The present invention concerns a laser spark plug having the features of the classifying portion of claim 1, an internal combustion engine having such a laser spark plug and a method of ascertaining the operating condition of such a laser spark plug.
In laser ignition systems based on laser spark plugs of the general kind set forth the ignition sparks are produced by focusing an intensive laser light pulse which lasts for only a few nanoseconds on the ignition location in the combustion chamber of the internal combustion engine. The laser light can be produced for example by means of a pump laser and an ignition laser (for example a laser crystal) connected downstream of the pump laser. A semiconductor laser which emits light over a plurality of milliseconds and which charges up the ignition laser is used as the pump laser. The ignition laser then delivers a laser light pulse which is in the order of nanoseconds in length and which is introduced into the combustion chamber of the internal combustion engine by way of the combustion chamber window.
Production of the laser light can suffer degradation over the operating time of the internal combustion engine and the combustion chamber window through which the laser light pulse is introduced into the combustion chamber can suffer from transmission losses due to deposits at the surface towards the combustion chamber.
In total that can result in a considerable weakening in the ignition spark or (as a consequence) worsening of combustion in the internal combustion engine.
DE 10 2009 000 911 A1 discloses an ignition spark plug having at least one optical sensor which is integrated into the laser spark plug and which serves to monitor the energy content of the pump radiation for the laser crystal. However that specification does not show detection of the ignition energy or light intensity which is actually of interest, being produced by the ignition laser or the laser crystal which is integrated into the laser spark plug. JP 2012-189044 A shows that a part of the light delivered by an ignition laser in the direction of the pump laser feeding the ignition laser is detected. In that case, that light from the ignition laser, that is delivered by the ignition laser in a direction away from the combustion chamber, is detected. That detection also cannot provide any information as to how high the level of light intensity of the laser light is, which is delivered in the direction of the combustion chamber, in order there to trigger an ignition spark.
The object of the invention is to provide a laser spark plug of the general kind set forth, an internal combustion engine and a method of ascertaining the operating condition of such a laser spark plug, which makes it possible to implement condition monitoring in respect of the energy content of the ignition energy coming from the ignition spark plug.
That object is attained by an ignition spark plug having the features of claim 1, an internal combustion engine having such a laser spark plug and a method having the features of claim 9.
Advantageous embodiments of the invention are defined in the appendant claims.
By virtue of the mirror deflection of a part of a laser light pulse at the mirrored or partially mirrored reflection surface of the combustion chamber optical means on to the laser light sensor which for example can be in the form of a photodiode, it is possible to detect or sense the light intensity of the laser light pulses issuing from the laser crystal. While, in the case of laser spark plugs known in the state of the art, the radiation of a pump laser feeding the laser crystal is detected, it is possible with the proposed solution to detect the light intensity, which is actually of interest, of the laser light pulses of the laser crystal.
It is preferably provided in that respect that the combustion chamber optical means includes a convergent lens, wherein the convergent lens is provided with the reflection surface, preferably in the edge region of the convergent lens. The location of the mirrored reflection surface at the usually curved surface of the convergent lens can in that case preferably be so selected that the beam path of the part of a laser light pulse, that is reflected at that mirroring, leads to the laser light sensor provided for detection of that reflected laser light.
To reduce the influence of troublesome ambient light or stray light during detection of the reflected laser light it can preferably be provided that an optical aperture is connected upstream of the laser light sensor in the direction of the beam path of the laser light incident in the laser light sensor. A specifically targeted orientation of the laser light beam on to the mirrored reflection surface and the provision of an optical aperture can thus ensure that the laser light sensor detects substantially exclusively the reflected laser light.
Generally it can be provided that the ignition energy is afforded by the laser crystal of the laser spark plug, wherein the radiation of a pump laser is coupled into the laser crystal, wherein for adjustment of the ignition energy the pump output and/or the pump duration of the pump laser is or are adjusted, preferably by adjusting the current strength of a pump current feeding the pump laser.
In that case adjustment of the current strength of the pump current can be effected for example in such a way that, starting from a stored or predeterminable cylinder-specific optimum current strength, the current strength is slightly altered downwardly and upwardly and the maximum laser light power or the maximum laser light intensity detected by the laser light sensor is ascertained in dependence on the current strength. That value can then be stored in a storage means as a new value for the optimum current strength.
In a particularly preferred variant it can be provided that integrated in the laser spark plug is an additional optical stray light sensor by which at least a part of a stray light which is scattered back during the duration of a laser light pulse by the combustion chamber optical means can be detected. In particular it can be provided in that case that the combustion chamber optical means includes a combustion chamber window with a coupling-in surface which delimits the combustion chamber, wherein at least a part of the stray light scattered back by the coupling-in surface can be detected by the stray light sensor. In that arrangement the additional stray light sensor can preferably be so arranged that it precisely does not sense or detect the laser light reflected at the mirrored reflection surface, but a part of the scatter light which comes from reflections at various regions of the beam path of the laser light pulses. As the stray light which is in the interior of the laser spark plug comes in particular from laser light pulses which are scattered back at the coupling-in surface of the combustion chamber window, it is thus possible to detect in particular that stray light which is scattered back from the coupling-in surface.
In the case of a clean combustion chamber window (without deposits) no or almost no radiation should be scattered back into the laser spark plug. The integration of an additional optical stray light sensor into the laser spark plug, by way of which back-scattered radiation can be detected, therefore makes it possible in principle to ascertain the deposit-induced transmission losses at the combustion chamber window by measurement of the radiation which is scattered back in respect of the laser light pulse at the coupling-in surface. As the transmission losses occurring in the case of a clean new combustion chamber window are known (for example by previous calibration, also when the machine is stopped), it is thus possible to conclude that there is a deterioration.
The deposits at the combustion chamber side of the coupling-in surface depend in particular on the conditions of use and the time of use of the laser spark plug. If there is provided an evaluation unit, wherein light intensities of the laser light detectable by the laser light sensor and the stray light detectable by the stray light sensor can be compared by the evaluation unit and a difference value in respect of the light intensities of detected laser light and detected stray light can be outputted by the evaluation unit it is thus possible to conclude the degree of fouling of the combustion chamber window by forming the difference in respect of the measurement signals of the two optical sensors.
It is possible in that way in particular to initiate suitable measures for ensuring proper engine operation. For example the pump output and the pump duration of a pump laser feeding the laser crystal can be suitably adapted. It is however also possible to initiate cleaning procedures or a need for maintenance can be displayed in good time.
Preferably it can therefore be provided that in dependence on the comparison of detected laser light with detected stray light, it is possible to arrive at a conclusion about transmittance of the combustion chamber optical means, preferably the combustion chamber window of the combustion chamber optical means, and the ignition energy can be adjusted in dependence on the transmittance of the combustion chamber optical means or the combustion chamber window respectively.
It is also possible to provide a further optical sensor which is integrated into the laser spark plug and which has a frequency sensitivity which is different relative to the laser light sensor and/or stray light sensor. For example it can be provided that the laser light sensor and/or the stray light sensor is matched to the wavelength of the laser light pulses passing into the combustion chamber and the further optical sensor is matched to the main emission spectrum of the combustion light.
That differing frequency sensitivity of the further optical sensor relative to the laser light sensor or the stray light sensor respectively and/or the differing time of detection of the radiation by the respective sensors can be used to distinguish between an ignition event in the combustion chamber and subsequent combustion.
In addition, by quantifying the transmittance or the transmission losses on the basis of the deposits at the combustion chamber window it is also possible to correct the measurement values detected by the further optical sensor for the light intensity from the combustion chamber.
The optical sensors (laser light sensor, stray light sensor, further optical sensor) are preferably arranged in a region of the ignition spark plug between the combustion chamber optical means and the laser crystal. For thermal and optical reasons, it is advantageous for them to be positioned at the housing wall at the maximum spacing relative to the combustion chamber optical means or the combustion chamber window thereof.
It is possible with the invention to implement various control strategies:
Generally it can also be provided in each case that the optical sensor or sensors is or are not themselves placed at the specified positions, but that a respective light guide member is connected upstream of the sensor or sensors and the inlet of the light guide is placed at the described positions. In that way the sensors themselves can be placed independently of the position for detection of the radiation.
Preferably photodiodes are used as the optical sensors. The internal combustion engine is preferably in the form of an—in particular stationary—gas engine (gas Otto-cycle engine).
Further advantages and details of the invention will be apparent from the Figures and the related description. In the Figures:
An optical stray light sensor 12 additionally integrated in the laser spark plug 1 detects a stray light 13 formed by back-scattering of the laser light pulses 5 at the combustion chamber optical means 4. As a large part of that stray light 13 is formed by back-scattering of the laser light pules 5 at the coupling-in surface 15 of the combustion chamber window 14, which surface is fouled at the combustion chamber side by deposits, that stray light sensor 12 serves primarily to detect the stray light 13 which is scattered back from that coupling-in surface 15.
The light intensities of the reflected laser light 9 and the stray light 13 respectively, that are detected by the laser light sensor 7 and the stray light sensor 12, are outputted in the form of optical or corresponding electrical signals to an evaluation unit 16 which compares those light intensities and performs an operation for forming the difference between those measurement signals. As a further consequence, in dependence on the difference in the detected light intensities, it is then possible to conclude about the fouling or the transmittance of the combustion chamber window 14 and the ignition energy can be suitably adjusted in dependence on the transmittance of the combustion chamber window. That can be effected by the current strength of a pump current 19 feeding the pump laser 18 (for example a VCSEL pump laser) being suitably adjusted to appropriately alter the pump output and/or the pump duration of the pump laser 18.
Number | Date | Country | Kind |
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A1131/2012 | Oct 2012 | AT | national |