Gas turbine engines for aircraft typically include an ignition system to aid in the starting of the engine. The engine ignition system may include an ignition exciter that stores energy and releases a high-energy spark to produce combustion of fuel in the engine in a way that is analogous to automobile ignition coils. The ignition exciter may provide sparks during initial engine start on the ground or, depending upon the environmental conditions, while the aircraft is airborne to prevent combustion from failing.
In one aspect, an embodiment of the invention relates to a method for controlling the operation of an ignition exciter comprising a rechargeable energy source supplying electricity to a solid-state switch. The method includes charging the energy source at a first rate when the voltage of the energy source is less than a first voltage reference value, charging the energy source at a second rate, greater than the first rate, when the voltage of energy source is greater than a first voltage reference value, and discharging the energy source through the switch to generate a spark when the voltage of the energy source satisfies a discharge voltage reference value.
In the drawings:
Surrounded by an annular fan casing 38, the fan section 14 includes a rotatable, axial-flow fan rotor 36. The fan casing 38 is supported about the core engine section 12 by a plurality of substantially radially-extending, circumferentially-spaced support struts 40. The fan casing 38 is supported by radially extending outlet guide vanes 42 and encloses the fan rotor 36 and a plurality of fan rotor blades 44. A downstream section 39 of the fan casing 38 extends over an outer portion of the core engine 12 to define a secondary, or bypass, airflow conduit 46 that provides additional propulsive jet thrust.
The EMI filter module 108 includes an EMI filter 118 and a smoothing capacitor 119 configured to prevent high frequency noise generated by the ignition exciter circuit 102 from leaking through the DC power input and to protect the power converter 110 from transient voltage surges present on the DC source 117. The power converter 110 may comprise a flyback type converter and is configured to step up an input voltage received from the EMI filter module 108 to an optimal level for energy storage. The power converter 110 utilizes a charge pump technique to build up the voltage at the rechargeable energy source 112 over a number of charge cycles. When the charge cycles have built the voltage at the rechargeable energy source 112 to a predetermined level, the charge pumping is interrupted, and the rechargeable energy source 112 is controlled to discharge. Alternatively, the power converter 110 is a DC-DC converter other than a flyback type converter.
The rechargeable energy source 112 is configured to store energy between sparking events. A voltage monitoring circuit and discharge switch module 114 is configured to release the energy stored in the rechargeable energy source 112. The PFN 116 is configured to optimize the shape and timing of the stored energy waveform for creating the spark at a firing tip 120 of the igniter plug 106. The PFN 116 may be an inductor but may also include a transformer and/or a high frequency capacitor to facilitate a higher output voltage or a longer duration for the resulting spark.
The ignition lead 104 transmits an output of the ignition exciter circuit 102 to the igniter plug 106. The igniter plug 106 conducts the energy from the ignition lead 104 to the firing tip 120 residing within the engine combustor 24 (shown in
The power converter 110 includes a transformer 122 and a power switch 124 electrically coupled to a primary winding 126 of the transformer 122. The power converter 110 also includes a first switch driver 128 electrically coupled to the power switch 124. A converter clock 130 and a discharge feedback circuit 132 are electrically coupled to the switch driver 128. A current sensor 134 is electrically coupled to the power switch 124 and a mode select power level voltage comparator 136.
The voltage monitoring circuit and discharge switch module 114 includes a second switch driver 138 electrically coupled to a discharge switch 140, a voltage comparator 142, a rectifier and a trigger capacitor module 144. The second switch driver is coupled to the discharge feedback circuit 132 in the power converter 110.
The rechargeable energy source 112 may include one or more energy storage or “tank” capacitors 210, 212, 214. The rechargeable energy source 112 may also include an array of storage capacitors 210, 212, 214 that may be coupled in parallel or in series. In this way, the voltage across the rechargeable energy source 112 includes the additive combination of the voltage across the array of in-series capacitors 210, 212, 214. Alternatively, the capacitors may be combined in parallel to implement a rechargeable energy source where the overall capacitance is the additive combination of the capacitance of the array of capacitors.
The clamper circuit 220 includes a freewheeling diode 222. Often coupled in parallel with a resistor (not shown), the freewheeling diode 222 eliminates sudden voltage spikes across an inductive load when a supply voltage from the rechargeable energy source 112 is suddenly reduced or removed, and provides an efficient energy delivery path once energy is switched from the rechargeable energy source 112, through the discharge switch 140 and into the circulating path formed by the PFN 116, the ignition lead 104 and igniter plug 106, and back through the freewheeling diode 222 as part of the timed energy release to facilitate optimal ignition.
The discharge switch 140 is a solid-state switch that may comprise one or more thyristors 218 connected in series, each having a high standoff voltage and pulse current capacity. Preferably, the solid-state switch 140 includes a single thyristor 218 but multiple solid-state switches may be implemented depending upon the required voltage of the ignition exciter circuit 102 and the rated voltage for the switches. Each thyristor 218 is inductively fired by way of a pulse transformer 216. Alternatively, the solid-state switch may include one or more insulated-gate bipolar transistor (IGBT) or metal oxide semiconductor field-effect transistor (MOSFET) devices.
The one or more thyristors 218 are inductively switched when the voltage in the storage capacitors 112 reaches a predetermined level for energy storage. When the voltage at the rechargeable energy source 112 reaches a predetermined voltage level (e.g., 2500 volts), the solid-state discharge switch 140 is closed so as to transfer the energy stored in the rechargeable energy source 112 to the output PFN.
Energy requirements of the engine ignition system 100 are specified to ensure sufficient energy delivery at the igniter firing tip 120 for a range of starting scenarios. Ignition exciters may endure temperature extremes ranging from −55° C. to 150° C. Exposure to high temperatures (e.g. above 121° C.) may limit the use of silicon semiconductor components (such as the one or more thyristors 218) for power switching and conversion because of excessive leakage current. That is, leakage current, or current that passes through a solid-state switch when it is ideally non-conductive (i.e. switched “off”), increases in solid-state switches as a function of temperature. In semiconductor devices like solid-state switches, leakage current is a quantum phenomenon where mobile charge carriers (electrons or holes) tunnel through an insulating region in the semiconductor. The phenomenon increases with temperature. While small levels of leakage current allow a solid-state switch to be considered as non-conductive, excessive leakage current running through the solid-state device renders the device deficient or inoperable as a switch. The leakage current must stay below a level that causes the solid-state device to overheat. The relationship between the leakage current and the junction temperature of the solid-state device is estimated by the following equation:
Ti=Ta+(VdIdθjc)
where Ti is the junction temperature of the solid-state device, Ta is the ambient temperature, the product of Vd and Id is the power dissipation (i.e. the voltage and leakage current) and Θjc is the thermal resistance from the junction to the case of the solid-state device. Based on this relationship, for silicon semiconductors which typically have a thermal resistance of about 0.25 K/W, when the leakage current increases by about a factor of 10 between 100° C. and 121° C., the solid-state device experiences a significant increase in junction temperature. Therefore, for silicon semiconductors, the level of leakage current becomes excessive at about 121° C. and above.
Upon charging the rechargeable energy source 112 at a first rate, the voltage level 330 in the rechargeable energy source 112 satisfies a predetermined leakage threshold that is indicative of a leakage current through the solid-state switch that is excessive (i.e. the switch does not sufficiently turn off when in the non-conducting state). The predetermined threshold may include, but not be limited to one or more of a voltage level, a current level, a time duration, a temperature, a power level. A measurement of one or more of the threshold criteria may include a sensing of the relevant phenomenology on one or more of the above described ignition exciter elements, including but not limited to the rechargeable energy source 112, the transformer 122, the discharge switch 140, etc. The term “satisfies” the threshold is used herein to mean that the variation comparison satisfies the predetermined threshold, such as being equal to, less than, or greater than the threshold value. It will be understood that such a determination may easily be altered to be satisfied by a positive/negative comparison or a true/false comparison. For example, a less than threshold value can easily be satisfied by applying a greater than test when the data is numerically inverted. It is also contemplated that the received data may include multiple sensor outputs and that comparisons may be made between the multiple sensor outputs and corresponding multiple reference values.
Upon satisfying the predetermined threshold, the voltage level 324 in the rechargeable energy source 112 charges at a second rate for the duration of time ranging from 314 to 316. As shown in the figure, the first rate that the voltage level 322 in the rechargeable energy source 112 charges is less than the second rate that the voltage level 324 in the rechargeable energy source 112 charges. Finally, the voltage level 326 in the rechargeable energy source 112 rapidly discharges following the completion of the second rate of charging for the short duration of time ranging from 316 to 318. The dual mode charging operation then repeats at a predetermined spark rate.
As shown in
To charge the rechargeable energy source 112 according to the first charging mode described above, the power converter 110 may deliver power by sensing the voltage level of the rechargeable energy source 112 and setting the charging rate based on the sensed voltage level. For example, the energy storage voltage comparator 142 may directly monitor the voltage level of the rechargeable energy source 112 and initiate the mode select power level voltage comparator 136 to charge the rechargeable energy source 112 to a predetermined voltage level. Alternatively, instead of sensing the voltage level and establishing a predetermined voltage charge rate, the power converter 110 may deliver power over a timed sequence. That is, for a set voltage level and charge rate, the power converter 110 may deliver power for a set time duration. The mode select power level voltage comparator 136 may initiate a predetermined duration that is indicative of the voltage limit of the rechargeable energy source 112 that is below the level where excessive leakage current occurs within the discharge switch 140.
Subsequent to the first charging mode sequence, during the second mode, the power converter 110 delivers power to quickly complete the charging of the rechargeable energy source 112 before extensive heat is dissipated within the discharge switch 140. The increase in power conversion is necessary to maintain the spark rate during higher temperature operation. Consequently, the second charging period may be minimized in time by maximizing the second charging rate for optimal switching performance. That is, to maintain a spark rate (i.e. one spark per the duration of time ranging from 312 to 318) as per the requirements of a particular gas turbine engine, the duration of time ranging from 312 to 316 is the total available charge time. The maximum rate at which the voltage level of the rechargeable energy source 112 may be charged is limited by the physical and electrical characteristics of the ignition exciter circuit elements including the rechargeable energy source 112 and the transformer 122. By charging rechargeable energy source 112 to the voltage level 324 during the second charging rate for the time ranging from 314 to 316 at the maximum charging rate, the duration of time from 314 to 316 is minimized. By charging the rechargeable energy source 112 at the maximum charging rate once the rechargeable energy source is charged to the voltage level 330 where the leakage current through the solid-state switch is excessive until the time 316 where the spark is generated, the remaining duration of time ranging from 312 to 314 is the maximum duration of time to charge the rechargeable energy source 112 at the slowest charging rate. Therefore, the duration of time from 312 to 314 is maximized and consequently, the first charging rate for the time duration of time from 314 to 316 is minimized. Durations of time to buffer the voltage level may be added prior to the initiation of the first charging at time 312 or at any time during the first charging duration ranging from 312 to 314 to maintain a desired spark rate.
Increasing the reference voltage of the mode select power level voltage comparator 136 that monitors the current mode control enable the increased conversion of energy from the power converter 110 to the rechargeable energy source 112 for the second charging mode. The increase in reference voltage allows additional current (and power) to be generated during each flyback cycle (i.e. charging and discharging stages of the transformer 122) before the mode select power level voltage comparator 136 triggers the main power switch 124 off, thus transferring the power to the rechargeable energy source 112.
The technical effect is to maintain the spark rate during higher temperature operation where the leakage current of the solid-state switch increases with temperature. Consequently, solid-state switches may be used for ignition exciters designed for ignition systems with high spark energy requirements. As such, solid-state discharge switches may be used in ignition systems of large aircraft.
To the extent not already described, the different features and structures of the various embodiments may be used in combination with each other as desired. That one feature may not be illustrated in all of the embodiments is not meant to be construed that it may not be, but is done for brevity of description. Thus, the various features of the different embodiments may be mixed and matched as desired to form new embodiments, whether or not the new embodiments are expressly described. All combinations or permutations of features described herein are covered by this disclosure.
This written description uses examples to disclose the invention, including the best mode, and also to enable any person skilled in the art to practice the invention, including making and using any devices or systems and performing any incorporated methods. The patentable scope of the invention is defined by the claims, and may include other examples that occur to those skilled in the art. Such other examples are intended to be within the scope of the claims if they have structural elements that do not differ from the literal language of the claims, or if they include equivalent structural elements with insubstantial differences from the literal languages of the claims.
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Number | Date | Country | |
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20150260146 A1 | Sep 2015 | US |