This invention relates to four-piston internal combustion engines.
The list of abbreviations used in the text and on the drawings follows.
ICE internal combustion engine
UDP upper dead point of the piston
LDP lower dead point of the piston
CC combustion chamber
RemG remnant gases
ExG exhaust gases
Inv inlet valve
ExV exhaust valve
VacV vacuum valve
StV stop valve
CB cylinder block
CBH head of cylinder block
EC efficiency coefficient
Pmax ICE maximum power, h.-p.
Pexp pressure inside the exhaust pipe
PC Pressure inside a cylinder, atm
VC Cylinder volume
VCC CC volume
Vexp exhaust pipe volume
GT gas turbine
VTP vacuum turbo pump
GTVP gas turbine vacuum pump
Abbreviations on the gas distribution circle diagrams
The opening or closing angle of the valves is measured in the clockwise direction, starting at the UDP of the intake stroke; measured in degrees of rotation of the crankshaft.
0° the reference point—UDP of the start of the inlet stroke
180° LMP of the inlet stroke
360° UDP of the compression stroke
540° LDP of the working stroke
720° UDP of the exhaust stroke
φ angles between the opening and shutting momenta of the valves
α the angle between UDP or LDP and the vales opening momenta of the valves
β angles between UDP or LDP and the shutting momenta of the valves
thick lines correspond to the valves shut position
fine lines, to the valves open situation
The illustrations include:
Operation of different internal combustion engines is discussed, using a single cylinder benzene ICE as an example. Supply and ignition systems are not indicated on the diagrams.
In general, a classic ICE (
The Internal combustion engine is depicted at the end of its outlet stroke, when the piston does not quite reach the 720° point. A classic ICE with two valves per cylinder has a high CO and CH contents on low speeds, while lacking power on high speeds. This is so because the air from the inlet collector is not capable of cleaning (blasting out) the combustion chamber (CC) from remnant gases (RemG) at the end of the inlet stroke/the start of the exhaust stroke (the 720° point). Air-blasting takes place when the valves are overlapped (angle φ34). At that time (see
Doubling the number of inlet or exhaust valves decreases the quantity of RemG in the combustion chamber in the vicinity of 720° (see
Transverse partition wall 9 in the combustion chamber (
Usually, the exhaust of all the cylinders of a multi-cylinder ICE from all the exhaust valves goes into a common collector, then into the system of neutralisation and damping. Due to the considerable hydraulic resistance, generated, mainly, by the damper, pressure in the exhaust collector is higher than the atmospheric pressure virtually during the entire exhaust stroke. This limits the extent to which the cylinder can be filled with a fresh charge and decreases the momentum of the engine. It is a known fact that Pmax of an internal combustion engine with a damper is 10% lower, on the average, than of such an engine without a damper.
In the vicinity of 720°, when one cylinder is being blasted out (
An internal combustion engine, in which ExG together with RemG is force-pumped out with an auxiliary cylinder/3/. Efficiency of this method is low because to form a considerable vacuum (0.5 atm for instance), the auxiliary cylinder has to have a 3-5 times greater volume than the main cylinder.
Another known internal combustion engine /4/ (accepted as the protagonist of this invention, in which at the start of the exhaust stroke (past the upper dead point) 0°, vacuum forms inside the cylinder through a separate valve. That vacuum is low. It is produced by ejection when the exhaust valve opens in another cylinder. However, this vacuum affords some reduction of the amount of RemG and some increase of the charge volume.
A positive effect takes place within a narrow speed range. In different operating conditions of an internal combustion engine, the effect might become negative, which is always observed when there is a gas connection between the cylinders.
We offer two engines based on the same principle to redeem these drawbacks: the ICE shown in
The ICE in
Vacuum in the pipeline and collector is produced by vacuum turbo pump 14. It is activated via pulley 15 from crankshaft 16 via pulley 17 and common belt 18, with reduction of the increase.
The internal combustion engine operates in the following fashion (
The cylinder picks up its charge during its exhaust stroke, compressing it during the following stroke, then the charge is ignited, then follows the working body expansion stroke (the working stroke). At the end of the working stroke, ExV 4 opens at angle α4 with LDP 540°. It lets out the main body of the exhaust gases (ExG) into collector 11 and damper 12. The duration of this is from α4 to αm. Then ExV 4 closes, while VacV 10 opens. While VacV 10 is open and InV 3 and ExV 4 are closed, RemG are pumped out from cylinder 1 by vacuum pump 14. The angle travelled during this time is 180°-αm-α3. During this time, piston 2, due to the vacuum, is pulled inside cylinder 1, carrying out its useful work.
When InV 3 opens and during the overlapping φ3, 10 of the valves, the combustion chamber (CC) is being blasted out by air from the inlet pipe. The RemG leave the chamber and enter collector 13 due to the vacuum produced by turbo pump 14.
When the 720° point has been reached, and a small angle β10 (approximately) 8° has been travelled, VacV 10 shuts. While InV 3 is open, cylinder 1 picks up a new charge during the down travel of its piston 2.
Generally speaking, VacV 10 can be closed even before the 720° point is reached.
When the vacuum in the low pressure collector is high (P=0.1 for example), the quantity of RemG around the 720° point decreases tenfold in comparison with the classic ICE. When this is the case, no air blasting is required, and φ3, 10 angle can be reduced even to zero. This decision depends on the gas distribution modification system.
The main part of the exhaust passes through ExV 4 and collector 11, which work under the most intensive heating conditions. VacV 10 opens later, when the temperature of the ExG in the cylinder is several times lower than at the start of the exhaust stroke, while the pressure slightly exceeds the atmospheric pressure. For this reason, pipeline 14 does not need to be designed to withstand high temperatures.
The most powerful acoustic front (explosion) occurs at the when ExV 4 opens. By the time VacV 10 opens, that noise will have already passed the damper. The flow of the ExG through collector 13 is not associated with much noise and, practically, requires no damper.
Having vacuum inside the cylinder during the exhaust stroke enables the designer to have considerably smaller α4, which has some important consequences:
1) Angle α4 can be decreased to 10-15° (against the usual 40-70°), working stroke angle 180°-α4 can be increased, which improves the efficiency coefficient of the engine.
2) The temperature and pressure of the ExG at the start of the exhaust stroke decrease, which means that the diameters of the exhaust valves can be increased.
3) The pressure of the noise of the working ICE decreases. It is worth noting that the amount of energy used for producing a vacuum in collector 13 is not wasted: it pulls the piston into the cylinder when VacV 10 opens and ExV 4 closes. The diagram in
ExV 4 and VacV 10 can have a φ10,4 overlap (see
The ICE shown in
This ICE is depicted at the end of its outlet stroke; the piston is slightly below the upper dead point (UDP), 720°. See also
Not reaching the 540° point by angle α4, ExV 4 opens, and StV 19 opens simultaneously. Exhaust gases leave cylinder 1 due to excess pressure and flow through the exhaust pipe into high pressure collector 11, then to gas turbine (GT) 20. The rotor of the turbine rotates the axis of the vacuum pump 14, so that a vacuum is formed in the vacuum pipeline and above VacV 10. When the α19+β19 position is passed, StV 19 shuts, while VacV 10 opens (angle α10). Because of the vacuum produced, the exhaust gases (their main bulk has already left the cylinder by that point, so that the pressure inside the cylinder PC≈1.5) flow into the low pressure collector 13. The pressure above the piston inside the cylinder is PC<1. The piston is pulled inside the cylinder, carrying out its useful work. This process continues up to the moment InV 3 opens (angle α3). Then, during the period when the valves 3 and 10 are overlapped (φ3,10 angle), the combustion chamber (CC) is blasted out. When this is completed, VacV 10 and ExV 4 become shut, and, while piston 2 travels downwards, cylinder 1 pick up a new charge via its InV 3. The compression and working strokes are identical with those in a classic ICE.
In this ICE model the outlet pipe (which serves as a receiver) cannot be of a great volume: otherwise too much energy would be required to produce a vacuum in it. On the average, VExP≈VCC.
This ICE keeps its working characteristics at α4<α19 and at α4>α19, tolerates small overlapping of StV 19 and VacV 10 (β19≠α10); when β10>β4, some vacuum will still remain in the exhaust pipe after the air blasting is over. This vacuum will help to remove ExG in the next stroke. The separate GT can generate a high vacuum (pressure at its entrance can measure PTE<0.1) even despite a small α4. This makes having partition wall 9 unnecessary, while the time required for air blasting is very short, and the angle is very small.
In this ICE model, the air for blasting flows through the open ExV 4, cooling it down to the atmospheric temperature (unlike in boost-using ICEs).
The vacuum as such reduces the temperature inside the cylinder, the vacuum at the start of the intake, accelerates the air in the inlet pipe and increases the charge without warming it up. This allows to use greater compression.
Using separate high and low pressure collectors helps avoiding interaction between the cylinders and, consequently, eliminate any failures of the momentum in the entire velocity range.
When the gas-distribution phase modification system is used, it can control InV 3 and ExV 4 as usually or, in a more sophisticated version, InV 3, ExV 4, and VacV 10, or in a simplified version, only VacV 10. Control over VacV 10 provides an opportunity to avoid excess blasting, maintain the vacuum and extract more useful work during the exhaust stroke in other cylinders.
On the whole, the ICE shown in
Number | Date | Country | Kind |
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2011104434 | Feb 2011 | RU | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/RU2012/000079 | 2/8/2012 | WO | 00 | 8/6/2013 |