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JP7760896B2 - Air-fuel ratio control device and air-fuel ratio control system - Google Patents
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JP7760896B2 - Air-fuel ratio control device and air-fuel ratio control system - Google Patents

Air-fuel ratio control device and air-fuel ratio control system

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Publication number
JP7760896B2
JP7760896B2 JP2021190055A JP2021190055A JP7760896B2 JP 7760896 B2 JP7760896 B2 JP 7760896B2 JP 2021190055 A JP2021190055 A JP 2021190055A JP 2021190055 A JP2021190055 A JP 2021190055A JP 7760896 B2 JP7760896 B2 JP 7760896B2
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air
fuel ratio
frequency
control device
downstream
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JP2023076990A (en
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豊史 津田
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Suzuki Motor Corp
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Suzuki Motor Corp
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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F01MACHINES OR ENGINES IN GENERAL; ENGINE PLANTS IN GENERAL; STEAM ENGINES
    • F01NGAS-FLOW SILENCERS OR EXHAUST APPARATUS FOR MACHINES OR ENGINES IN GENERAL; GAS-FLOW SILENCERS OR EXHAUST APPARATUS FOR INTERNAL-COMBUSTION ENGINES
    • F01N9/00Electrical control of exhaust gas treating apparatus
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F02COMBUSTION ENGINES; HOT-GAS OR COMBUSTION-PRODUCT ENGINE PLANTS
    • F02DCONTROLLING COMBUSTION ENGINES
    • F02D41/00Electrical control of supply of combustible mixture or its constituents
    • F02D41/02Circuit arrangements for generating control signals
    • F02D41/14Introducing closed-loop corrections
    • F02D41/1438Introducing closed-loop corrections using means for determining characteristics of the combustion gases; Sensors therefor
    • F02D41/1439Introducing closed-loop corrections using means for determining characteristics of the combustion gases; Sensors therefor characterised by the position of the sensor
    • F02D41/1441Plural sensors
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F02COMBUSTION ENGINES; HOT-GAS OR COMBUSTION-PRODUCT ENGINE PLANTS
    • F02DCONTROLLING COMBUSTION ENGINES
    • F02D41/00Electrical control of supply of combustible mixture or its constituents
    • F02D41/02Circuit arrangements for generating control signals
    • F02D41/14Introducing closed-loop corrections
    • F02D41/1438Introducing closed-loop corrections using means for determining characteristics of the combustion gases; Sensors therefor
    • F02D41/1444Introducing closed-loop corrections using means for determining characteristics of the combustion gases; Sensors therefor characterised by the characteristics of the combustion gases
    • F02D41/1454Introducing closed-loop corrections using means for determining characteristics of the combustion gases; Sensors therefor characterised by the characteristics of the combustion gases the characteristics being an oxygen content or concentration or the air-fuel ratio
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F01MACHINES OR ENGINES IN GENERAL; ENGINE PLANTS IN GENERAL; STEAM ENGINES
    • F01NGAS-FLOW SILENCERS OR EXHAUST APPARATUS FOR MACHINES OR ENGINES IN GENERAL; GAS-FLOW SILENCERS OR EXHAUST APPARATUS FOR INTERNAL-COMBUSTION ENGINES
    • F01N2430/00Influencing exhaust purification, e.g. starting of catalytic reaction, filter regeneration, or the like, by controlling engine operating characteristics
    • F01N2430/06Influencing exhaust purification, e.g. starting of catalytic reaction, filter regeneration, or the like, by controlling engine operating characteristics by varying fuel-air ratio, e.g. by enriching fuel-air mixture
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F01MACHINES OR ENGINES IN GENERAL; ENGINE PLANTS IN GENERAL; STEAM ENGINES
    • F01NGAS-FLOW SILENCERS OR EXHAUST APPARATUS FOR MACHINES OR ENGINES IN GENERAL; GAS-FLOW SILENCERS OR EXHAUST APPARATUS FOR INTERNAL-COMBUSTION ENGINES
    • F01N2560/00Exhaust systems with means for detecting or measuring exhaust gas components or characteristics
    • F01N2560/02Exhaust systems with means for detecting or measuring exhaust gas components or characteristics the means being an exhaust gas sensor
    • F01N2560/025Exhaust systems with means for detecting or measuring exhaust gas components or characteristics the means being an exhaust gas sensor for measuring or detecting O2, e.g. lambda sensors
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F01MACHINES OR ENGINES IN GENERAL; ENGINE PLANTS IN GENERAL; STEAM ENGINES
    • F01NGAS-FLOW SILENCERS OR EXHAUST APPARATUS FOR MACHINES OR ENGINES IN GENERAL; GAS-FLOW SILENCERS OR EXHAUST APPARATUS FOR INTERNAL-COMBUSTION ENGINES
    • F01N2560/00Exhaust systems with means for detecting or measuring exhaust gas components or characteristics
    • F01N2560/14Exhaust systems with means for detecting or measuring exhaust gas components or characteristics having more than one sensor of one kind
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F01MACHINES OR ENGINES IN GENERAL; ENGINE PLANTS IN GENERAL; STEAM ENGINES
    • F01NGAS-FLOW SILENCERS OR EXHAUST APPARATUS FOR MACHINES OR ENGINES IN GENERAL; GAS-FLOW SILENCERS OR EXHAUST APPARATUS FOR INTERNAL-COMBUSTION ENGINES
    • F01N2900/00Details of electrical control or of the monitoring of the exhaust gas treating apparatus
    • F01N2900/04Methods of control or diagnosing
    • F01N2900/0408Methods of control or diagnosing using a feed-back loop
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F01MACHINES OR ENGINES IN GENERAL; ENGINE PLANTS IN GENERAL; STEAM ENGINES
    • F01NGAS-FLOW SILENCERS OR EXHAUST APPARATUS FOR MACHINES OR ENGINES IN GENERAL; GAS-FLOW SILENCERS OR EXHAUST APPARATUS FOR INTERNAL-COMBUSTION ENGINES
    • F01N2900/00Details of electrical control or of the monitoring of the exhaust gas treating apparatus
    • F01N2900/04Methods of control or diagnosing
    • F01N2900/0422Methods of control or diagnosing measuring the elapsed time
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F01MACHINES OR ENGINES IN GENERAL; ENGINE PLANTS IN GENERAL; STEAM ENGINES
    • F01NGAS-FLOW SILENCERS OR EXHAUST APPARATUS FOR MACHINES OR ENGINES IN GENERAL; GAS-FLOW SILENCERS OR EXHAUST APPARATUS FOR INTERNAL-COMBUSTION ENGINES
    • F01N2900/00Details of electrical control or of the monitoring of the exhaust gas treating apparatus
    • F01N2900/06Parameters used for exhaust control or diagnosing
    • F01N2900/14Parameters used for exhaust control or diagnosing said parameters being related to the exhaust gas
    • F01N2900/1402Exhaust gas composition
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F01MACHINES OR ENGINES IN GENERAL; ENGINE PLANTS IN GENERAL; STEAM ENGINES
    • F01NGAS-FLOW SILENCERS OR EXHAUST APPARATUS FOR MACHINES OR ENGINES IN GENERAL; GAS-FLOW SILENCERS OR EXHAUST APPARATUS FOR INTERNAL-COMBUSTION ENGINES
    • F01N3/00Exhaust or silencing apparatus having means for purifying, rendering innocuous, or otherwise treating exhaust
    • F01N3/08Exhaust or silencing apparatus having means for purifying, rendering innocuous, or otherwise treating exhaust for rendering innocuous
    • F01N3/10Exhaust or silencing apparatus having means for purifying, rendering innocuous, or otherwise treating exhaust for rendering innocuous by thermal or catalytic conversion of noxious components of exhaust
    • F01N3/101Three-way catalysts

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  • Engineering & Computer Science (AREA)
  • Chemical & Material Sciences (AREA)
  • Combustion & Propulsion (AREA)
  • Mechanical Engineering (AREA)
  • General Engineering & Computer Science (AREA)
  • Electrical Control Of Air Or Fuel Supplied To Internal-Combustion Engine (AREA)
  • Exhaust Gas After Treatment (AREA)

Description

本発明の実施形態は、エンジンの空燃比制御技術に関する。 Embodiments of the present invention relate to engine air-fuel ratio control technology.

一般に、内燃機関に供給される燃料及び空気の混合気は、混合気中の酸素と燃料とが過不足なく反応する理論空燃比に維持するためにフィードバック制御がかけられる。
内燃機関の排気系に設置されるセンサで燃料リッチな状態が検知されると、エンジン制御装置(ECU:Engine Control Unit)を介して混合気の空燃比が引き上げられる。反対に、燃料リーンな状態が検知されると燃料が足されて空燃比が引き下げられる。このように、排気ガス成分に基づくフィードバック制御により、空燃比は理論空燃比を跨いで所定の周波数で変動しながら理論空燃比におおよそ維持される。
Generally, a mixture of fuel and air supplied to an internal combustion engine is subjected to feedback control to maintain a stoichiometric air-fuel ratio at which the oxygen in the mixture reacts with the fuel in just the right amount.
When a fuel-rich condition is detected by a sensor installed in the exhaust system of an internal combustion engine, the air-fuel ratio of the mixture is raised via the engine control unit (ECU). Conversely, when a fuel-lean condition is detected, fuel is added to lower the air-fuel ratio. In this way, through feedback control based on exhaust gas components, the air-fuel ratio is maintained approximately at the stoichiometric air-fuel ratio while fluctuating at a predetermined frequency across the stoichiometric air-fuel ratio.

ところで、従来から、空燃比を強制的に増減振動させることで排気浄化触媒(適宜、単に「触媒」という)の浄化率が向上することが知られている。この増減振動の周波数に対して触媒の浄化率が向上するメカニズムについては、酸素活性種の関与によるものと推測されている。また、空燃比の振動により反応成分を触媒に多く接触させることで触媒を昇温し、触媒の浄化率を向上させる技術も知られている。 It has long been known that the purification rate of an exhaust gas purification catalyst (sometimes simply referred to as "catalyst") can be improved by forcibly oscillating the air-fuel ratio. The mechanism by which the catalyst's purification rate improves with the frequency of this oscillation is thought to be due to the involvement of oxygen activated species. Another known technology improves the catalyst's purification rate by increasing the temperature of the catalyst by oscillating the air-fuel ratio to bring more reactive components into contact with the catalyst.

特開昭52-081438号公報Japanese Unexamined Patent Publication No. 52-081438

しかしながら、触媒コンバータの浄化率は、排気ガス量の変化など内燃機関の運転状態や排気浄化触媒の温度が変化した際に、浄化率が最高値から外れることがあるという課題があった。 However, there was an issue with the purification rate of catalytic converters, in that the purification rate could deviate from its maximum value when the operating conditions of the internal combustion engine, such as changes in exhaust gas volume, or the temperature of the exhaust purification catalyst changed.

本発明はこのような事情を考慮してなされたもので、簡易な構成で、内燃機関の運転状態や排気浄化触媒の温度が変化した場合にも、高い浄化率を維持することができる空燃比制御装置及び空燃比制御システムを提供することを目的とする。 The present invention was made in consideration of these circumstances, and aims to provide an air-fuel ratio control device and air-fuel ratio control system with a simple configuration that can maintain a high purification rate even when the operating state of the internal combustion engine or the temperature of the exhaust purification catalyst changes.

本実施形態に係る空燃比制御装置は、エンジンに接続された排気浄化触媒を流れる排気ガスの上流側における空燃比をリッチ側とリーン側とに振動させる空燃比調整部と、前記振動の周波数を段階的に変更して前記排気浄化触媒の下流側の前記排気ガスにおける空燃比である下流側空燃比または前記周波数に対する前記下流側空燃比の変化を測定する探索部と、前記下流側空燃比の値または前記周波数に対する前記下流側空燃比の変化の傾きが既定の閾値に達したときの前記周波数を最適周波数として決定する周波数決定部と、を備えるものである。 The air-fuel ratio control device according to this embodiment includes an air-fuel ratio adjusting unit that oscillates the air-fuel ratio on the upstream side of the exhaust gas flowing through an exhaust purification catalyst connected to an engine between the rich side and the lean side, a searching unit that changes the frequency of the oscillation in stages to measure a downstream air-fuel ratio, which is the air-fuel ratio in the exhaust gas on the downstream side of the exhaust purification catalyst, or a change in the downstream air-fuel ratio with respect to the frequency , and a frequency determining unit that determines, as an optimum frequency, the frequency when the value of the downstream air-fuel ratio or the gradient of the change in the downstream air-fuel ratio with respect to the frequency reaches a predetermined threshold value.

本発明により、簡易な構成で、内燃機関の運転状態や排気浄化触媒の温度が変化した場合にも、高い浄化率を維持することができる空燃比制御装置及び空燃比制御システムが提供される。 The present invention provides an air-fuel ratio control device and air-fuel ratio control system that has a simple configuration and can maintain a high purification rate even when the operating state of the internal combustion engine or the temperature of the exhaust purification catalyst changes.

本発明の第1実施形態に係る空燃比制御装置が適用された吸気ポート燃料噴射エンジンを示すブロック図。1 is a block diagram showing an intake port fuel injection engine to which an air-fuel ratio control device according to a first embodiment of the present invention is applied; 検証実験で用いたモデルガスの組成分を示す図。FIG. 1 shows the composition of the model gas used in the verification experiment. 触媒の性能、温度及び体積速度を変化させて測定した周波数と触媒の浄化率との関係を示す実験グラフを示す図。FIG. 10 is an experimental graph showing the relationship between the frequency measured by changing the catalyst performance, temperature, and volumetric velocity and the conversion rate of the catalyst. 触媒の性能、温度及び体積速度を変化させて測定した周波数と触媒の浄化率との関係を示す実験グラフを示す図。FIG. 10 is an experimental graph showing the relationship between the frequency measured by changing the catalyst performance, temperature, and volumetric velocity and the conversion rate of the catalyst. 触媒の性能、温度及び体積速度を変化させて測定した周波数と触媒の浄化率との関係を示す実験グラフを示す図。FIG. 10 is an experimental graph showing the relationship between the frequency measured by changing the catalyst performance, temperature, and volumetric velocity and the conversion rate of the catalyst. 触媒の性能、温度及び体積速度を変化させて測定した周波数と触媒の浄化率との関係を示す実験グラフを示す図。FIG. 10 is an experimental graph showing the relationship between the frequency measured by changing the catalyst performance, temperature, and volumetric velocity and the conversion rate of the catalyst. 浄化率の極大値より高い高周波数領域における上流側及び下流側の空燃比センサの出力波形を示すグラフ。6 is a graph showing output waveforms of the upstream and downstream air-fuel ratio sensors in a high frequency region higher than the maximum value of the purification rate. 図8は、浄化率の極大値より低い低周波数領域における上流側及び下流側の空燃比センサの出力波形を示すグラフ。FIG. 8 is a graph showing output waveforms of the upstream and downstream air-fuel ratio sensors in a low frequency region below the maximum value of the purification rate. 最適周波数を決定して浄化率を最適値に調整する手順について説明するフローチャート。4 is a flowchart illustrating a procedure for determining an optimum frequency and adjusting the purification rate to an optimum value. 第2実施形態に係る空燃比制御装置の動作を説明するフローチャート。10 is a flowchart illustrating the operation of an air-fuel ratio control device according to a second embodiment.

以下、本発明の実施形態を添付図面に基づいて説明する。
なお、実施形態において、エンジンから排出された排気ガスが正常に流れる向きを基準にして「上流」「下流」の用語を用いる。つまり、エンジンにより近い側が「上流側」、その反対側が「下流側」である。
Hereinafter, an embodiment of the present invention will be described with reference to the accompanying drawings.
In the embodiment, the terms "upstream" and "downstream" are used based on the normal flow direction of exhaust gas discharged from the engine. In other words, the side closer to the engine is the "upstream side," and the opposite side is the "downstream side."

(第1実施形態)
まず、図1のエンジン50及びその周辺機器のブロック図を用いて、第1実施形態に係る空燃比制御装置(以下、単に「制御装置」という)10について概説する。
第1実施形態に係る制御装置10は、直列接続型ハイブリッドエンジンや定置型エンジンなど、エンジン運転領域の変化が比較的緩慢なエンジン50に好適に適用される。
エンジン50には、図1に示されるように、エアクリーナ51を介して大気開放された吸気管52が、吸気マニホールドを介して接続される。エンジン50の燃料室に供給される空気は、この吸気管52から導入される。
(First embodiment)
First, an air-fuel ratio control device (hereinafter simply referred to as the "control device") 10 according to a first embodiment will be outlined using a block diagram of an engine 50 and its peripheral devices in FIG.
The control device 10 according to the first embodiment is suitably applied to an engine 50 in which the engine operating range changes relatively slowly, such as a series-connected hybrid engine or a stationary engine.
1, an intake pipe 52 that is open to the atmosphere via an air cleaner 51 is connected to the engine 50 via an intake manifold. Air is supplied to the fuel chamber of the engine 50 through this intake pipe 52.

また、エンジン50の排気ポートには、排気マニホールドを介して排気管53が接続される。また、排気管53の下流には、触媒コンバータ54が接続される。
触媒コンバータ54には、排気ガスG中のCO、HC及びNOxを除去する三元触媒などの排気浄化触媒(以下、単に「触媒」という)56が収容されている。また、触媒コンバータ54には、触媒56の上流側及び下流側にそれぞれ空燃比センサ(A/Fセンサ)57,58が設けられる。触媒56の上流側に設置された上側空燃比センサ57は、エンジン50で燃焼して排気され触媒56に流入してくる排気ガスGの空燃比を計測する。また、触媒56の下流側に設置された下側空燃比センサ58は、触媒56で浄化されて触媒56から流出してくる排気ガスGの空燃比(以下、「下流側空燃比」という)を計測する。つまり、第1実施形態における排気系の浄化システムは、いわゆる2A/Fセンサシステムで構成される。
An exhaust pipe 53 is connected to an exhaust port of the engine 50 via an exhaust manifold. A catalytic converter 54 is connected downstream of the exhaust pipe 53.
The catalytic converter 54 houses an exhaust purification catalyst (hereinafter simply referred to as the "catalyst") 56, such as a three-way catalyst, that removes CO, HC, and NOx from the exhaust gas G. The catalytic converter 54 is also provided with air-fuel ratio sensors (A/F sensors) 57, 58, respectively, upstream and downstream of the catalyst 56. The upper air-fuel ratio sensor 57, located upstream of the catalyst 56, measures the air-fuel ratio of the exhaust gas G that is burned in the engine 50, exhausted, and flows into the catalyst 56. The lower air-fuel ratio sensor 58, located downstream of the catalyst 56, measures the air-fuel ratio of the exhaust gas G that is purified by the catalyst 56 and flows out of the catalyst 56 (hereinafter referred to as the "downstream air-fuel ratio"). In other words, the exhaust purification system in the first embodiment is configured as a so-called two A/F sensor system.

また、エンジン50には、エンジン制御装置(ECU:Engine Control Unit)59が接続される。ECU59は、CPU(Central Processing Unit)、ROM(Read Only Memory)及びRAM(Random Access Memory)を備えたマイクロコンピュータとして構成される。CPUは、制御プログラムに従って所望の演算を実行して、種々の処理や制御を行う。ROMは、CPUで処理する制御プログラムや制御データを記憶し、RAMは、主として制御処理のための各種作業領域として使用される。
ECU59は、ネットワーク60でエンジン50各所や触媒コンバータ54に設けられるセンサ61,57,58及びアクチュエータに接続されて、エンジン50の動作を監視制御する。
An engine control unit (ECU) 59 is also connected to the engine 50. The ECU 59 is configured as a microcomputer equipped with a central processing unit (CPU), read-only memory (ROM), and random access memory (RAM). The CPU executes desired calculations in accordance with a control program to perform various processes and controls. The ROM stores the control programs and control data processed by the CPU, and the RAM is mainly used as a work area for various control processes.
The ECU 59 is connected via a network 60 to sensors 61 , 57 , 58 and actuators provided at various locations on the engine 50 and the catalytic converter 54 , and monitors and controls the operation of the engine 50 .

また、ECU59には、第1実施形態に係る制御装置10が設けられる。制御装置10は、空燃比調整部11、周波数決定12及び探索部13を備える。
空燃比調整部11は、上述の2つの空燃比センサ57,58からECU59に送られてくる排気ガスGの空燃比の情報に基づいて、エンジン50内の混合気がリッチ(燃料リッチ)であるかリーン(燃料リーン)であるか判断する。そして、空燃比調整部11は、空燃比が理論空燃比になるように、燃料の供給量を常時増減させて調整する。この調整により、吸気の空燃比の数値は、理論空燃比を跨いでリッチ及びリーン間を一定周期で変動する。この変動を以下、λ振動とよび、またこのλ振動の振動周波数を周波数Hとよぶ。なお、吸気の空燃比を振動させることで排気ガスGの空燃比の数値も周波数Hでλ振動をする。
The ECU 59 is also provided with the control device 10 according to the first embodiment. The control device 10 includes an air-fuel ratio adjusting unit 11, a frequency determining unit 12, and a searching unit 13.
The air-fuel ratio adjustment unit 11 determines whether the mixture in the engine 50 is rich (fuel rich) or lean (fuel lean) based on information about the air-fuel ratio of the exhaust gas G sent to the ECU 59 from the two air-fuel ratio sensors 57, 58 described above. The air-fuel ratio adjustment unit 11 then constantly increases or decreases the amount of fuel supplied to adjust the air-fuel ratio to the stoichiometric air-fuel ratio. This adjustment causes the intake air-fuel ratio to fluctuate between rich and lean at a constant cycle, straddling the stoichiometric air-fuel ratio. This fluctuation is hereinafter referred to as λ oscillation, and the oscillation frequency of this λ oscillation is referred to as frequency H. Note that by oscillating the intake air-fuel ratio, the air-fuel ratio of the exhaust gas G also oscillates λ at frequency H.

ここで、空燃比とほぼ同じ概念で、空燃比を理論空燃比で除算して規格化した物理量に空気過剰率λがある。このように規定される空気過剰率λは、空燃比が理論空燃比と一致したときに1となる。また、空気過剰率λが1より小さいときに空燃比はリッチな状態、空気過剰率λが1より大きいときに空燃比はリーンな状態となる。
以下では、制御装置10の各構成部11~13は、空燃比の代わりに空燃比を規格化したこの空気過剰率λを監視制御するものとして説明する。
Here, the excess air ratio λ is a physical quantity that is standardized by dividing the air-fuel ratio by the stoichiometric air-fuel ratio, and is based on almost the same concept as the air-fuel ratio. The excess air ratio λ defined in this way is 1 when the air-fuel ratio matches the stoichiometric air-fuel ratio. When the excess air ratio λ is less than 1, the air-fuel ratio is rich, and when the excess air ratio λ is greater than 1, the air-fuel ratio is lean.
In the following description, each of the components 11 to 13 of the control device 10 will be described as monitoring and controlling this excess air ratio λ, which is a normalized air-fuel ratio, instead of the air-fuel ratio itself.

探索部13は、空燃比調整部11を介して上側空燃比センサ57で取得される上側空気過剰率λに基づいてこの上側空気過剰率λのλ振動の周波数Hを変化させて最適周波数Hoを探索する。最適周波数Hoにおいて酸素活性種を最も効率良く利用できるため浄化率が極大になると推定されるためである。 The search unit 13 searches for the optimum frequency Ho by changing the frequency H of the λ oscillation of the upper air excess ratio λ f based on the upper air excess ratio λ f acquired by the upper air-fuel ratio sensor 57 via the air-fuel ratio adjustment unit 11. This is because it is estimated that the purification rate becomes maximum at the optimum frequency Ho because oxygen active species can be utilized most efficiently.

ここで、図2~図6を用いて、環境条件を変更させながらλ振動の周波数H、触媒56の浄化率及び下流側空燃比に基づく空気過剰率λの関係を調べた検証実験について説明する。
図2は、この検証実験で用いたモデルガスの組成分を示す表である。
この検証実験では、モデルガスの空気過剰率λをリッチ(λ=0.95)とリーン(λ=1.05)との間で振動させ、λ振動の周波数Hに対するTHC(全炭化水素)とNOxの浄化率を調べた。図2の表では、空気過剰率λのλ振動に合わせてリッチのときでは燃料の未燃成分である一酸化炭素COの含有量が多く、リーンのときでは酸素Oの含有率が高くなっていることが確認できる。
2 to 6, a verification experiment will be described in which the relationship between the frequency H of the λ oscillation, the purification rate of the catalyst 56, and the excess air ratio λ based on the downstream air-fuel ratio was investigated while changing environmental conditions.
FIG. 2 is a table showing the composition of the model gas used in this verification experiment.
In this verification experiment, the excess air ratio λ of the model gas was oscillated between rich (λ = 0.95) and lean (λ = 1.05), and the purification rates of THC (total hydrocarbons) and NOx were investigated as a function of the λ oscillation frequency H. The table in Figure 2 confirms that when the excess air ratio λ is rich in accordance with the λ oscillation, the content of carbon monoxide (CO), an unburned component of fuel, is high, and when it is lean, the content of oxygen (O2 ) is high.

また、図3~図6は、触媒56の性能、温度及び体積速度を変化させて測定した周波数Hと触媒56の浄化率との関係を示す実験グラフである。
図3~図6のいずれも、横軸は対数表示した周波数H[Hz]、左縦軸は浄化率[%]、右縦軸は後に図7,8を用いて詳述する最小空気過剰率λr_minである。横軸は対数表示なため、目盛の0は1[Hz]、目盛の-1は10-1[Hz]を示している。また、図3~図6において、「■」及び細い実線で表されるグラフは全炭化水素の浄化率、「●」及び細い破線で表されるグラフはNOxの浄化率を示す。また、「▲」,「△」は空気過剰率λの実測値であり、太い破線はこれらの空気過剰率λの実測値を直線でフィッティングしたものである。
3 to 6 are experimental graphs showing the relationship between the frequency H and the purification rate of the catalyst 56, measured by changing the performance, temperature, and volumetric velocity of the catalyst 56.
In all of Figures 3 to 6, the horizontal axis represents the frequency H [Hz] in logarithmic scale, the left vertical axis represents the purification rate [%], and the right vertical axis represents the minimum excess air factor λ r_min , which will be described in detail later using Figures 7 and 8. Because the horizontal axis is displayed logarithmically, 0 on the scale represents 1 [Hz], and -1 on the scale represents 10 -1 [Hz]. In addition, in Figures 3 to 6, graphs represented by "■" and thin solid lines represent the purification rate of total hydrocarbons, and graphs represented by "●" and thin dashed lines represent the purification rate of NOx. Furthermore, "▲" and "△" represent measured values of the excess air factor λ, and the thick dashed lines are linear fittings of these measured values of the excess air factor λ.

また、図3は、触媒性能を高性能、供給する排気ガスGの流量を触媒流量の30×103倍である「低流量」、触媒56の温度を450℃としたときの実験結果を表す。図4は図3の条件で温度を350℃に変更したときの実験結果を表す。図5は図3の条件で流量を約8倍の「高流量」に変更したときの実験結果を表す。図6は、図3の条件で触媒性能を低性能に変更したときの実験結果を表す。 Figure 3 shows the experimental results when the catalyst performance was set to high, the flow rate of the supplied exhaust gas G was set to "low flow rate" which is 30 x 103 times the catalyst flow rate, and the temperature of the catalyst 56 was set to 450°C. Figure 4 shows the experimental results when the temperature was changed to 350°C under the conditions of Figure 3. Figure 5 shows the experimental results when the flow rate was changed to "high flow rate" which is approximately 8 times the flow rate under the conditions of Figure 3. Figure 6 shows the experimental results when the catalyst performance was changed to low performance under the conditions of Figure 3.

このように環境条件を変えた図3~図6のいずれにおいても、最小空気過剰率λr_minは周波数Hの対数に対して直線的に変化し、浄化率が極大となる点で傾きgが不連続に変化していることが分かる。
言い換えると、空気過剰率λの測定値が不連続に飛躍している周波数H付近で全炭化水素及びNOxの両方の浄化率がほぼ極大値に達していることがわかる。つまり、空気過剰率λが最も1に近づいたときに触媒56の浄化率がほぼ極大になっていることが確認できる。
In this way, in all of Figures 3 to 6 where the environmental conditions are changed, it can be seen that the minimum excess air factor λ r_min changes linearly with the logarithm of the frequency H, and the slope g changes discontinuously at the point where the purification efficiency becomes maximum.
In other words, it can be seen that the purification rates of both total hydrocarbons and NOx reach their maximum values in the vicinity of frequency H where the measured value of the excess air ratio λ jumps discontinuously. In other words, it can be confirmed that the purification rates of the catalyst 56 reach their maximum when the excess air ratio λ approaches 1.

ここで、図3~図6中の右縦軸の変数である最小空気過剰率λr_minについて説明する。
図7は、浄化率の極大値より高い高周波数領域αにおける上流側及び下流側の空燃比センサ57,58の出力波形を示すグラフである。また、図8は、浄化率の極大値より低い低周波数領域βにおける上流側及び下流側の空燃比センサ57,58の出力波形を示すグラフである。
図7,8のグラフにおいて、横軸は時間[s]、左縦軸は触媒56の入口箇所のガス温度[℃]、右縦軸は空気過剰率λを表す。
グラフ中上側空燃比センサ57が検出した空気過剰率λを上側空気過剰率λとして細線で表している。また、下側空燃比センサ58が検出した下流側空燃比に基づく空気過剰率λを下側空気過剰率λrとして太線で表している。
Here, the minimum excess air ratio λ r_min, which is the variable on the right vertical axis in FIGS. 3 to 6, will be described.
Fig. 7 is a graph showing the output waveforms of the upstream and downstream air-fuel ratio sensors 57, 58 in a high frequency range α higher than the maximum value of the purification rate, and Fig. 8 is a graph showing the output waveforms of the upstream and downstream air-fuel ratio sensors 57, 58 in a low frequency range β lower than the maximum value of the purification rate.
7 and 8, the horizontal axis represents time [s], the left vertical axis represents the gas temperature [° C.] at the inlet of the catalyst 56, and the right vertical axis represents the excess air factor λ.
In the graph, the excess air ratio λ detected by the upper air-fuel ratio sensor 57 is represented by a thin line as an upper excess air ratio λf , and the excess air ratio λ based on the downstream air-fuel ratio detected by the lower air-fuel ratio sensor 58 is represented by a thick line as a lower excess air ratio λr .

図7の高周波数領域αにおいては、下側空気過剰率λrの振動が上側空気過剰率λと比較して大きく減衰していることが確認できる。この減衰は、触媒56の酸素貯蔵機能(OSC機能)がλ振動を吸収するためと考えられる。一方、図8の低周波数領域βにおいては、下側空気過剰率λrの振動が減衰していないことが確認できる。低周波数領域βにおいては触媒56のOSC機能ではもはやλ振動を緩和できないためと考えられる。
この結果から、高周波数領域αにおいては、下側空気過剰率λrは周波数Hの影響が極めて小さく、したがって傾きgの値は相対的に小さくなることが予想できる。また、低周波数領域βにおいては、下側空気過剰率λrは周波数Hが低下するほど小さくなり、したがって傾きgの値は相対的に大きくなることが予想できる。
It can be seen that in the high frequency region α of Fig. 7, the oscillations of the lower air excess ratio λr are attenuated more significantly than those of the upper air excess ratio λf . This attenuation is thought to be due to the oxygen storage capacity (OSC) function of the catalyst 56 absorbing the λ oscillations. On the other hand, in the low frequency region β of Fig. 8, it can be seen that the oscillations of the lower air excess ratio λr are not attenuated. This is thought to be due to the fact that the OSC function of the catalyst 56 can no longer mitigate the λ oscillations in the low frequency region β.
From this result, it can be predicted that in the high frequency region α, the effect of frequency H on the lower-side air excess factor λr is extremely small, and therefore the value of slope g will be relatively small. Also, in the low frequency region β, it can be predicted that the lower-side air excess factor λr will become smaller as frequency H decreases, and therefore the value of slope g will be relatively large.

そこで、検証実験では、下側空気過剰率λrの振動の極小値である最小空気過剰率λr_minを図7,8のグラフから読み取り図3~図6のグラフにプロットしていき、上述の傾向を実際に確認した。
なお、低周波数領域βよりもさらに周波数Hを下げた場合、定常リッチと定常リーンとが繰り返される状態になり、再び最小空気過剰率λr_minは周波数Hの影響を受けなくなる。また、この領域における触媒56の浄化率は低いことが確認されている。
Therefore, in the verification experiment, the minimum air excess ratio λ r_min , which is the minimum value of the oscillation of the lower air excess ratio λ r, was read from the graphs of FIGS. 7 and 8 and plotted on the graphs of FIGS. 3 to 6 to actually confirm the above-mentioned tendency.
If the frequency H is further lowered below the low frequency region β, the steady rich and steady lean states are repeated, and the minimum air excess ratio λ r_min is again no longer affected by the frequency H. It has also been confirmed that the purification rate of the catalyst 56 is low in this region.

この検証実験を踏まえ、探索部13は、図3~図6で示される周波数Hを変化させて最小空気過剰率λr_minを次々に測定していく。そして、探索部13は、高周波数領域αから低周波数領域βへ状態が転移して最小空気過剰率λr_minの値が不連続に急激に変化するときの周波数Hすなわち最適周波数Hoを探索する。
最適周波数Hoは、最小空気過剰率λr_minに代えて縦軸の最小空気過剰率λr_minの値の変化を横軸の周波数Hの変化で除算した傾きgを用いて探索してもよい。つまり、下側空燃比センサ58の出力値から次式(1)で計算される傾きgを用いて探索してもよい。

g=Δλr_min/Δlog(周波数H) (1)

なお、周波数Hを周波数そのものでなくその対数をとることで周波数Hに対する最小空気過剰率λr_minの傾向をより明確に検知することができる。
周波数決定12は、傾きgを急激に変化させる周波数Hを最適周波数Hoとして決定する。周波数決定12が決定した最適周波数Hoを空燃比調整部11が維持する。
Based on this verification experiment, the search unit 13 successively measures the minimum air excess factor λ r_min while changing the frequency H shown in Figures 3 to 6. Then, the search unit 13 searches for the frequency H at which the value of the minimum air excess factor λ r_min changes suddenly and discontinuously as the state transitions from the high frequency region α to the low frequency region β, i.e., the optimal frequency Ho .
The optimal frequency H o may be searched for using a gradient g obtained by dividing a change in the value of the minimum excess air ratio λ r_min on the vertical axis by a change in the frequency H on the horizontal axis, instead of the minimum excess air ratio λ r_min . In other words, the optimal frequency H o may be searched for using a gradient g calculated from the output value of the lower air-fuel ratio sensor 58 using the following equation (1).

g=Δλ r_min /Δlog (frequency H) (1)

It should be noted that by taking the logarithm of the frequency H rather than the frequency itself, the tendency of the minimum air excess factor λ r — min relative to the frequency H can be detected more clearly.
The frequency determination unit 12 determines the frequency H that causes the gradient g to change rapidly as the optimum frequency H 0. The air-fuel ratio adjustment unit 11 maintains the optimum frequency H 0 determined by the frequency determination unit 12.

なお、傾きgではなく、上述のように最小空気過剰率λr_min自体の数値を監視し、最小空気過剰率λr_minの不連続変化から浄化率が極大となる周波数Hを推定してもよい。この場合、例えば周波数Hを下げていく場合において、予め設定した閾値Ω未満となったことを以て浄化率が極大となる周波数領域であると判断する。
また、傾きgによる推定と、この最小空気過剰率λr_min自体による推定と、を組み合わせて最適周波数Hoを特定してもよい。これらを組み合わせて最適周波数Hoを決定することで、最適周波数Hoの精度を高めることができる。
Note that instead of the gradient g, the numerical value of the minimum air excess factor λ r_min itself may be monitored as described above, and the frequency H at which the purification efficiency becomes maximum may be estimated from discontinuous changes in the minimum air excess factor λ r_min . In this case, for example, when the frequency H is lowered, the frequency range at which the purification efficiency becomes maximum is determined to be the frequency range at which the purification efficiency becomes maximum when the frequency H becomes less than a preset threshold Ω.
Furthermore, the optimum frequency H o may be determined by combining the estimation based on the gradient g and the estimation based on the minimum air excess factor λ r_min itself. By combining these to determine the optimum frequency H o , the accuracy of the optimum frequency H o can be improved.

なお、エンジン回転数と運転負荷との関係を示すマップなど、エンジン50の運転状態を表すマップを各周波数HごとにECU59に保持させておくことが望ましい。そして、運転状態が異なるマップに移行したことをトリガーとして、探索部13が最適周波数Hoの探索を開始することが望ましい。運転状態が大きく変更されたタイミングで探索をかけなおすことで、常時浄化率を最高値に維持することができる。また、マップごとに最適周波数Hoの妥当範囲をECU59に記憶させておいてもよい。異なるマップに移行した場合にそのマップについて記憶させておいた妥当範囲内で最適周波数Hoを探索することで、より短時間で浄化率を最高値にすることができる。 It is desirable that the ECU 59 stores a map showing the operating state of the engine 50 for each frequency H, such as a map showing the relationship between engine speed and operating load. It is desirable that the search unit 13 starts searching for the optimal frequency H when the operating state changes to a different map. By restarting the search when the operating state changes significantly, the purification rate can be maintained at its highest value. The ECU 59 may also store a valid range for the optimal frequency H for each map. When a different map is switched to, the purification rate can be maximized in a shorter time by searching for the optimal frequency H within the valid range stored for that map.

また、例えば1万時間または1万kmなど、運転時間または走行距離が一定値を超えた際にも最適周波数Hoを探索して更新することが望ましい。このようなタイミングで補正することで、エンジン50や触媒56の劣化の進行による極大値の変化に合わせて最適周波数Hoを補正することができる。 It is also desirable to search for and update the optimum frequency H o when the driving time or distance exceeds a certain value, such as 10,000 hours or 10,000 km. By correcting the optimum frequency H o at such timing, it is possible to correct the optimum frequency H o in accordance with changes in the maximum value due to the progression of deterioration of the engine 50 and the catalyst 56.

次に、図9のフローチャートを用いて、最適周波数Hoを決定して浄化率を最適値に調整する手順について説明する(適宜図3~図8を参照)。なお、図9及び以下の説明において、各ステップを「S11」などと表記する。
また、探索部13は、周波数Hを横軸、最小空気過剰率λr_minを縦軸としたときの傾きgを用いて探索する例で説明する。
Next, the procedure for determining the optimum frequency H0 and adjusting the purification rate to the optimum value will be described using the flowchart in Figure 9 (see Figures 3 to 8 as appropriate). Note that in Figure 9 and the following description, each step will be denoted as "S11," etc.
Further, an example will be described in which the search unit 13 performs a search using a gradient g when the horizontal axis represents the frequency H and the vertical axis represents the minimum air excess factor λ r — min .

まず、探索部13は、図9に示されるように、下側空燃比センサ58の出力値である下側空気過剰率λr及び上側空燃比センサ57の出力値である上側空気過剰率λをモニタする(S11)。このとき、探索部13は、空燃比調整部11を介して上側空燃比センサ57の出力する上側空気過剰率λに基づいてλ振動を制御する。そして、探索部13は、下側空気過剰率λrのλ振動の極小値である最小空気過剰率λr_minを抽出する。
次に、周波数Hを標準値1Hzから対数目盛の所定目盛ずつ徐々に下げて、片対数グラフ上に最小空気過剰率λr_minをプロットしていく(S12)。
9 , the searching unit 13 monitors the lower excess air factor λr, which is the output value of the lower air-fuel ratio sensor 58, and the upper excess air factor λf , which is the output value of the upper air-fuel ratio sensor 57 (S11). At this time, the searching unit 13 controls the λ oscillation based on the upper excess air factor λf output by the upper air-fuel ratio sensor 57 via the air-fuel ratio adjusting unit 11. Then, the searching unit 13 extracts the minimum excess air factor λr_min , which is the minimum value of the λ oscillation of the lower excess air factor λr .
Next, the frequency H is gradually decreased by a predetermined number of divisions on the logarithmic scale from the standard value of 1 Hz, and the minimum air excess factor λ r — min is plotted on a semi-logarithmic graph (S12).

グラフの傾きgが閾値g未満のうちは、周波数Hを引き下げていく(S13においてNO,S12へ)。
そして、グラフの傾きgが閾値gを超えた場合(S13においてYES)、低周波数領域βに遷移したと判断して終了する(S14,END)。
周波数決定12は、このときの周波数Hを最適周波数Hoとして決定する。また、空燃比調整部11は、λ振動の周波数Hとするように調整する。
While the gradient g of the graph is less than the threshold value g0 , the frequency H is decreased (NO in S13, return to S12).
If the gradient g of the graph exceeds the threshold value g0 (YES in S13), it is determined that a transition has occurred to the low frequency region β, and the process ends (S14, END).
The frequency determination unit 12 determines the frequency H at this time as the optimum frequency Ho . The air-fuel ratio adjustment unit 11 also adjusts the frequency H to be the frequency of λ oscillation.

なお、閾値gの値が大きすぎると高周波数領域αから低周波数領域βに遷移しても閾値gではその遷移を検知できなくなる。また、閾値gの値が小さすぎると遷移をしていない段階で遷移があったと誤診断して不適切な周波数Hを誤検出してしまう。この閾値gは、実験的に0.015~0.025程度とすることが望ましいと分かっている。閾値gをこの範囲とすることで、精度よく最適周波数Hoを特定することができる。ただし、触媒56の仕様やエンジン50の仕様に応じて設計段階で決定される。 If the value of the threshold g0 is too large, the threshold g0 will not be able to detect a transition from the high frequency region α to the low frequency region β. If the value of the threshold g0 is too small, a transition will be erroneously diagnosed when it has not actually occurred, resulting in an inappropriate frequency H being erroneously detected. Experiments have shown that the threshold g0 is preferably set to approximately 0.015 to 0.025. By setting the threshold g0 within this range, the optimal frequency H0 can be identified with high accuracy. However, this is determined at the design stage depending on the specifications of the catalyst 56 and the engine 50.

以上のように、第1実施形態に係る制御装置10によれば、簡易な構成で、内燃機関の運転状態や触媒56の温度が変化した場合にも、高い浄化率を維持することができる。 As described above, the control device 10 according to the first embodiment has a simple configuration and can maintain a high purification rate even when the operating state of the internal combustion engine or the temperature of the catalyst 56 changes.

(第2実施形態)
図10は第2実施形態に係る制御装置10の動作を説明するフローチャートである。
第2実施形態では、図10に示されるように、周波数決定12が、傾きgが閾値gを超えた際のλ振動の周波数Hを微小割合増加または減少させて最適周波数Hoとする(S15)。
ここで、微小割合とは、周波数Hの刻み幅の例えば1割など、2割以下の割合のことをいう。つまり、第2実施形態では、第1実施形態で決定した最適周波数Hoに微小割合だけ加減して補正して、改めて最適周波数Hoとする。
Second Embodiment
FIG. 10 is a flowchart illustrating the operation of the control device 10 according to the second embodiment.
In the second embodiment, as shown in FIG. 10, the frequency determination 12 increases or decreases the frequency H of the λ vibration when the gradient g exceeds the threshold value g 0 by a small percentage to set it as the optimum frequency H 0 (S15).
Here, the term "tiny proportion" refers to a proportion of 20% or less, such as 10% of the step width of the frequency H. In other words, in the second embodiment, the optimum frequency H 0 determined in the first embodiment is corrected by adding or subtracting a small proportion, and the optimum frequency H 0 is set anew.

周波数Hの変化の刻み幅を小さくすると、その度にトルク変動が発生して乗車者の乗り心地を損なう。特にフライホイールが小さい場合、乗車者が体感するトルク変動は大きくなる。
そこで、第2実施形態では、周波数Hの刻みを大きくとり、探索部13による探索によるトルク変動の回数を低減させる。そして、傾きgが閾値gを超えたことを検知したときには、既に最適周波数Hoを跨いだ先のより小さい周波数Hが検出されていると想定する。そして、周波数決定12は、最適周波数Hoよりも小さいと考えられる検出された周波数Hに微小割合を加えた値を最適周波数Hoとする。
なお、低周波数領域βから周波数Hを段階的に上げていく場合には、閾値gを超えたときの周波数Hから微小割合だけ減じて最適周波数Hoとする。
If the step size of the change in frequency H is made small, torque fluctuations occur each time, which impairs the riding comfort of the passenger. In particular, if the flywheel is small, the torque fluctuations felt by the passenger become large.
Therefore, in the second embodiment, the frequency H is increased in increments to reduce the number of torque fluctuations due to the search by the search unit 13. When it is detected that the gradient g exceeds the threshold value g0 , it is assumed that a lower frequency H beyond the optimum frequency Ho has already been detected. The frequency determination unit 12 then sets the optimum frequency Ho to a value obtained by adding a small percentage to the detected frequency H that is considered to be lower than the optimum frequency Ho .
When the frequency H is increased stepwise from the low frequency region β, the optimum frequency H 0 is obtained by subtracting a small percentage from the frequency H when the threshold value g 0 is exceeded.

なお、第2実施形態では、探索部13の動作手順に検出した周波数Hに微小割合だけ補正をして最適周波数Hoとすること以外は第1実施形態と同様であるため、重複する説明を省略する。図面においても同様に、重複する構成には同一の符号を付して説明を省略する。 In the second embodiment, the frequency H detected in the operation procedure of the search unit 13 is corrected by a small percentage to obtain the optimum frequency Ho, and therefore a duplicated description will be omitted. Similarly, in the drawings, duplicated components are denoted by the same reference numerals and a description thereof will be omitted.

以上のように、第2実施形態に係る制御装置10によれば、トルク変動が小さく乗車者に快適な乗り心地を提供することができる。 As described above, the control device 10 according to the second embodiment reduces torque fluctuations, providing a comfortable ride for the passenger.

以上述べた各実施形態に係る制御装置10によれば、簡易な構成で、エンジン50の運転状態または排気浄化触媒56の温度が変化した場合にも、高い浄化率を維持することができることができる。 The control device 10 according to each of the above-described embodiments has a simple configuration and can maintain a high purification rate even when the operating state of the engine 50 or the temperature of the exhaust purification catalyst 56 changes.

本発明の実施形態を説明したが、この実施形態は、例として提示したものであり、発明の範囲を限定することは意図していない。
実施形態は、その他の様々な形態で実施されることが可能であり、発明の要旨を逸脱しない範囲で、種々の省略、置き換え、変更、組み合わせを行うことができる。実施形態やその変形は、発明の範囲や要旨に含まれると同様に、特許請求の範囲に記載された発明とその均等の範囲に含まれるものである。
Although an embodiment of the present invention has been described, this embodiment is presented as an example and is not intended to limit the scope of the invention.
The embodiments may be embodied in various other forms, and various omissions, substitutions, modifications, and combinations may be made without departing from the spirit of the invention. The embodiments and their modifications are included in the scope of the inventions and their equivalents as defined in the claims, as well as in the scope and spirit of the inventions.

例えば、エンジン運転領域の変化が比較的緩慢なエンジンに対してより好適であると説明したが、空燃比制御装置が適用されるエンジンは変化が緩慢なエンジンに限定されるものではない。 For example, although it has been explained that the air-fuel ratio control device is more suitable for engines in which the engine operating range changes relatively slowly, engines to which the air-fuel ratio control device is applicable are not limited to engines in which the changes are slow.

10…制御装置、11…空燃比調整部、12…周波数決定、13…探索部、50…エンジン、51…エアクリーナ、52…吸気管、53…排気管、54…触媒コンバータ、56…排気浄化触媒(触媒)、57…上側空燃比センサ、58…下側空燃比センサ、59…ECU、60…ネットワーク、61…センサ、G…排気ガス、H…周波数、Ho…最適周波数、g…傾き、g…閾値、Ω…閾値、α…高周波数領域、β…低周波数領域、λ…空気過剰率、λ…上側空気過剰率、λr…下側空気過剰率、λr_min…最小空気過剰率。 10...control device, 11...air-fuel ratio adjustment unit, 12...frequency determination, 13...search unit, 50...engine, 51...air cleaner, 52...intake pipe, 53...exhaust pipe, 54...catalytic converter, 56...exhaust purification catalyst (catalyst), 57...upper air-fuel ratio sensor, 58...lower air-fuel ratio sensor, 59...ECU, 60...network, 61...sensor, G...exhaust gas, H...frequency, H o ...optimum frequency, g...slope, g 0 ...threshold, Ω...threshold, α...high frequency region, β...low frequency region, λ...air excess ratio, λ f ...upper air excess ratio, λ r ...lower air excess ratio, λ r_min ...minimum air excess ratio.

Claims (6)

エンジンに接続された排気浄化触媒を流れる排気ガスの上流側における空燃比をリッチ側とリーン側とに振動させる空燃比調整部と、
前記振動の周波数を段階的に変更して前記排気浄化触媒の下流側の前記排気ガスにおける空燃比である下流側空燃比または前記周波数に対する前記下流側空燃比の変化を測定する探索部と、
前記下流側空燃比の値または前記周波数に対する前記下流側空燃比の変化の傾きが既定の閾値に達したときの前記周波数を最適周波数として決定する周波数決定部と、を備えることを特徴とする空燃比制御装置。
an air-fuel ratio adjusting unit that oscillates an air-fuel ratio between a rich side and a lean side on the upstream side of exhaust gas flowing through an exhaust purification catalyst connected to the engine;
a searching unit that measures a downstream air-fuel ratio, which is an air-fuel ratio in the exhaust gas downstream of the exhaust purification catalyst, or a change in the downstream air-fuel ratio with respect to the frequency by changing the frequency of the vibration in a stepwise manner;
a frequency determination unit that determines, as an optimal frequency, the frequency when the value of the downstream air-fuel ratio or a gradient of change in the downstream air-fuel ratio with respect to the frequency reaches a predetermined threshold value.
前記傾きは、前記周波数の対数に対する前記下流側空燃比の変化の割合である請求項1に記載の空燃比制御装置。 2. The air-fuel ratio control device according to claim 1, wherein the gradient is a rate of change of the downstream air-fuel ratio with respect to the logarithm of the frequency. 前記閾値は、0.015~0.025の範囲であり、
前記周波数決定部は、前記振動の周波数を低下させていく際に、前記周波数の対数に対して前記下流側空燃比が減少する傾きの絶対値が前記閾値に達したときの前記周波数を、前記最適周波数として決定する請求項2に記載の空燃比制御装置。
the threshold value is in the range of 0.015 to 0.025;
3. The air-fuel ratio control device according to claim 2, wherein the frequency determiner determines, as the optimal frequency, the frequency at which an absolute value of a gradient at which the downstream air-fuel ratio decreases with respect to a logarithm of the frequency reaches the threshold value when lowering the frequency of the vibration .
前記周波数毎に内燃機関の回転数と運転負荷との関係を示すマップを備え、
前記探索部は、異なる前記マップに移行した際に探索をやりなおす請求項1から請求項3のいずれか一項に記載の空燃比制御装置。
a map showing a relationship between the rotation speed and the operating load of the internal combustion engine for each of the frequencies;
4. The air-fuel ratio control device according to claim 1, wherein the search unit performs the search again when the map is changed to a different map.
前記周波数決定部は、探索に用いた周波数幅の所定割合を前記最適周波数に加減算して前記最適周波数を補正する請求項1から請求項4のいずれか一項に記載の空燃比制御装置。 An air-fuel ratio control device according to any one of claims 1 to 4, wherein the frequency determination unit corrects the optimal frequency by adding or subtracting a predetermined percentage of the frequency width used in the search to the optimal frequency. 請求項1から請求項5のいずれか一項に記載の空燃比制御装置と、
前記エンジンと、
前記排気浄化触媒と、
前記排気浄化触媒の上流側及び下流側に配置されて空燃比を検知する2以上の空燃比センサと、を備えることを特徴とする空燃比制御システム。
An air-fuel ratio control device according to any one of claims 1 to 5;
the engine;
the exhaust purification catalyst;
and two or more air-fuel ratio sensors arranged upstream and downstream of the exhaust purification catalyst to detect the air-fuel ratio.
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