EP1561029B2 - Procede et dispositif pour mesurer le debit d'injection d'un injecteur de liquides - Google Patents

Procede et dispositif pour mesurer le debit d'injection d'un injecteur de liquides Download PDF

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Publication number
EP1561029B2
EP1561029B2 EP03809686A EP03809686A EP1561029B2 EP 1561029 B2 EP1561029 B2 EP 1561029B2 EP 03809686 A EP03809686 A EP 03809686A EP 03809686 A EP03809686 A EP 03809686A EP 1561029 B2 EP1561029 B2 EP 1561029B2
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EP
European Patent Office
Prior art keywords
pressure
injection
measurement
measurement volume
volume
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.)
Expired - Lifetime
Application number
EP03809686A
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German (de)
English (en)
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EP1561029B1 (fr
EP1561029A1 (fr
Inventor
Ulrich Kuhn
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Robert Bosch GmbH
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Robert Bosch GmbH
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Application filed by Robert Bosch GmbH filed Critical Robert Bosch GmbH
Publication of EP1561029A1 publication Critical patent/EP1561029A1/fr
Publication of EP1561029B1 publication Critical patent/EP1561029B1/fr
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Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F02COMBUSTION ENGINES; HOT-GAS OR COMBUSTION-PRODUCT ENGINE PLANTS
    • F02MSUPPLYING COMBUSTION ENGINES IN GENERAL WITH COMBUSTIBLE MIXTURES OR CONSTITUENTS THEREOF
    • F02M65/00Testing fuel-injection apparatus, e.g. testing injection timing ; Cleaning of fuel-injection apparatus
    • F02M65/001Measuring fuel delivery of a fuel injector
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F02COMBUSTION ENGINES; HOT-GAS OR COMBUSTION-PRODUCT ENGINE PLANTS
    • F02MSUPPLYING COMBUSTION ENGINES IN GENERAL WITH COMBUSTIBLE MIXTURES OR CONSTITUENTS THEREOF
    • F02M65/00Testing fuel-injection apparatus, e.g. testing injection timing ; Cleaning of fuel-injection apparatus
    • F02M65/005Measuring or detecting injection-valve lift, e.g. to determine injection timing

Definitions

  • the injected fuel causes pressure oscillations in the corresponding natural frequencies of the measuring volume, these natural frequencies depending on the geometric dimensions of the measuring volume.
  • many harmonics are usually excited, with several vibration modes are usually possible. This makes it difficult to filter the pressure sensor measuring signal, since the frequencies of the natural oscillations are partly in the range of the frequencies of the measuring signal.
  • the density depends on the temperature of the test medium. To take this into account, the temperature will be Measured in the measuring volume by means of a temperature sensor and the density corrected accordingly. The temperature measurement is selective and does not take into account a possibly unequal temperature in the entire measuring volume. Such a method is described in WO 02/064970 A described.
  • the device according to the invention with the features of claim 1 has the advantage that can be determined from the pressure curve in a simple manner, the injection quantity.
  • the time course of the pressure in the measuring volume is recorded during the injection and from this the time course of the injection quantity is calculated.
  • the sound velocity is determined. From the increase in pressure and the speed of sound can then directly the injection quantity or its time course, so calculate the rate of injection rate.
  • the speed of sound is determined by means of a separate measurement process, in which a sound pulse is emitted by a sound generator into the measurement volume and is collected by the pressure sensor. If the sound generator and the pressure sensor are arranged opposite each other, the sound velocity can be calculated directly from the distance and the running time. This is a very fast measuring method, which causes hardly any significant delays in the measurement process.
  • the measurement data of the pressure curve are stored with the aid of an electronic computer, which also makes a direct further processing of the data possible.
  • the frequency of a natural pressure oscillation of the measuring volume is determined from the pressure measured values. From the natural frequency, the sound velocity then results as an average value over the entire measurement volume, without the need for a separate measurement with corresponding devices.
  • the filtering of the pressure measured values is carried out, for example, with a low-pass filter, so that disturbances and noise are largely eliminated. From the time differentiation of the pressure signal can then determine the injection rate.
  • the device according to the invention with the features of claim 1 has the advantage over the prior art that the measurement signal can be better filtered.
  • the pressure sensor is arranged in the pressure node of the first compressive natural vibration, that is, the natural vibration, so that the pressure sensor does not detect a signal of the natural vibration. Therefore, the cut-off frequency of the low-pass filter can be shifted upwards by a factor of two for smoothing the pressure measurement values.
  • FIG. 1 the measuring device is shown in a partially sectioned view.
  • a cylindrical measuring volume 1 with a wall 2 is completely filled with a test liquid, wherein the measuring volume 1 is completed on all sides.
  • the wall 2 has a first base area 102 and a second base area 202, which are connected by the side wall 303, which has a longitudinal axis 4.
  • an injection valve 3 projects with its tip into the measuring volume 1, wherein the passage of the injection valve 3 is closed by the wall 2 liquid-tight.
  • the injection valve 3 has a valve body 7, in which in a bore 6, a piston-shaped valve needle 5 is arranged longitudinally displaceable.
  • test liquid flows from a pressure space 9 formed between the valve needle 5 and the wall of the bore 6 to the injection openings 12 and is injected from there into the measuring volume 1 until the injection openings 12 pass through the valve needle 5 are closed again.
  • the injection of the test liquid takes place here with a high pressure, which can be up to 200 MPa depending on the injection valve used.
  • a pressure holding valve 17 line 16 In the side wall 303 of the cylindrical wall 2 opens a connected to a pressure holding valve 17 line 16, can be derived by the test liquid from the measuring volume 1 in a not shown in the drawing leakage volume.
  • a control valve 15 is also arranged, through which the line 16 can be closed if necessary, if a derivation of test liquid from the measuring volume 1 is not desired.
  • the pressure-maintaining valve 17 ensures that a certain pressure in the measuring volume 1 is maintained and this always remains completely filled with liquid.
  • a holder 22 projects through the second base 202 of the wall 2 into the measuring volume 1.
  • a pressure sensor 20 is arranged, which is connected via a signal line 24, which leads out of the measuring volume 1 in the holder 22 with an electronic computer 28, wherein the passage of the holder 22 is sealed by the wall 2 liquid-tight.
  • the pressure sensor 20 is arranged in the median plane between the two base surfaces 102, 202 of the wall 2 and thus has the same distance to both base surfaces 102, 202. Since the pressure sensor 20 is also located on the longitudinal axis 4, it has to the side surface 303 on all sides the same distance s.
  • the signal that the pressure sensor 20 supplies read and stored electronically.
  • the pressure sensor 20 is constructed, for example, on a piezo-based basis, so that even rapid changes in pressure can be measured without appreciable delay.
  • a sounder 21 is arranged, which has the distance s from the pressure sensor 20.
  • a separate sound receiver 30 diametrically opposite the sounder 21 on the side surface 303 in order to obtain the largest possible distance of the sound signal and thus greater accuracy in determining the speed of sound c.
  • the time course of the pressure is measured, from which in turn the injection rate r (t) can be determined, ie the amount dm (t) of the test fluid injected per unit time dt.
  • the pressure in the measuring volume 1 increases. Liquids are virtually incompressible compared to gases, so that even a small increase in volume leads to a well-measurable pressure increase. Due to the impact-like introduction of the test liquid, pressure oscillations are excited in the measuring volume 1.
  • the natural frequencies depend on the geometric dimensions of the measurement volume 1:
  • FIG. 2 shows this first natural compressive vibration schematically, wherein the lines designated p show the pressure curve, in which at the edges bellies are to be found and in the middle, ie in the radial plane of the cylindrical measuring volume in which the pressure sensor 20 is disposed, a pressure node.
  • the pressure sensor 20 does not register the first natural pressure vibration since no pressure changes occur at the pressure node. Nor are the 2nd, 4th and all other even harmonics recorded by the pressure sensor 20.
  • the procedure is as follows: Into the measuring volume 1, in which the test liquid is located, the injection valve 3 injects a certain amount of liquid by a rapid longitudinal movement of the valve needle 5, through which the injection openings 12 are opened and closed again.
  • the pressure sensor 20 measures the pressure p (t) which is read out and stored by the computer 28 at a specific rate of, for example, 100 kHz.
  • equation (III) is used.
  • the measured values p (t) stored in the computer are time-differentiated and multiplied by the factor V / c 2 , which directly yields the injection rate r (t).
  • the cut-off frequency ⁇ G for the low-pass filter can be selected to be twice as large as the first fundamental vibration is not registered by the pressure sensor 20.
  • the smoothed pressure readings are then differentiated in time, and after multiplication by the factor V / c 2 results in a known volume V, the injection rate r (t).
  • the speed of sound c can also be determined in a separate method.
  • FIG. 3 shows the time course of pressure p (t) and its derivative dp (t) / dt as a function of time t in arbitrary units U.
  • an injector as used for direct-injection, auto-ignition internal combustion engines, this corresponds to a fuel injection, which is divided into a pilot or pilot injection and a subsequent main injection.
  • the derivative dp (t) / dt gives a value which is proportional to the injection rate r (t).
  • V / c 2 By multiplication by the factor V / c 2 , one finally obtains from this the absolute value of the injection rate r (t).
  • the measurement method together with the described measurement setup thus makes it possible to measure the pressure profile and to determine the speed of sound c under the current test conditions, from which the injection quantity and the injection rate can be determined. If the speed of sound c is calculated from the frequency of the natural vibrations, then all the necessary variables from the pressure curve can be determined, which excludes errors due to additional components. Due to the arrangement of the pressure sensor 20 exactly between the two base areas 102, 202, the cut-off frequency ⁇ G of the low-pass filter can be raised to twice the frequency of the fundamental vibration ⁇ e , without a qualitative impairment is to be expected by the filtering. Elaborate calibration procedures, in which the speed of sound is determined in a separate measurement method, can thus be dispensed with.
  • the test fluid may be fuel or another fluid whose properties are similar to that used in normal use of the fuel injector.
  • the measurement volume 1 need not be cylindrical, but instead of a cylinder, a cuboid measuring volume 1 or another suitable shape may be provided, for example a ball.
  • the pressure sensor 20 is also arranged here in a pressure node of the first natural pressure vibration of the measuring volume 1 in order to set the cutoff frequency for the filtering as high as possible.

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  • Engineering & Computer Science (AREA)
  • Chemical & Material Sciences (AREA)
  • Combustion & Propulsion (AREA)
  • Mechanical Engineering (AREA)
  • General Engineering & Computer Science (AREA)
  • Measuring Volume Flow (AREA)
  • Measuring Fluid Pressure (AREA)
  • Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)
  • Feeding, Discharge, Calcimining, Fusing, And Gas-Generation Devices (AREA)

Claims (6)

  1. Dispositif pour mesurer le débit d'injection (r(t)) d'un injecteur (3) de liquides avec un volume de mesure (1) scellé de tous côtés et rempli avec un liquide d'essai, une ouverture (10) dans la paroi (2) du volume de mesure (1) pour recevoir un injecteur (3), de sorte que l'injecteur (3) en position d'installation pénètre avec au moins une ouverture d'injection (12) dans le volume de mesure (1), et avec un capteur de pression (20) dans le volume de mesure (1), caractérisé en ce que
    le capteur de pression (20) est placé dans le noeud de pression de la première oscillation de pression propre du volume de mesure (1), et la vitesse du son peut être déterminée par mesure du temps de propagation d'un signal sonore dans le volume de mesure (1), ou directement à partir des valeurs de mesure de pression.
  2. Dispositif selon la revendication 1, caractérisé en ce que le volume de mesure (1) a une forme cylindrique.
  3. Dispositif selon la revendication 2, caractérisé en ce que le capteur de pression (20) est dans le plan radial à mi-chemin entre les deux surfaces de base (102; 202) du cylindre.
  4. Dispositif selon la revendication 1, caractérisé en ce qu'un ordinateur (28) enregistre et mémorise les valeurs de mesure du capteur de pression (20).
  5. Dispositif selon la revendication 4, caractérisé en ce que l'ordinateur (28) exécute un programme de calcul des fréquences fondamentales du volume de mesure (V) à partir des valeurs de mesure de pression enregistrées (p(t)).
  6. Dispositif selon la revendication 1, caractérisé par une source sonore (21) et un capteur de son (30) dans le volume de mesure (V).
EP03809686A 2002-10-25 2003-06-04 Procede et dispositif pour mesurer le debit d'injection d'un injecteur de liquides Expired - Lifetime EP1561029B2 (fr)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
DE10249754A DE10249754A1 (de) 2002-10-25 2002-10-25 Verfahren und Vorrichtung zur Messung der Einspritzrate eines Einspritzventils für Flüssigkeiten
DE10249754 2002-10-25
PCT/DE2003/001852 WO2004040129A1 (fr) 2002-10-25 2003-06-04 Procede et dispositif pour mesurer le debit d'injection d'un injecteur de liquides

Publications (3)

Publication Number Publication Date
EP1561029A1 EP1561029A1 (fr) 2005-08-10
EP1561029B1 EP1561029B1 (fr) 2006-08-23
EP1561029B2 true EP1561029B2 (fr) 2011-07-06

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ID=32087191

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EP03809686A Expired - Lifetime EP1561029B2 (fr) 2002-10-25 2003-06-04 Procede et dispositif pour mesurer le debit d'injection d'un injecteur de liquides

Country Status (6)

Country Link
US (1) US7171847B2 (fr)
EP (1) EP1561029B2 (fr)
JP (1) JP4130823B2 (fr)
AT (1) ATE337484T1 (fr)
DE (2) DE10249754A1 (fr)
WO (1) WO2004040129A1 (fr)

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DE102007032745A1 (de) 2007-07-13 2009-01-15 Robert Bosch Gmbh Erfassung des Totaldrucks in Gasmassenströmen von Verbrennungsmotoren
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Also Published As

Publication number Publication date
US20060156801A1 (en) 2006-07-20
EP1561029B1 (fr) 2006-08-23
WO2004040129A1 (fr) 2004-05-13
JP4130823B2 (ja) 2008-08-06
DE10249754A1 (de) 2004-05-06
DE50304788D1 (de) 2006-10-05
US7171847B2 (en) 2007-02-06
ATE337484T1 (de) 2006-09-15
EP1561029A1 (fr) 2005-08-10
JP2006504038A (ja) 2006-02-02

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