Carburetors are reliable, robust mechanisms for efficiently metering fuel to an internal combustion engine. A carburetor meters the appropriate amount of fuel according to engine demand based on intake airflow to the engine. Generally, carburetors operate on the principle that as the velocity of airflow through a restriction increases, its pressure decreases. Carburetors are configured to take advantage of the pressure differential created between atmospheric pressure surrounding the carburetor and a low pressure region created inside the carburetor, usually by way of a venturi. As an engine draws air through the venture, the low pressure region created by the increasing air velocity meters a proportional amount of fuel into the intake airflow stream. As passive devices, carburetors are both reliable and robust, while thoroughly mixing fuel with incoming airflow which enhances efficient combustion.
While carburetors are simple and cost effective fuel delivery systems, modern emission requirements have limited the application of carburetors on newer products. Many applications have implemented electronic fuel injection in order to maintain precise control of fuel delivery, which allows catalytic converters to be used in an emissions reduction strategy. The introduction of electronic fuel injection has added complexity, cost, weight, and increased electronic load to modern engines. Fuel injection systems rely on a sensor network. The failure of any single sensor can drastically reduce the emissions performance of the fuel system.
In order to continue to benefit from the carburetor's advantages, improvements to traditional carburetor design are needed in order to ensure the carburetor's ability to meet emission requirements for modern engines.
Provided herein is a carburetor for an internal combustion engine, comprising a body having an air inlet opening portion, an air outlet opening portion, and a throat portion extending there between. A fuel reservoir is in fluid communication with the throat portion and a slide assembly is movably disposed in the body for movement across the throat portion. The slide assembly includes a throttle slide and a metering rod extending across the throat portion and into the fuel reservoir. The air inlet opening includes a pair of concavities operative to direct airflow toward the metering rod. The concavities begin near a peripheral margin of the inlet opening portion and extend inward as the concavities approach the throat portion. The throat portion includes upper and lower portions and the concavities are adjacent the upper portion.
Also contemplated herein is a carburetor having an air inlet opening that includes a manifold, which may be in the form of an arcuate scoop, adjacent to and extending along a portion of a peripheral margin of the inlet opening portion. The manifold is in fluid communication with the fuel reservoir. The manifold has a volume that is proportional to the cross-sectional area of the throat portion. The throat portion includes upper and lower portions, and the manifold is adjacent the upper portion. This carburetor may also include an air inlet opening that includes a pair of concavities operative to direct airflow toward the metering rod that are located proximate either end of the manifold. Wherein the concavities begin near a peripheral margin of the inlet opening portion and extend inward as the concavities approach the throat portion.
In another embodiment, a carburetor for an internal combustion engine is contemplated that includes a slide assembly movably disposed in the body for movement across the throat portion. The slide assembly includes a throttle slide having a metering rod bore and a positioner bore. A metering rod extends through the metering rod bore and across the throat portion into the fuel reservoir. The slide assembly includes a positioning mechanism operative to adjust the position of the metering rod relative to the throttle slide. The positioning mechanism includes a barrel rotatably disposed in the positioner bore. The barrel is threadably engaged with the metering rod such that rotation of the barrel adjusts the position of the metering rod.
The barrel includes a detent for selectively indexing the barrel in one of a plurality of rotational positions. The detent is operative to engage one of a plurality of indentations located at the bottom of the positioner bore. The indentations may be formed in the bottom of the positioner bore or formed in a detent washer disposed in the bottom of the positioner bore, as examples.
In yet another embodiment, a carburetor for an internal combustion engine is contemplated that includes a throttle slide having an outlet gate and an inlet gate including a flow guide disposed on the inlet gate in alignment with the metering rod. The flow guide bisects an arcuate relief on an underside of the inlet gate thereby forming a pair of funnel-shaped grooves. The arcuate relief may be frusto-conical in configuration and the flow guide may be in the form of a pyramid shaped point. Furthermore, the throttle slide may include a stepped portion disposed on the inlet gate for accelerating an airflow past a lower end of the throttle slide.
A method for configuring the throat of a carburetor to optimize airflow to an engine is also contemplated. Where the carburetor includes an upper portion of a first diameter and a lower portion of a second diameter that is offset from the first diameter, the method comprises deriving an optimum size for the first and second diameters and the offset based on mass airflow requirements of an engine. Broadly, the method comprises determining the venturi flow coefficient (Cv) of the carburetor and determining the mass airflow requirements ({dot over (m)}) of the engine. The optimum size for the first and second diameters and the offset are derived based on the mass airflow requirements and venturi flow coefficient. Both the venturi flow coefficient and the mass airflow requirements may be determined experimentally. In addition, determining the mass airflow requirements of the engine may include measuring the pressure differential (ΔP) and the air density (p).
The method includes resolving the width (w) as a function of throttle slide position (y) according to the equation
The optimum size for the first diameter (Ø1) is selected to match the width (Wwot) at a wide open throttle slide position (Ywot). The optimum size for the second diameter (Ø2) is selected to match the width (Wi) at an idle throttle slide position (yi). The optimum offset (X) is the difference between the wide open throttle slide position (Ywot) and the idle throttle slide position (Yi).
Also contemplated herein is a metering rod for use on a carburetor. The metering rod comprises an elongated cylindrical rod extending along a rod axis and having opposed first and second end portions. A wake generator is formed on the cylindrical rod extending from the first end portion and varying in cross-sectional areas along at least a portion of the length of the cylindrical rod.
In an embodiment, the wake generator comprises a flat region angled with respect to the rod axis and bordered by an elliptical edge. The metering rod may further comprise a plurality of grooves intersecting the elliptical edge.
The wake generator may include grooves that extend parallel to at least a portion of the rod axis and may include an arcuate portion. The wake generator may comprise a concave cross-section, such as, for example, and without limitation a dihedral cross-section.
Basic carburetor design is generally well known to those of ordinary skill in the art. For example, a suitable carburetor to which the present improvements may be applied is described in U.S. Pat. No. 6,505,821 issued Jan. 14, 2003 to Edmonston, the disclosure of which is hereby incorporated by reference in its entirety.
The carburetor, shown in
The geometry of the manifold 20 may be altered to change some characteristics of the carburetor performance. Turbulent flow enters the manifold and comes to rest. It is this conversion of dynamic pressure into static pressure that applies compensating pressure on top of the fuel reservoir. Both the volume and depth of the manifold are elements that damp oscillations in the flow. The length and diameter of the passages 22 leading to the fuel reservoir are of an appropriate ratio to allow viscosity to dominate the fuel driving pressure. The damping acts only upon the transient pressures encountered by the manifold.
The underside 34 of the forward gate 36 of the slide includes two funnel-shaped grooves 38 placed directly to either side of the metering rod location 40. The material between the grooves forms a frenulum or flow guide 42, in the form of a pyramid shaped point or chevron, leading into the flow. The flow guide bisects an arcuate relief on the underside of the inlet gate thereby forming a pair of funnel-shaped grooves. The arcuate relief is preferably frusta-conical in configuration. Flow guide 42 causes the metering rod to appear to have a teardrop-shape within the flow at low throttle position. The funnel-shaped grooves 38 allow air to accelerate to their highest velocity more near to the metering portion of the venturi increasing atomization. Flow separation and the orthogonal surface vector of the feature reduce lift on the slide, which may cause undesirable fluctuations in the fuel delivery. This design has been shown to improve function in the form of lower NOx emissions and a resistance to slide float.
With reference to
In one embodiment, the geometry of the throat 12 includes an upper portion 13 of a first diameter and a lower portion 15 of a second diameter that is offset a distance “X” from the first diameter. The sizes of the circle(s) determine the throttle bore size.
Methods for configuring the throat of a carburetor, such as described above, are also contemplated. The geometry (Ø1, Ø2, X) of throat 12 may be optimized to improve airflow to an engine depending on the engine parameters. Several parameters of carburetor design may be optimized in a prescribed fashion to achieve the highest atomization efficiency and flow for improved performance of an internal combustion engine.
Generally, the method uses the mass airflow requirements ({dot over (m)}) for a particular engine to define the carburetor venturi profile. The mass airflow requirements ({dot over (m)}) are obtained by direct measurement and isolation of the air delivery requirements of a particular engine. The airflow requirements are combined with carburetor venturi flow coefficients (Cv) to define the required throat or venturi area (Av) as a function of throttle slide position.
Regarding measurement of the mass airflow requirements ({dot over (m)}), piston engines, both two-cycle and four-cycle, consume air as part of an unsteady process. Air metering technology is not optimally suited for net mass flow measurement of this unsteady flow. It is advantageous to damp out these perturbations and flow reversions in the case of some two-cycle engines in order to support accurate measurements. Accordingly, the inlet port of the engine is ducted to a vessel of sufficient volume to suppress the effects of unsteady pumping action such that the volume of the vessel is much greater than the displacement of the engine. The vessel is then supplied air at a pressure equivalent to atmospheric or desired conditions by a rotary style blower, for example. Mass flow of air ({dot over (m)}) is measured at the intake of the blower which provides a smooth continuous flow.
Once mass flow ({dot over (m)}) is determined as a function of engine speed and load, the carburetor venturi cross section is calculated. Using the incompressible form of Bernoulli's equation and one-dimensional continuity equation, an equation for ideal mass flow rate can be shown.
{dot over (m)}=A
v√{square root over (2ρΔp)}
{dot over (m)}=Mass Flow Rate of Air
Av=Area of Carburetor Venturi, where Av=f(Slide Position)
p=Air Density
ΔP=Static Pressure Differential of Venturi vs. Atmosphere
Geometry, turbulence, and viscous effects all contribute to reduce the mass flow rate below indicated by the ideal expression. For standard venturi tube profiles, flow coefficients are experimentally determined and included in the mass flow equation. A flow coefficient (Cr) specific to the subject carburetor is similarly determined by experimentation. This coefficient is itself a function of area ratio or slide position, density, and pressure differential. The modified equation is shown below:
{dot over (m)}=A
v
C
v√{square root over (2ρΔP)}
C
v
=f(a,ΔP,slide position)
The mass flow rate ({dot over (m)}), pressure differential (ΔP), and venturi flow coefficient (Cv) are all determined by experimentation as described above, while the density (p) is measured directly from the environment. The mass flow equation can then be solved, as described more fully below, to give an expression for area (Av) as a function of throttle position (y).
For an arbitrary venturi profile, the area of the revealed shape can be described in relation to the shapes in
Combining the mass flow rate equation with the area integral, and solving for the width (w) returns the following expression.
This equation for width (w) as a function of throttle position (y) describes the venturi geometry. As can be appreciated with reference to the integral below, the ideal throat 12 geometry is approximated with two diameters (Ø1, Ø2) separated by a distance (X).
By matching the throat cross section to the engine's characteristics, combustion is improved by improved flow, increased atomization, and consistent fuel delivery. Furthermore, a carburetor tailored, according to the above defined method, will deliver a fuel mixture that is more uniform and consistent and provides a progressive, linear throttle response to the user.
Turning now to
Metering rod 10 is fashioned with a flat 17 to engage a D-shaped washer 63 that is fixed in position by a spring tension from below (spring 65) and a retaining ring 63 from above. The D-shaped washer 63 engages a contour (not shown) within the slide assembly 16 to maintain the angular orientation of the metering rod 10 with respect to the throttle slide 16 and throat portion 12.
With reference to
A combination of features creates a system where liquid fuel is ordered and delivered directly into the region of airflow with the highest shear force. Fuel is directed to the corners formed where the cylindrical surface is interrupted by the flat surface. Droplets are then sheared into much finer particles than when they are simply lifted from the flat into the wake region. Finer atomization allows for more efficient combustion and reduces the production of harmful emissions.
The surface finish of the rod may be sufficiently fine to accurately meter fuel at the metering rod and nozzle interface, yet coarse enough to reduce surface tension effects and allow the fuel to wet into the flat surface of the rod. The cylindrical portion 114 of the rod 110 may be polished to as fine a finish as is economically feasible to reduce wear against the nozzle. A suitable surface finish in may be approximately 25 to 50 micro centimeters and, in at least one embodiment approximately 40-41 micro centimeters. In order to encourage fuel to wick into the rod, large surface discontinuities should be sufficiently reduced. Pockets, pores, or damage from manufacturing processes may all work against the smooth surface adhesion of fuel and discourage flow up the rod.
As seen in
Linear grooves 118 provide good atomization for those grooves which terminate near the maximum cord length of the rod. However, many grooves would terminate near the peak of the ellipse (I.e. edge 120) in the wake region far from the high gradients near the outside edges. In another embodiment shown in
The low pressure inside the wake region behind the metering rod is a primary component in the driving pressure associated with moving liquid fuel into the venturi of the carburetor. The wake generator, such as flat portion 117, of the metering rod may be modified to enhance the formation of the wake and then also the fuel driving pressure. The wake generator of the metering rod can be augmented by a variety of shapes to enhance the wake. For example and without limitation, the wake generator may be in the form of a dihedral section 317 or concave conical section 417 as shown in
Returning briefly to
Accordingly, the carburetor and methods, therefore, have been described with some degree of particularity directed to the exemplary embodiments. It should be appreciated, though, that the present invention is defined by the following claims construed in light of the prior art so that modifications or changes may be made to the exemplary embodiments without departing from the inventive concepts contained herein.
The present application is a divisional of U.S. application Ser. No. 13/807,999 which claims the benefit of PCT/US2011/039254 filed on Jun. 6, 2011. PCT/US2011/039254 is a continuation in part of application Ser. No. 12/913,629 filed Oct. 27, 2010, which claims the benefit of U.S. Provisional Application No. 61/361,117, filed Jul. 2, 2010. Each of these disclosures are hereby incorporated by reference in their entirety.
Number | Date | Country | |
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61361117 | Jul 2010 | US |
Number | Date | Country | |
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Parent | 13807999 | Feb 2013 | US |
Child | 14458482 | US |
Number | Date | Country | |
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Parent | 12913629 | Oct 2010 | US |
Child | 13807999 | US |