DE3417349A1 - Machine with complete balancing of the effects of mass - Google Patents

Machine with complete balancing of the effects of mass

Info

Publication number
DE3417349A1
DE3417349A1 DE19843417349 DE3417349A DE3417349A1 DE 3417349 A1 DE3417349 A1 DE 3417349A1 DE 19843417349 DE19843417349 DE 19843417349 DE 3417349 A DE3417349 A DE 3417349A DE 3417349 A1 DE3417349 A1 DE 3417349A1
Authority
DE
Germany
Prior art keywords
mass
counter
crankshaft
shafts
piston unit
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
DE19843417349
Other languages
German (de)
Inventor
Tang Sanh Dipl.-Ing. 1000 Berlin Nguyen
Viet Dipl.-Ing. Vu-Han
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
VU HAN VIET
Original Assignee
VU HAN VIET
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Priority claimed from DE19833310416 external-priority patent/DE3310416A1/en
Application filed by VU HAN VIET filed Critical VU HAN VIET
Priority to DE19843417349 priority Critical patent/DE3417349A1/en
Publication of DE3417349A1 publication Critical patent/DE3417349A1/en
Withdrawn legal-status Critical Current

Links

Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F16ENGINEERING ELEMENTS AND UNITS; GENERAL MEASURES FOR PRODUCING AND MAINTAINING EFFECTIVE FUNCTIONING OF MACHINES OR INSTALLATIONS; THERMAL INSULATION IN GENERAL
    • F16FSPRINGS; SHOCK-ABSORBERS; MEANS FOR DAMPING VIBRATION
    • F16F15/00Suppression of vibrations in systems; Means or arrangements for avoiding or reducing out-of-balance forces, e.g. due to motion
    • F16F15/22Compensation of inertia forces
    • F16F15/26Compensation of inertia forces of crankshaft systems using solid masses, other than the ordinary pistons, moving with the system, i.e. masses connected through a kinematic mechanism or gear system
    • F16F15/261Compensation of inertia forces of crankshaft systems using solid masses, other than the ordinary pistons, moving with the system, i.e. masses connected through a kinematic mechanism or gear system where masses move linearly
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F01MACHINES OR ENGINES IN GENERAL; ENGINE PLANTS IN GENERAL; STEAM ENGINES
    • F01BMACHINES OR ENGINES, IN GENERAL OR OF POSITIVE-DISPLACEMENT TYPE, e.g. STEAM ENGINES
    • F01B9/00Reciprocating-piston machines or engines characterised by connections between pistons and main shafts and not specific to preceding groups
    • F01B9/02Reciprocating-piston machines or engines characterised by connections between pistons and main shafts and not specific to preceding groups with crankshaft
    • F01B9/023Reciprocating-piston machines or engines characterised by connections between pistons and main shafts and not specific to preceding groups with crankshaft of Bourke-type or Scotch yoke
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F02COMBUSTION ENGINES; HOT-GAS OR COMBUSTION-PRODUCT ENGINE PLANTS
    • F02BINTERNAL-COMBUSTION PISTON ENGINES; COMBUSTION ENGINES IN GENERAL
    • F02B1/00Engines characterised by fuel-air mixture compression
    • F02B1/02Engines characterised by fuel-air mixture compression with positive ignition
    • F02B1/04Engines characterised by fuel-air mixture compression with positive ignition with fuel-air mixture admission into cylinder
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F02COMBUSTION ENGINES; HOT-GAS OR COMBUSTION-PRODUCT ENGINE PLANTS
    • F02BINTERNAL-COMBUSTION PISTON ENGINES; COMBUSTION ENGINES IN GENERAL
    • F02B75/00Other engines
    • F02B75/02Engines characterised by their cycles, e.g. six-stroke
    • F02B2075/022Engines characterised by their cycles, e.g. six-stroke having less than six strokes per cycle
    • F02B2075/027Engines characterised by their cycles, e.g. six-stroke having less than six strokes per cycle four
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F02COMBUSTION ENGINES; HOT-GAS OR COMBUSTION-PRODUCT ENGINE PLANTS
    • F02BINTERNAL-COMBUSTION PISTON ENGINES; COMBUSTION ENGINES IN GENERAL
    • F02B3/00Engines characterised by air compression and subsequent fuel addition
    • F02B3/06Engines characterised by air compression and subsequent fuel addition with compression ignition
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F02COMBUSTION ENGINES; HOT-GAS OR COMBUSTION-PRODUCT ENGINE PLANTS
    • F02BINTERNAL-COMBUSTION PISTON ENGINES; COMBUSTION ENGINES IN GENERAL
    • F02B67/00Engines characterised by the arrangement of auxiliary apparatus not being otherwise provided for, e.g. the apparatus having different functions; Driving auxiliary apparatus from engines, not otherwise provided for

Abstract

The invention represents a favourable possibility for the design of a machine with complete balancing of masses. It is an additional application to Patent Application P 3310416. With the aid of two counterweight shafts (20) it is possible completely to balance the first-order inertia forces, the following points having been taken into account: - the axes of the counterweight shafts (20) and of the crankshaft (7) should be parallel; - the distance of the counterweight shafts (20) from the crankshaft (7) should be equal for both counterweight shafts (20); - the centres of gravity of the counterweight shaft (20) and of the piston unit (2) should lie in a common plane perpendicular to the crankshaft axis; - the line connecting the axes of the counterweight shafts at their centre of gravity is perpendicular to the line of motion of the centre of gravity of the piston unit (2); - the two counterweight shafts (20) rotate in opposite directions; - the counterweight shafts (20) and the crankshaft (7) rotate at the same speed. Second- and higher-order effects of mass do not occur due to the use of the so-called Scotch-yoke mechanism. <IMAGE>

Description

BESCHREIBUNG DESCRIPTION

Arbeitsmaschine mit vollständigem Ausgleich der Massenwirkungen Die Erfindung ist eine Zusatzanmeldung zur Patentanmeldung P 33 10 416. Working machine with complete compensation of the mass effects Invention is an additional application to patent application P 33 10 416.

Im folgenden wird die Erfindung beisDielhaft von Zeichnungen näher erläutert. Es zeigen: Fig. 1 bis Fig. 4 die Stellungen der Gegenmassenwellen (20) relativ zur Kurbelwellenstellung, Fig. 5 in Diagrammform die Kraftkomponenten in x-Richtung, Fig. 6 in Diagrammform die KraftkomDonenten in z-Richtung.In the following the invention is illustrated by drawings explained. They show: Fig. 1 to Fig. 4 the positions of the counter-mass shafts (20) relative to the crankshaft position, FIG. 5 in diagram form the force components in x-direction, Fig. 6 in diagram form the force components in the z-direction.

Die Gegenmassenkräfte links Pl und rechts Fr sind gleich groß und entsprechen zusammen der Kolbenmassenkraft Fk. Die Achsen der Gegenmassenwellen (20) und der Kurbelwelle (7) sind parallel. Die Abstände AO und OB sind gleich lang. Die Gegenmassenwellen (20) haben entgegengesetzte Drehrichtungen.The counter-mass forces on the left Pl and on the right Fr are equal and together correspond to the piston mass force Fk. The axes of the counter mass waves (20) and the crankshaft (7) are parallel. The distances AO and OB are the same length. The counter mass shafts (20) have opposite directions of rotation.

Wenn die Kolbeneinheit (2) ihren obersten Punkt erreicht, wirkt eine Kolbenmassenkraft Fk in z-Richtung nach oben, die durch die nach unten gerichteten Kräfte Fl und Fr der linken und rechten Gegenmassenwellen (20) ausgeglichen wird (Fig.When the piston unit (2) reaches its uppermost point, a Piston mass force Fk in the z-direction upwards, which is caused by the downwards-directed Forces Fl and Fr of the left and right counter-mass shafts (20) is balanced (Fig.

1).1).

In der Mittelstellung der Kolbeneinheit (2) ist die Kolbenkraft Fk null, die Kräfte Fl und Fr der Geqenmassenwellen (20) heben sich gegenseitig auf (Fig. 2 und 4).In the middle position of the piston unit (2), the piston force Fk zero, the forces Fl and Fr of the geqenmassewellen (20) cancel each other out (Figures 2 and 4).

Geht die Kolbeneinheit (2) ganz nach unten, wirkt die Kolbenkraft Fk in z-Richtung wieder am stärksten, wie ebenfalls die beiden nach oben gerichteten Kräfte Fl und Fr der Gegenmassenwellen (20) (Fig. 3).When the piston unit (2) goes all the way down, the piston force acts Fk strongest again in the z-direction, as are the two upward-facing ones Forces Fl and Fr of the counter mass waves (20) (Fig. 3).

In x-Richtung treten nur die Kraftkomponenten der Gegenmassenwellen (20) in Sinus-Form in Abhängigkeit vom Kurbelwinkel auf. Diese Kraftkomponenten heben sich gegenseitia auf (Fig.Only the force components of the counter-mass waves occur in the x-direction (20) in sinus form as a function of the crank angle. These force components cancel each other out (Fig.

5).5).

In z-Richtung addieren sich die Kraftkomponenten der Gegenmassenwellen (20) und gleichen die in z-Richtung wirkende Kolbenkraft Fk aus (Fig. 6). Die Größe dieser Kräfte hängt vom Kurbelwinkel ab und ist sinusförmig.The force components of the counter-mass waves add up in the z-direction (20) and compensate for the piston force Fk acting in the z-direction (Fig. 6). The size of these forces depends on the crank angle and is sinusoidal.

- Leerseite -- blank page -

Claims (2)

PATENTANSPRÜCHE Arbeitsmaschine mit vollständigem Ausgleich der Massenwirkungen P7 wirkungen, - bei der die Kolben (1) geradlinig zwischen Arbeitsräumen hin- und hergehen, - deren Kolben (1) direkt, und nicht über die Kurbelwelle (7), miteinander fest oder gelenkig zu einer Kolbeneinheit (2) verbunden sind, - bei der die rotierende Kurbelwelle (7) direkt über ein 2freiheitsgradiges Gelenk mit der hin- und hergehenden Kolbeneinheit (2) verbunden ist und von dieser angetrieben wird, - die als Verbrennungskraftmaschine nach dem 2-Takt-Verfahren pro Maschineneinheit (3) jeweils zwei direkt miteinander verbundene Kolben (1 ) als eine Zweikolben-Einheit aufweist, - die als Verbrennungskraftmaschine nach dem 4-Takt-Verfahren pro Maschineneinheit (3) jeweils vier in H-förmiger bzw. Boxer-Anordnung direkt miteinander verbundene Kolben (1) als eine Vierkolben-Einheit aufweist, - bei der die Maschineneinheiten (3) hinter- und miteinander über eine entsprechend ausgestaltete Kurbelwelle (7) gekoppelt werden können, - bei der die rotierenden Massen durch entsprechende, nach bekannter Massenausgleichsmethode angebrachte Gegenmassen ausgeglichen werden, dadurch gekennzeichnet, daß - die durch die geradlinig oszillierende Bewegung der Kolbeneinheit (2) hervorgerufenen Massenkräfte und -momente zweiter und höherer Ordnung durch die 2freiheitsgradige sog. Kreuzschubkurbel nicht auftreten, - die Massenkräfte erster Ordnung durch Gegenmassenwellen (20) ausgeglichen werden, wobei - die Drehachsen dieser Gegenmassenwellen (20) zueinander und zur Achse der Kurbelwelle (7) parallel sind, - der Achsenabstand der beiden Gegenmassenwellen (20) zur Kurbelwellenachse gleich lang ist, - die Schwerpunkte der Gegenmassenwellen (20) und der Kolbeneinheit (2) in einer Ebene senkrecht zur Kurbelwellenachse liegen, - die Verbindungslinie der Achsen der Gegenmassenwellen in ihrem Schwerpunkt senkrecht zur Bewegungslinie des Schwerpunktes der Kolbeneinheit (2) ist - die beiden Gegenmassenwellen (20) mit der gleichen Drehzahl entgegengesetzt drehen, - die Kolbenmassenkraft 1. Ordnung Fk gleich der Summe der Massenkräfte links Fl und rechts Fr der Gegenmassenwellen (20) d.h. Fk = Fl + Fr ist und es gilt F1 = Fr = Fk/2 und diese Kräfte dem Produkt der Masse mit dem zugehörigen Kurbel- bzw. PATENT CLAIMS Working machine with complete compensation of the effects of masses P7 effects, - in which the pistons (1) straight back and forth between working spaces - their pistons (1) directly, and not via the crankshaft (7), with one another fixed or articulated to form a piston unit (2), - in which the rotating Crankshaft (7) directly via a joint with 2 degrees of freedom with the reciprocating Piston unit (2) is connected and is driven by this, - the internal combustion engine according to the 2-stroke process, two directly with each other per machine unit (3) connected piston (1) as a two-piston unit, - the internal combustion engine according to the 4-stroke process per machine unit (3) four in H-shaped resp. Boxer arrangement, pistons (1) connected directly to one another as a four-piston unit has, - in which the machine units (3) behind and with one another via a appropriately designed crankshaft (7) can be coupled, - in which the rotating masses by means of appropriate mass balancing methods Counterweights are balanced, characterized in that - the straight through the oscillating movement of the piston unit (2) caused inertial forces and moments second and higher order due to the 2 degrees of freedom so-called cross thrust crank appear, - the first-order inertial forces are balanced by counter-mass waves (20), - The axes of rotation of these counter-mass shafts (20) to one another and to the axis of the The crankshaft (7) are parallel, - the distance between the axes of the two counter-mass shafts (20) is the same length as the crankshaft axis, - the centers of gravity of the counter-mass shafts (20) and the piston unit (2) lie in a plane perpendicular to the crankshaft axis, - the line connecting the axes of the counter-mass waves perpendicular to their center of gravity to the line of movement of the center of gravity of the piston unit (2) is - the two counter mass waves Turn (20) in the opposite direction at the same speed, - the piston mass force 1. Order Fk equal to the sum of the inertial forces on the left Fl and on the right Fr of the counter-mass waves (20) i.e. Fk = Fl + Fr and we have F1 = Fr = Fk / 2 and these forces add to the product the mass with the associated crank or Exzenterradius und dem Quadrat der zugehörigen Winkelgeschwindigkeit proportional sind, - die Massenmomente erster Ordnung durch die zuvor genannten Voraussetzungen nicht auftreten bzw. sich gegenseitig aufheben, - sich die Lage des Schwerpunktes der gesamten Arbeitsmaschine während des Betriebs theoretisch nicht verändert. Eccentric radius and the square of the associated angular velocity are proportional, - the mass moments of the first order by the aforementioned Conditions do not arise or mutually cancel each other out - the situation of the center of gravity of the entire work machine during operation, theoretically not changed. 2. Arbeitsmaschine mit vollständigem Ausgleich der Massenwirkungen nach Anspruch 1, dadurch gekennzeichnet, daß der Exzenterradius der Gegenmassenwellen (20) und der Kurbelradius der Kurbelwelle (7) gleich groß sind und die Masse der Gegenmassenwellen (20) halb so groß wie die der Kolbeneinheit (2) ist.2. Working machine with complete compensation of the mass effects according to claim 1, characterized in that the eccentric radius of the counter-mass shafts (20) and the crank radius of the crankshaft (7) are equal and the mass of the Counter mass shafts (20) half as large as that of the piston unit (2).
DE19843417349 1983-03-18 1984-05-08 Machine with complete balancing of the effects of mass Withdrawn DE3417349A1 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
DE19843417349 DE3417349A1 (en) 1983-03-18 1984-05-08 Machine with complete balancing of the effects of mass

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
DE19833310416 DE3310416A1 (en) 1983-03-18 1983-03-18 Machine with complete balancing of the inertia effects
DE19843417349 DE3417349A1 (en) 1983-03-18 1984-05-08 Machine with complete balancing of the effects of mass

Publications (1)

Publication Number Publication Date
DE3417349A1 true DE3417349A1 (en) 1985-11-14

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Family Applications (1)

Application Number Title Priority Date Filing Date
DE19843417349 Withdrawn DE3417349A1 (en) 1983-03-18 1984-05-08 Machine with complete balancing of the effects of mass

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Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7191742B2 (en) * 2005-01-11 2007-03-20 Schrick, Inc. Diesel aircraft engine
WO2009089596A1 (en) * 2008-01-18 2009-07-23 Raffaele, Michael, John Scotch yoke engine or pump
US9181868B2 (en) 2011-10-12 2015-11-10 Engineered Propulsion Systems, Inc. Aerodiesel engine
US11428157B2 (en) 2017-07-21 2022-08-30 General Atomics Aeronautical Systems, Inc. Enhanced aero diesel engine
US11473520B2 (en) 2011-10-05 2022-10-18 General Atomics Aeronautical Systems, Inc. Aero compression combustion drive assembly control system

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7191742B2 (en) * 2005-01-11 2007-03-20 Schrick, Inc. Diesel aircraft engine
US7373905B2 (en) 2005-01-11 2008-05-20 Schrick, Inc. Diesel aircraft engine
US8453611B2 (en) 2005-01-11 2013-06-04 Schrick, Inc. Diesel aircraft engine
WO2009089596A1 (en) * 2008-01-18 2009-07-23 Raffaele, Michael, John Scotch yoke engine or pump
US11473520B2 (en) 2011-10-05 2022-10-18 General Atomics Aeronautical Systems, Inc. Aero compression combustion drive assembly control system
US9181868B2 (en) 2011-10-12 2015-11-10 Engineered Propulsion Systems, Inc. Aerodiesel engine
US9447729B2 (en) 2011-10-12 2016-09-20 Engineered Propulsion Systems, Inc. Aerodiesel engine
US11428157B2 (en) 2017-07-21 2022-08-30 General Atomics Aeronautical Systems, Inc. Enhanced aero diesel engine

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