Intake Nbsp n Nbsp Exhaust+Part1-2
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Design of an Inlet Manifold for a Formula SAE Vehicle, Including Experimental Evaluation
Francis Evans 2002
48
A typical commercial flow bench uses manometers across an orifice plate, to measure the
mass flow rate (usually expressed as CFM @ STP) at a given test pressure. A cylinder head,
or a number of cylinder heads, once tested, can then be run on a calibrated dynamometer. The
readings from the dynamometer can then be correlated with mass flow rate results, for a given
test pressure on a given flow bench.
Commercial flow bench units may be supplied with a series of charts that attempt to relate the
mass flow rate through a cylinder head at a given flow bench test pressure, with expected
dynamometer results.
6.3 Description Of Flowbench Hardware
A flowbench was constructed to specifically evaluate the performance of the air filter, throttle
assembly, and restrictor. The flowbench was constructed with geometry to try and mimic the
flow from the restrictor into a symmetric plenum. The flowbench uses a stagnation pressure
probe, and a static pressure probe (wall tapping) to determine the peak velocity,
downstream, through a 27.5 mm internal diameter pipe. The pipe has a very rough (corroded
galvanised iron) internal surface finish, and is of sufficient length at ensure fully developed
turbulent flow at the pressure probes. By assuming fully developed turbulent flow, we can
also assume a reasonably consistent velocity profile through the pipe over a small range of
Reynolds numbers.
Pitot probes were chosen over an orifice plate so as to reduce the required power of the
vacuum unit, and hence increase the available test pressure. Manometers were favoured over
differential pressure transducers, to reduce error modes, and so that the device could be used
again without the need for sourcing additional hardware (except a source of vacuum).
It must be stressed that this testing device could never accurately measure the true mass flow
rate through the manifolds tested. It is also important to realize that error analysis for the true
mass flow rate is impossible to formulate.
Design of an Inlet Manifold for a Formula SAE Vehicle, Including Experimental Evaluation
Francis Evans 2002
49
The device does provide a very accurate comparison of mass flow rates at a given
downstream (plenum) test pressure. The error analysis for the comparison is easily performed
and yields very encouraging results.
The available blower limits the choice of downstream test pressure. An industrial vacuum
cleaner was borrowed to be the source of vacuum. All testing was conducted at 250 mm of
water, corresponding to absolute plenum pressures near 99.1 kPa.
The temperature of the flow near the Pitot probes was not measured using a stagnant air
temperature probe. Instead, the ambient air temperature was used. It is assumed that this
method did not cause significant error.
6.4 Restrictor Test Without Throttle Bodies
The first flow bench test was a comparison between the current restrictor profile and the
profile used in last years entry. Both profiles exhibit a smooth surface finish. The old profile
can be seen to display a slight mismatch at the tangency between the radius and exit angle.
Fittings were used to bring the flow to the restrictors.
Figure 6-1 Comparison Of 2001 And 2002 Geometry
Both units displayed some level of unsteady stall. This is obvious due to a fluctuating
downstream (test) pressure. It can also be heard (and even felt) upstream. The old profile
displayed a greater level of unsteady stall.
Design of an Inlet Manifold for a Formula SAE Vehicle, Including Experimental Evaluation
Francis Evans 2002
50
The new profile, despite displaying a reduced level of unsteady stall, passed a significantly
lower mass flow rate. (This is difficult to measure, due to the unstable test pressure without
air filter and throttle body, but a 7% reduction is the ballpark figure)
6.5 Modified Area Ratio Test
The new profile was subsequently modified (more correctly a fitting was modified) to match
the area ratio of the old profile.
Figure 6-2 Modified Area Ratio Geometries (2002 Device)
The unsteady stall became more pronounced with this modification, and the mass flow rate
decreased.
It seems likely the new profile is affecting a lower mass flow rate than the old profile due to
geometries upstream of the throat (for tests without air filters and throttle bodies).
The question remains to be answered as to exactly which geometries upstream of the throat
are more favourable on the older profile. Possible geometric sources of increased flow rates
include:
The parallel tract length
Parallel tract diameter
The presence of an inlet angle
The presence of an inlet angle seems most likely.
Design of an Inlet Manifold for a Formula SAE Vehicle, Including Experimental Evaluation
Francis Evans 2002
51
It must be stated that it is somewhat difficult to capture a reading whilst the unsteady stall
condition is present. The same methodology was used for both units, and the difference in
mass flow rates is very obvious, although there is significant inaccuracy in the values.
The modified area ratio test was then performed with the throttle and air cleaner attached. The
flow was steady with the original area ratio, and a slight fluctuation was noted with the
increased area ratio. A reduced mass flow rate was recorded with increased area ratio. The
reduction was 3% +1.9% / -2.4%.
6.6 Testing With Air Filters And Throttle Bodies
The new and old profiles were again tested with throttle bodies and air filters (Note: The new
profile was tested with its original area ratio). Both units display fairly stable flow. The 2002
unit is very stable, and the 2001 unit fluctuating very slightly. This is a somewhat puzzling
situation. Obviously the addition of an air filter and throttle body was likely to cause some
reduction in mass flow rate, and hence lower Reynolds numbers.
White suggests that separation increases with boundary layer thickness prior to diffusion. The
addition of an air filter and throttle body might be decreasing the boundary layer thickness.
The level of swirl might also be having an effect.
With the addition of air filters and throttle bodies, the new profile has a lower mass flow rate
at the given test pressure, a reduction of 7% + 1.9% / -2.4%.
Interestingly, dynamometer results show that this years engine has decreased in maximum
power (7% 1%).
A series of modified dynamometer tests was used to show that the power decrease is due to
components upstream of the plenum. This is explained in detail in section 8.
Design of an Inlet Manifold for a Formula SAE Vehicle, Including Experimental Evaluation
Francis Evans 2002
52
7 Dynamometer TestingThe dynamometer testing for this study was performed at Stafford Tune. The dynamometer
operator was Mr. Paul Masterson. Mr Masterson is a renowned dynamometer operator who
specialises with engines using Motec engine management systems. The dynamometer at
Stafford tune is regularly calibrated. Inertia correction, and barometric compensation is also
available. Stafford tune claim their hardware to be accurate within 1%. An SAE J607
correction factor was used for test readings.
The engine was coupled to the dynamometer using a cardan shaft. The inertia corrected power
figures are the values of power at the shaft. The actual engine exhaust system was in place for
dynamometer testing.
The engine systems need be mapped before power readings are taken. This means that the
parameters of injector pulse width and spark timing are programmed over a range of throttle
positions and engine speeds.
Once the engine is mapped, it can be run at WOT over its operating rpm range, and
horsepower readings taken.
Figure 7-1 Engine At Dynamometer Testing
Design of an Inlet Manifold for a Formula SAE Vehicle, Including Experimental Evaluation
Francis Evans 2002
53
7.1 Plenum Comparisons
The first series of comparative tests involved changing between two plenums, whilst using the
new restrictor, throttle body and air filter. The two plenums are both of symmetric design, and
both use the same runner lengths. The difference is that the 2002 plenum has significantly less
volume. The 2001 plenum is 3800 cc whilst the 2001 plenum is 980 cc. The 2002 plenum has
a smaller runner spacing within the plenum.
Plenum Comparison
0.0
10.0
20.0
30.0
40.0
50.0
60.0
4000 5000 6000 7000 8000 9000 10000 11000 12000
rpm
2002 Nm2001 Nm2002 Kw2001 Kw
Figure 7-2 Plen