Abstract A combustible mixture of air and minute fuel droplets is produced for supply to the cylinders of an internal combustion engine. This mixture is formed by accurately controlling both the atomization of fuel and the mass flow rate of air over substantially the entire operating range of the engine. These controls are accomplished by introducing liquid fuel into a stream of intake air and uniformly distributing the fuel in the air followed by passing the air and fuel mixture through a constricted zone to increase the velocity of the mixture to sonic. The sonic velocity air at the constricted zone divides the fuel into minute droplets that are uniformly entrained throughout the air stream. The area of the constricted zone and the quantity of fuel introduced are adjustably varied in correlation with operating demands imposed upon the engine. Downstream from the constricted sonic zone, the air and fuel mixture is accelerated to supersonic velocity in a supersonic zone without imparting substantial turbulent flow thereto. Thereafter the mixture is decelerated to subsonic velocity in a subsonic zone to produce a shock zone where the fuel droplets entrained in the air are believed to be further subdivided and uniformly distributed throughout the combustible mixture before the mixture is supplied to the engine cylinders. The supersonic and subsonic velocities occur in a gradually increasing cross-sectional area corresponding to that of a conical section having an apex angle in the range of about 6 to 18 degrees.
A method for delivering a gaseous medium at a controlled mass flow rate to a downstream location subject to a range of variable pressure conditions comprising the steps of flowing a gaseous medium from an upstream entry point toward the downstream location, passing the gaseous medium through a variable area constricted zone to increase the velocity thereof to sonic, passing the gaseous medium immediately downstream from the variable area constricted zone through a zone of gradually increasing cross-sectional area substantially corresponding to that of a conical section having an apex angle in the range of about 6° to 18° and having an exit comprising the downstream location in order to gradually reduce the velocity of the gaseous medium and efficiently recover kinetic energy as static pressure, and adjustably varying the cross-sectional areas of the constricted zone and the zone of gradually increasing cross-sectional area in accordance with mass flow rate requirements of associated equipment in communication with the downstream location and to which the gaseous medium is to be delivered whereby the kinetic energy of the gaseous medium recovered as static pressure within the zone of gradually increasing cross-sectional area maintains the velocity of the gaseous medium through the constricted zone sonic where the pressure at the downstream location is at or below a predetermined value less than the gaseous medium pressure at the entry point but substantially more than 60% thereof so that the mass flow rate of the gaseous medium, at a given entry temperature and pressure, is directly proportional to, and is determined by the cross-sectional area of the constricted zone.
Claim 2
Independent Claim
264 words
A method for delivering a gaseous medium at a controlled mass flow rate to a downstream location subject to a range of variable pressure conditions comprising the steps of flowing a gaseous medium from an upstream entry point toward the downstream location, passing the gaseous medium through a variable area constricted zone to increase the velocity thereof to sonic, passing the gaseous medium immediately downstream from the variable area constricted zone through a zone of gradually increasing cross-sectional area substantially corresponding to that of a conical section having an apex angle in the range of about 6° to 18° and having an exit comprising the downstream location in order to gradually reduce the velocity of the gaseous medium and efficiently recover kinetic energy as static pressure, and adjustably varying the cross-sectional areas of the constricted zone and the zone of gradually increasing cross-sectional area in accordance with mass flow rate requirements of associated equipment in communication with the downstream location and to which the gaseous medium is to be delivered whereby the kinetic energy of the gaseous medium recovered as static pressure within the zone of gradually increasing cross-sectional area maintains the velocity of the gaseous medium through the constricted zone sonic where the pressure at the downstream location is at or below a predetermined value less than the gaseous medium pressure at the entry point but substantially more than 60% thereof so that the mass flow rate of the gaseous medium, at a given entry temperature and pressure, is directly proportional to, and is determined by the cross-sectional area of the constricted zone.
Claim 3
Dependent Claim
17 words
A method as in claim 1 wherein the gaseous medium pressure at the entry point is atmospheric.