium point almost immediately, but the slow moving wall flow requires almost 100 engine cycles before it reaches the higher flow level.
The net result is that the engine cylinder receives insufficient fuel at the increased speed operating point for the first 100 cycles. The engine runs lean, and may stumble and miss. The traditional solution is to add an accelerator pump that delivers extra fuel during the transition. This additional fuel travels down the port primarily as spray flow and works to overcome the momentary lag in the wall flow fuel delivery.
When the engine is already running at full throttle under rapid acceleration, the accelerator pump has no effect. In this case, the normal solution is to increase the jet size so that the engine will run rich. Unfortunately, the engine then always operates rich during full throttle; a richness that is greater than necessary, if the engine was running at a constant speed. That is why the engine may stutter or blubber due to a rich air-fuel ratio.
On the dynamometer, you will generally find that the engine requires one or two steps richer to achieve maximum power under acceleration tests than during steady state tests at the same speed.
In a race car application, engines frequently accelerate at different speeds, rates, and times. First gear acceleration might exceed 2,000 rpm a second, while fifth gear acceleration may be less than 100 rpm a second as a vehicle reaches top speed. The same air-fuel ratio will not be correct in both situations. Currently, there is no mechanical carburetion system that can compensate for this problem.
If you want to determine how much enrichment is required for your particular engine, it is necessary to run a series of tests at progressively richer settings at each of the acceleration rates your engine will experience in its normal application. You will probably discover that the richest setting is required for the highest rate of acceleration and the leanest setting for the best steady speed power. You cannot determine the correct mixture by the air-fuel ratio, but only by the net power produced. For a performance application, you should select the mixture for the acceleration rate that will be used the greatest portion of the time.
Production engines experience this problem to a lesser degree, because of increased manifold heat and the higher vapor pressure of typical pump gasoline. The extra manifold heat evaporates the wall flow back into the air stream and also promotes vaporization of the droplets of fuel and the spray flow.
Unfortunately, manifold heat also increases the temperature of the air charge and reduces the volumetric efficiency at maximum power.
To determine how quickly air and fuel flow systems respond during acceleration testing, you can perform a simple test. If you have a SF-901 system, put the test select knob in the standard test position and set the auto test rate to 25. (With these settings, data is collected every .25 seconds and averaged by exponential decay over 0.8 of a second.) Run the engine at a constant speed, such as 3000 rpm at full throttle, and push the auto test button.
After 3 seconds, increase the speed rapidly by flipping the speed control knob upward approximately 500 rpm. Let the engine run another 10 seconds at this point and push stop test. If you print this set of test data, you will see the actual air and fuel flow readings: first at 3000 rpm and then at the higher test speed. By comparing the data changes over time, you can determine how long it takes to reach a stable reading.
This test should be the worst possible combination, because you are using the longest data averaging time while making the most rapid step change possible. You will probably discover that it requires 5 to 7 seconds to reach a stable data point.
Larry Meaux (meauxrace2@aol.com)
Meaux Racing Heads
MaxRace Software
ET_Analyst for DragRacers
..from SuperFlow concerning what we are discussing
Fuel Flow When Accelerating
You only have to run a few tests on an accelerating engine with your SuperFlow Dynamometer system to discover that the power output and the air-fuel ratio change with the speed of acceleration. An understanding of fuel flow within the engine can shed light on these changes. What happens to fuel delivery when the engine is accelerating? How does fuel flow differ when the engine is running at steady speed?
When an engine is running at a steady speed, fuel is mixed with air and travels down the port as spray flow. Some of the fuel is vaporized and behaves exactly as air does. Other fuel remains in droplet form. These un-vaporized fuel droplets will partially coat the walls of the ports as a result of turns and general turbulence. This will create a slow moving flow along the wall which ranges from .010" to .020", (.25 to.5mm), thick. Moving much more slowly than the spray flow, this fuel moves down the port and breaks off at the valve, where it enters the cylinder as additional spray droplets. When the engine is running at a steady speed, the wall flow and the spray flow reach a point of equilibrium, delivering the desired air-fuel ratio to the cylinder. When the engine speed changes suddenly, as during acceleration from 4,000 rpm to 5,000 rpm, the spray flow rushes to the new equilibrium point almost immediately, but the slow moving wall flow requires almost 100 engine cycles before it reaches the higher flow level.
The net result is that the engine cylinder receives insufficient fuel at the increased speed operating point for the first 100 cycles. The engine runs lean, and may stumble and miss. The traditional solution is to add an accelerator pump that delivers extra fuel during the transition. This additional fuel travels down the port primarily as spray flow and works to overcome the momentary lag in the wall flow fuel delivery.
When the engine is already running at full throttle under rapid acceleration, the accelerator pump has no effect. In this case, the normal solution is to increase the jet size so that the engine will run rich. Unfortunately, the engine then always operates rich during full throttle; a richness that is greater than necessary, if the engine was running at a constant speed. That is why the engine may stutter or blubber due to a rich air-fuel ratio.
On the dynamometer, you will generally find that the engine requires one or two steps richer to achieve maximum power under acceleration tests than during steady state tests at the same speed.
In a race car application, engines frequently accelerate at different speeds, rates, and times. First gear acceleration might exceed 2,000 rpm a second, while fifth gear acceleration may be less than 100 rpm a second as a vehicle reaches top speed. The same air-fuel ratio will not be correct in both situations. Currently, there is no mechanical carburetion system that can compensate for this problem.
If you want to determine how much enrichment is required for your particular engine, it is necessary to run a series of tests at progressively richer settings at each of the acceleration rates your engine will experience in its normal application. You will probably discover that the richest setting is required for the highest rate of acceleration and the leanest setting for the best steady speed power. You cannot determine the correct mixture by the air-fuel ratio, but only by the net power produced. For a performance application, you should select the mixture for the acceleration rate that will be used the greatest portion of the time.
Production engines experience this problem to a lesser degree, because of increased manifold heat and the higher vapor pressure of typical pump gasoline. The extra manifold heat evaporates the wall flow back into the air stream and also promotes vaporization of the droplets of fuel and the spray flow.
Unfortunately, manifold heat also increases the temperature of the air charge and reduces the volumetric efficiency at maximum power.
To determine how quickly air and fuel flow systems respond during acceleration testing, you can perform a simple test. If you have a SF-901 system, put the test select knob in the standard test position and set the auto test rate to 25. (With these settings, data is collected every .25 seconds and averaged by exponential decay over 0.8 of a second.) Run the engine at a constant speed, such as 3000 rpm at full throttle, and push the auto test button.
After 3 seconds, increase the speed rapidly by flipping the speed control knob upward approximately 500 rpm. Let the engine run another 10 seconds at this point and push stop test. If you print this set of test data, you will see the actual air and fuel flow readings: first at 3000 rpm and then at the higher test speed. By comparing the data changes over time, you can determine how long it takes to reach a stable reading.
This test should be the worst possible combination, because you are using the longest data averaging time while making the most rapid step change possible. You will probably discover that it requires 5 to 7 seconds to reach a stable data point.
Larry Meaux (meauxrace2@aol.com)
Meaux Racing Heads
MaxRace Software
ET_Analyst for DragRacers