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Hi,
The benz fluid drive coupling power loss follows this equation (RAE ref E/2410/2/6/13.D).
P_v=P_comp ((N_in-N_out)/N_out )
Where, Pv is power to oil heating, Pcomp is supercharger impeller compressor drive power and N is shaft speed.
In other words the losses to oil
are highest when the coupling is doing its thing. The slip was around 2.5 %, the power loss
at locked condition was hence less as per equation above. The tests show
that at 0.7/1 (max slip) you`re loosing 42% of the supercharger drive power to oil.
For a 601-E, at 1.3Ata at GND>5000feet zone the coupling looses 39bhp in pure oil heating alone,
at 1.15ata (hence lower compressor pressure ratio) its reduced to 24bhp. So it doesnt take
long to imagine whats happening with fairly moderate boost increases. Going up 0.15 Ata
boost puts 61% more power to oil.
Once you`re at 17,000feet or above thats reduced to nominally insignificant (in the case
of this particular engine in that particular condition, it depends on how the secondary
control pump is set to come online).
Not too bad as long as you`re just going up and down once. But evidently if you do any sort of
time in the band between min and max slip, you need a much bigger oil cooler. I do not
know much about air operations as I`m just an engines man - but just saying that is the
case with this type of drive. Conversely it was stated by other studies that in a pure intercept
and return home scenario the coupling was actually quite nice, as it warmed the engine up
fast, and then the losses become small above rated height. So it all depends (like all
engines) on deciding what the exact nature of the application is.
Geoffery Wilde at Rolls did a study on the coupling for Stanley Hooker, as he had worked
previously with these couplings and knew their workings. Because the Merlin was a smaller
engine they knew they would have to boost it considerably higher than the DB in order to
have a chance. This means higher compressor air power, hence in a Merlin with a higher
pressure ratio compressor, the power lost to the coupling will go up and up.
Geoffery worked out that a Merlin equipped with a fluid drive (there are layout drawings
and a complete theoretical set of curves), that with projected boost developments,
that the drag of the required oil cooler would almost nullify the advantage of the
coupling (which is basically that it "fills-in" the area under the "saw-tooth"
pattern of a gearbox equipped supercharged aero engine).
This is further complicated by the characteristics of the Fottinger coupling,
which follows this mathematical behaviour.
Pt=ρ x d^5 x n^3 x c
Where Pt = power transmission capacity (Watts), d= outer diameter of coupling (m), ρ= oil density (kg/m^3), n= shaft speed (rads/sec) and c=a geometry constant (depending on the shape of internal ribs of the particular coupling and so on).
To get a compact installation Geoffrey worked out that running it off the back of a crank (like a automatic gearbox in a modern car) you`d need a huge toriod.
So (like Benz) realised it needed to be speeded up (see the n^3 term). However once you do this the viscous heating losses go up further.
This tended to sludge up the couplings, because the oils were pretty awful back then compared to what we run now, so you would often find the superchargers
on the DB not performing to factory spec at the mid-end of their lives. I`ve got a coupling here thats in "as used" condition and it extremely gummed up
inside. Not a design error really, just something that one aspect of tech. of the day didnt quite deliver on in real life. I think if Geoffery had
done the study for Stanley 6 months prior, they would definetly have at least built a test-stand.
Geoffery and Stanley hooker both visited Sinclair Fluid Drives in person to discuss
developing the coupling into the Merlin - but within a month hostilities officially
started and all efforts swung into "get the most out of what we`ve got now".
Hence the Merlin with fluid drive never happened for these two reasons.
In other words, if you want a larger lower boosted engine the fluid drive is better,
because the losses into oil are less and hence smaller oil cooler = lower drag = more speed.
If you study the Merlin vs DB series compressor power - you`ll see the Merlin expends
considerably more shaft power driving its impeller. Which it would as it was nearly
always running at a higher pressure ratio than the DB. Another very good reason
why DB used methods to increase power late-on that didnt involve running
extremely high pressure ratios in their compressors (eg Nox), as
that power comes from direct chemical energy not increasing the compressor
pressure ratio.
Kind Regards
Calum
Hi,
The benz fluid drive coupling power loss follows this equation (RAE ref E/2410/2/6/13.D).
P_v=P_comp ((N_in-N_out)/N_out )
Where, Pv is power to oil heating, Pcomp is supercharger impeller compressor drive power and N is shaft speed....
....Geoffery and Stanley hooker both visited Sinclair Fluid Drives in person to discuss
developing the coupling into the Merlin - but within a month hostilities officially
started and all efforts swung into "get the most out of what we`ve got now".
Hence the Merlin with fluid drive never happened for these two reasons.
In other words, if you want a larger lower boosted engine the fluid drive is better,
because the losses into oil are less and hence smaller oil cooler = lower drag = more speed.
If you study the Merlin vs DB series compressor power - you`ll see the Merlin expends
considerably more shaft power driving its impeller. Which it would as it was nearly
always running at a higher pressure ratio than the DB. Another very good reason
why DB used methods to increase power late-on that didnt involve running
extremely high pressure ratios in their compressors (eg Nox), as
that power comes from direct chemical energy not increasing the compressor
pressure ratio.
Kind Regards
Calum
Hi,
The benz fluid drive coupling power loss follows this equation (RAE ref E/2410/2/6/13.D).
P_v=P_comp ((N_in-N_out)/N_out )
Where, Pv is power to oil heating, Pcomp is supercharger impeller compressor drive power and N is shaft speed.
In other words the losses to oil
are highest when the coupling is doing its thing. The slip was around 2.5 %, the power loss
at locked condition was hence less as per equation above. The tests show
that at 0.7/1 (max slip) you`re loosing 42% of the supercharger drive power to oil.
For a 601-E, at 1.3Ata at GND>5000feet zone the coupling looses 39bhp in pure oil heating alone,
at 1.15ata (hence lower compressor pressure ratio) its reduced to 24bhp. So it doesnt take
long to imagine whats happening with fairly moderate boost increases. Going up 0.15 Ata
boost puts 61% more power to oil.
Once you`re at 17,000feet or above thats reduced to nominally insignificant (in the case
of this particular engine in that particular condition, it depends on how the secondary
control pump is set to come online).
Not too bad as long as you`re just going up and down once. But evidently if you do any sort of
time in the band between min and max slip, you need a much bigger oil cooler. I do not
know much about air operations as I`m just an engines man - but just saying that is the
case with this type of drive. Conversely it was stated by other studies that in a pure intercept
and return home scenario the coupling was actually quite nice, as it warmed the engine up
fast, and then the losses become small above rated height. So it all depends (like all
engines) on deciding what the exact nature of the application is.
Geoffery Wilde at Rolls did a study on the coupling for Stanley Hooker, as he had worked
previously with these couplings and knew their workings. Because the Merlin was a smaller
engine they knew they would have to boost it considerably higher than the DB in order to
have a chance. This means higher compressor air power, hence in a Merlin with a higher
pressure ratio compressor, the power lost to the coupling will go up and up.
Geoffery worked out that a Merlin equipped with a fluid drive (there are layout drawings
and a complete theoretical set of curves), that with projected boost developments,
that the drag of the required oil cooler would almost nullify the advantage of the
coupling (which is basically that it "fills-in" the area under the "saw-tooth"
pattern of a gearbox equipped supercharged aero engine).
This is further complicated by the characteristics of the Fottinger coupling,
which follows this mathematical behaviour.
Pt=ρ x d^5 x n^3 x c
Where Pt = power transmission capacity (Watts), d= outer diameter of coupling (m), ρ= oil density (kg/m^3), n= shaft speed (rads/sec) and c=a geometry constant (depending on the shape of internal ribs of the particular coupling and so on).
To get a compact installation Geoffrey worked out that running it off the back of a crank (like a automatic gearbox in a modern car) you`d need a huge toriod.
So (like Benz) realised it needed to be speeded up (see the n^3 term). However once you do this the viscous heating losses go up further.
This tended to sludge up the couplings, because the oils were pretty awful back then compared to what we run now, so you would often find the superchargers
on the DB not performing to factory spec at the mid-end of their lives. I`ve got a coupling here thats in "as used" condition and it extremely gummed up
inside. Not a design error really, just something that one aspect of tech. of the day didnt quite deliver on in real life. I think if Geoffery had
done the study for Stanley 6 months prior, they would definetly have at least built a test-stand.
Geoffery and Stanley hooker both visited Sinclair Fluid Drives in person to discuss
developing the coupling into the Merlin - but within a month hostilities officially
started and all efforts swung into "get the most out of what we`ve got now".
Hence the Merlin with fluid drive never happened for these two reasons.
In other words, if you want a larger lower boosted engine the fluid drive is better,
because the losses into oil are less and hence smaller oil cooler = lower drag = more speed.
If you study the Merlin vs DB series compressor power - you`ll see the Merlin expends
considerably more shaft power driving its impeller. Which it would as it was nearly
always running at a higher pressure ratio than the DB. Another very good reason
why DB used methods to increase power late-on that didnt involve running
extremely high pressure ratios in their compressors (eg Nox), as
that power comes from direct chemical energy not increasing the compressor
pressure ratio.
Kind Regards
Calum
Since the DB 601 et al was the larger engine but weighed about the same as the Merlin it would seem to be the better execution of a V -12 design. For a given fuel flow the larger displacement allowed for greater conversion of heat energy to power. Conversely, the Merlin would have a hotter exhaust that saw low efficiency in power extraction as through exhaust thrust and such. Both greater stress through higher boost and larger components tend to drive engine weight. Just an opinion but I see the Merlin as the result of evolution that involved compromises (of spec creep) while the DB was more of a clean sheet of paper design.
So I guess one is faced with the choice of a multi-speed geared supercharger drive, a torque converter driven supercharger, or a turbo charger.
The latter seems to avoid some of the issues of the former, while creating some of its own.