JPS6034065B2 - Air fuel ratio detection method - Google Patents
Air fuel ratio detection methodInfo
- Publication number
- JPS6034065B2 JPS6034065B2 JP54164822A JP16482279A JPS6034065B2 JP S6034065 B2 JPS6034065 B2 JP S6034065B2 JP 54164822 A JP54164822 A JP 54164822A JP 16482279 A JP16482279 A JP 16482279A JP S6034065 B2 JPS6034065 B2 JP S6034065B2
- Authority
- JP
- Japan
- Prior art keywords
- layer
- oxygen
- fuel ratio
- air
- partial pressure
- 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
Links
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- Measuring Oxygen Concentration In Cells (AREA)
- Electrical Control Of Air Or Fuel Supplied To Internal-Combustion Engine (AREA)
Description
【発明の詳細な説明】
この発明は、特に理論空燃比(理論状態にある空気と燃
料との比)よりも希薄な空燃比を検出するのに好適な空
燃比検出方法に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an air-fuel ratio detection method particularly suitable for detecting an air-fuel ratio leaner than the stoichiometric air-fuel ratio (the ratio of air to fuel in a stoichiometric state).
酸素イオン伝導性団体電解質を使用し、酸素濃淡電池の
原理を応用して酸素濃度の検出をおこなうようにして酸
素センサ素子は既知である。Oxygen sensor elements are known that use an oxygen ion-conducting collective electrolyte and apply the principle of an oxygen concentration battery to detect oxygen concentration.
第1図はこの種酸素センサ素子の一例を示す断面説明図
であって、Y203を添加して安定化したZr02固体
電解質粉末を管状に成形焼結した固体電解質管1の内外
表面に、それぞれ基準極電子伝導層2および測定極電子
伝導層3を設け、基準極電子伝導層2を大気Aにさらす
と共に、測定極電子伝導層3を保護層4を介して被検ガ
ス(たとえば、内燃機関の排ガス)Gにさらすようにし
た構造をなしている。このとき、保護層4は上記内燃機
関の高温高速排ガスが直接測定極電子伝導層3に接触す
るのを防止して酸素センサ素子の耐久性を向上させるた
めに設けられている。そこで、酸素濃淡電池の原理によ
り、上記固体電解質管1の両面における酸素分圧の差に
対応して起電力Eを次式{1}に基いて発生する。E辛
1農三 .・・.・・【11
ただし、R:気体定数
T:絶対温度
F:ファラデー定数
P。FIG. 1 is an explanatory cross-sectional view showing an example of this type of oxygen sensor element, in which reference marks are placed on the inner and outer surfaces of a solid electrolyte tube 1 made by shaping and sintering Zr02 solid electrolyte powder stabilized by adding Y203 into a tube shape. A polar electron conductive layer 2 and a measuring electrode electronic conductive layer 3 are provided, and the reference electrode electronic conductive layer 2 is exposed to the atmosphere A, and the measuring electrode electronic conductive layer 3 is exposed to a test gas (for example, from an internal combustion engine) through a protective layer 4. The structure is such that it is exposed to exhaust gas). At this time, the protective layer 4 is provided to prevent the high-temperature, high-speed exhaust gas of the internal combustion engine from directly contacting the measurement electrode electron conductive layer 3, thereby improving the durability of the oxygen sensor element. Therefore, according to the principle of an oxygen concentration battery, an electromotive force E is generated based on the following equation {1} in accordance with the difference in oxygen partial pressure on both sides of the solid electrolyte tube 1. E spicy 1 Nozo .・・・. ...[11 However, R: gas constant T: absolute temperature F: Faraday constant P.
2:測定極酸素分圧
ところで、排ガス中の酸素濃度は、第2図に示すように
、理論空燃比付近から次第に増大するが、測定極酸素分
圧P。2: Measured polar oxygen partial pressure By the way, as shown in FIG. 2, the oxygen concentration in the exhaust gas gradually increases from around the stoichiometric air-fuel ratio, but the measured polar oxygen partial pressure P.
2は、第3図に示すように、測定極電子伝導層3を形成
する白金(Pt)の触媒作用のために、理論空燃比より
濃い空燃比(ガソリン内燃機関の場合はA/F<14.
7)ではほぼ位tmとなり、理論空燃比より空燃比が希
薄になると酸素分圧は急峻に増大する。2, as shown in FIG. 3, the air-fuel ratio is higher than the stoichiometric air-fuel ratio (A/F<14 in the case of a gasoline internal combustion engine) due to the catalytic action of platinum (Pt) forming the measurement electrode electron conductive layer 3. ..
7), it becomes approximately tm, and when the air-fuel ratio becomes leaner than the stoichiometric air-fuel ratio, the oxygen partial pressure increases sharply.
したがって、式‘1’に示す起電力(E)と空燃比(A
/F)との関係は、第4図に示すよに、燃料過剰側で大
きな起電力を発生する特性を示し、理論空燃比(入=1
)の検出が可能である。そのほか、この種の酸素センサ
素子としては、基板上に基準極電子伝導層、酸素イオン
伝導性固体電解質層および測定極電子伝導層を順次積層
した膜構造型の酸素センサ素子も試みられており、測定
極電子伝導層が直接高温高速の排ガス流にさらされるの
を防止するために同様に測定極電子伝導層の表面または
酸素センサ素子表面の全体に保護層を設けて耐久性の向
上をはかった上で第4図の場合と同様の特性を得て理論
空燃比の検出を可能にしたものである。Therefore, the electromotive force (E) and air-fuel ratio (A
/F), as shown in Figure 4, shows the characteristic that a large electromotive force is generated on the fuel excess side, and the stoichiometric air-fuel ratio (input = 1
) can be detected. In addition, as this type of oxygen sensor element, a membrane structure type oxygen sensor element in which a reference electrode electron conductive layer, an oxygen ion conductive solid electrolyte layer, and a measurement electrode electron conductive layer are successively laminated on a substrate has also been attempted. In order to prevent the measurement electrode electron conduction layer from being directly exposed to high-temperature, high-speed exhaust gas flow, a protective layer was similarly provided on the entire surface of the measurement electrode electron conduction layer or the surface of the oxygen sensor element to improve durability. The same characteristics as in the case shown in FIG. 4 are obtained and the stoichiometric air-fuel ratio can be detected.
しかしながら、上述した従来の酸素センサ素子を用いて
空燃比の検出をおこなう場合、測定極電子伝導層に直接
排ガス等の被検ガスを接触させ、測定極電子伝導層の触
媒作用による測定極酸素分圧の理論空燃比を境とした急
激な変化(第3図参照)をもとにして理論空燃比を検出
するようにしているため、理論空燃比以外の検出は不可
能であった。However, when detecting the air-fuel ratio using the conventional oxygen sensor element described above, a test gas such as exhaust gas is brought into direct contact with the electron conductive layer of the measurement electrode, and the oxygen concentration at the measurement electrode is caused by the catalytic action of the electron conduction layer of the measurement electrode. Since the stoichiometric air-fuel ratio is detected based on a sudden change in pressure around the stoichiometric air-fuel ratio (see FIG. 3), it has been impossible to detect anything other than the stoichiometric air-fuel ratio.
したがって、たとえば理論空燃比における内燃機関の空
燃比制御には適しているものの、希薄燃焼させて燃料消
費効率の向上をはかろうとする場合における内燃機関の
空燃比制御には使用できない欠点を有していた。この発
明の目的は、上述した従来技術の欠点を解消し、理論空
燃比よりも希薄な空燃比の検出が可能な空燃比検出方法
を堤供することにあり、これによって、たとえば内燃機
関の空燃比制御において希薄燃焼を可能にして燃料消費
効率を高めうるようにすることにある。Therefore, although it is suitable for controlling the air-fuel ratio of an internal combustion engine at the stoichiometric air-fuel ratio, it has the disadvantage that it cannot be used for controlling the air-fuel ratio of an internal combustion engine when trying to improve fuel consumption efficiency by performing lean combustion. was. An object of the present invention is to eliminate the drawbacks of the prior art described above and to provide an air-fuel ratio detection method capable of detecting an air-fuel ratio leaner than the stoichiometric air-fuel ratio. The purpose is to enable lean combustion in control and increase fuel consumption efficiency.
この発明の空燃比制御方法は、隔膜層、基準極鰭子伝導
層、酸素イオン伝導性固体電解質層および測定極電子伝
導層を横層し、前記隔膜層および酸素イオン伝導性固体
電解質層のうち少なくともいずれか一方がガス透過性で
あり、前記基準極電子伝導層と測定極電子伝導層との間
に直流電源を接続する酸素センサ素子の前記測定極電子
伝導層の表面に、酸素に関するガス拡散係数が6×10
‐9なし・し2xlo−7mole/a肌・secの範
囲であって酸素分子の拡散を制御しうるガス拡散制御層
を設けて被検ガスと接触可能にした酸素センサ素子を用
い、前記直流電源により供給される電流によって前記測
定極電子伝導層から基準極電子伝導層に向けて酸素イオ
ンの移動を強制的に生じさせることにより前記測定極酸
素分圧を被検ガス中の酸素分圧よりも所望値だけ低下さ
せ、前記低下させた測定極酸素分圧と基準極酸素分圧と
の差に対応して発生する起電力を測定することによって
理論空燃比よりも希薄な空燃比の検出を可能にしたこと
を特徴としている。The air-fuel ratio control method of the present invention includes horizontally layering a diaphragm layer, a reference pole fin conductive layer, an oxygen ion conductive solid electrolyte layer, and a measurement pole electron conductive layer, and among the diaphragm layer and the oxygen ion conductive solid electrolyte layer. At least one of them is gas permeable, and a DC power source is connected between the reference electrode electron conductive layer and the measurement electrode electron conductive layer. The coefficient is 6×10
-9 None/2 x lo -7 mole/a skin/sec using an oxygen sensor element that is provided with a gas diffusion control layer that can control the diffusion of oxygen molecules and that can come into contact with the test gas; By forcing the movement of oxygen ions from the measurement electrode electron conduction layer toward the reference electrode electron conduction layer by means of the current supplied by It is possible to detect an air-fuel ratio leaner than the stoichiometric air-fuel ratio by lowering it by a desired value and measuring the electromotive force generated in response to the difference between the reduced measured polar oxygen partial pressure and the reference polar oxygen partial pressure. It is characterized by the fact that
第5図はこの発明の実施に適用されうる酸素センサ素子
10の縦断面模型的結線図、第6図は第5図の酸素セン
サ素子10の模型的分解斜視図であって、隔膜層11は
アルミナ、ムライト、スピネル等の絶縁性物質からなり
、その内部には第7図に例示する如き形状の発熱体12
を設けていると共に、構造基体としての強度を保持して
いる。FIG. 5 is a schematic vertical cross-sectional wiring diagram of the oxygen sensor element 10 that can be applied to the implementation of the present invention, and FIG. 6 is a schematic exploded perspective view of the oxygen sensor element 10 of FIG. It is made of an insulating material such as alumina, mullite, spinel, etc., and has a heating element 12 in the shape shown in FIG.
It also maintains the strength as a structural base.
この隔膜層11の表面上には、二つに分けた基準極電子
伝導層13,14を積層し、さらにその上に酸素イオン
伝導性固体電解質層15を積層している。この固体電解
質層15の素材としては、Y203やCaoで安定化し
たZの2その他既知のものを採用することができる。こ
の固体電解質層15の表面には測定極電子伝導層16を
務層し、この測定極電子伝導層16と前記一方の基準極
電子伝導層13との間に電圧測定手段17を接続して起
電力Eの測定を可能にすると共に、測定極電子伝導層1
6と前記他方の基準極電子伝導層14との間に直流電源
18接続している。このとき、基準極電子伝導層13,
14および測定極電子伝導層16には触媒活性の白金を
用いるのが望ましく、そのほか白金と白金族元素との合
金その他の材料を適宜選択して使用するのが良い。また
、上記各電子伝導層13,14,16および固体電解質
層15を積層するに際しては、たとえばそれらの粉末を
ペースト状にしてスクリーンに印刷し、その後焼成する
手段などを用いることができ、その他の手段によること
も可能である。また、発熱体12には加熱用電源19を
接続して酸素センサ素子の温度を制御させうるようにし
ている。さらに、前記測定極電子伝導層16上には、被
検ガスから流入する酸素分子の拡散を制御しうるガス拡
散制御層20を設け、このガス拡散制御層20を被検ガ
スと接触可能している。この場合、ガス拡散制御層20
のガス拡散係数は、後述の実施例においても示すように
、6×10‐9なし、し2×10‐7mole/atm
・secの範囲内とするのがよい。そして、このガス拡
散制御層20の素材としては、たとえばムライト、スピ
ネル、フオルステライト、カルシウムジルコネートなど
を使用することができ、粉末を用いたスクリーン印刷法
や溶射法などによって積層する。このとき、後述するよ
うにガス拡散制御層20の酸素分子に関する拡散係数を
上記溶射条件等によって選定しうるようにする。そこで
、上記酸素センサ素子10を用い、直流電源18の正極
側を他方の基準極電子伝導層14に接続して電流を供給
すると、前記測定極電子伝導層16から基準極電子伝導
層14に向けて強制的に酸素イオンの移動を生ずる。こ
のとき、ガス拡散制御層20の存在によって被検ガスか
らの酸素分子の流入拡散が制御されているため、測定極
酸素分圧は被検ガス中の酸素分圧よりも低下する。他方
、基準極電子伝導層14に向けて酸素イオンが流れるこ
とにより基準極酸素分圧が高められるが、この基準極電
子伝導層14に存在する酸素分子は、隔膜層11が多孔
性の場合に前記隔膜層11内を拡散して、あるいは隅膜
層11がち密で固体電解質層15が多孔性の場合に前記
固体電解質層15内を拡散して、もしくは両方を拡散し
て、前記酸素イオンの流入と前記酸素分子の拡散との均
衡した状態の基準極酸素分圧が維持される。そこで、前
記被検ガス中の酸素分圧よりも低下した測定極酸素分圧
と上記基準極酸素分圧との差に対応して発生する起電力
Eを電圧測定手段17によって測定すれば、前記測定極
酸素分圧が被検ガス中の酸素分圧よりも低下した関係を
維持しつつ被検ガス中の酸素分圧の変化に応じて上記測
定極酸素分圧も変化するために、理論空燃比よりも希薄
な空燃比の検出が可能になる。以下、これをさらに第8
図をもとにして詳細に説明する。第8図はこの発明の空
燃比検出方法の実施に用いられる酸素センサ素子の作用
的断面説明図であって、この場合には、酸素に関する拡
散係数がk,である多孔質隔膜層11、基準極電子伝導
層14、固体電解質層15、測定極電子伝導層16、酸
素に関する拡散係数がk2である拡散層20を順次積層
した状態を示している。そこで、直流電源18を接続し
て基準極電子伝導層14から測定極電子伝導層16に向
けて直流電流1を流し込むと、第8図にすように、固体
電解質層15内で測定極電子伝導層16から基準極電子
伝導層14向けて酸素分子がイオンの形でQ(mol/
sec)だけ送り込まれ、Q=1/岬の関係で示される
。また、被検ガス中の酸素分圧をPとすると、測定極電
子伝導層16における酸素分圧P2は、Q=k2(P−
P2) …・・・‘21なる関係式から
、P2=P−Q/k2 ・・・・・・
‘3}で表わされる。On the surface of this diaphragm layer 11, two reference electrode electron conductive layers 13 and 14 are laminated, and an oxygen ion conductive solid electrolyte layer 15 is further laminated thereon. As the material for this solid electrolyte layer 15, Y203, Cao-stabilized Z2, and other known materials can be used. A measurement electrode electron conduction layer 16 is provided on the surface of this solid electrolyte layer 15, and a voltage measuring means 17 is connected between the measurement electrode electron conduction layer 16 and the reference electrode electron conduction layer 13. In addition to making it possible to measure the power E, the measurement electrode electron conductive layer 1
6 and the other reference electrode electron conductive layer 14, a DC power source 18 is connected. At this time, the reference electrode electron conductive layer 13,
14 and the measurement electrode electron conductive layer 16 are preferably made of catalytically active platinum, and in addition, alloys of platinum and platinum group elements and other materials are preferably selected and used as appropriate. Further, when laminating the electron conductive layers 13, 14, 16 and the solid electrolyte layer 15, for example, a method may be used in which powders thereof are made into a paste, printed on a screen, and then baked, or other methods may be used. It is also possible to do so by means. Further, a heating power source 19 is connected to the heating element 12 so that the temperature of the oxygen sensor element can be controlled. Furthermore, a gas diffusion control layer 20 capable of controlling the diffusion of oxygen molecules flowing from the test gas is provided on the measurement electrode electron conduction layer 16, and this gas diffusion control layer 20 is made to be in contact with the test gas. There is. In this case, the gas diffusion control layer 20
As shown in the examples below, the gas diffusion coefficient is 6×10-9 and 2×10-7 mole/atm
・It is better to set it within the range of sec. The material for the gas diffusion control layer 20 can be, for example, mullite, spinel, forsterite, calcium zirconate, etc., and is laminated by a screen printing method using powder, a thermal spraying method, or the like. At this time, as will be described later, the diffusion coefficient of the gas diffusion control layer 20 for oxygen molecules can be selected based on the thermal spraying conditions and the like. Therefore, when using the oxygen sensor element 10 and connecting the positive electrode side of the DC power source 18 to the other reference electrode electron conductive layer 14 and supplying current, the current is directed from the measurement electrode electron conductive layer 16 to the reference electrode electron conductive layer 14. This forces the movement of oxygen ions. At this time, since the inflow and diffusion of oxygen molecules from the test gas is controlled by the presence of the gas diffusion control layer 20, the measured polar oxygen partial pressure is lower than the oxygen partial pressure in the test gas. On the other hand, the oxygen partial pressure at the reference electrode is increased by the flow of oxygen ions toward the reference electrode electron conductive layer 14, but the oxygen molecules present in the reference electrode electron conductive layer 14 are The oxygen ions are diffused within the diaphragm layer 11, or when the corneal membrane layer 11 is dense and the solid electrolyte layer 15 is porous, the oxygen ions are diffused within the solid electrolyte layer 15, or both. A reference polar oxygen partial pressure is maintained in which the inflow and the diffusion of the oxygen molecules are balanced. Therefore, if the voltage measuring means 17 measures the electromotive force E generated in response to the difference between the measured polar oxygen partial pressure, which is lower than the oxygen partial pressure in the test gas, and the reference polar oxygen partial pressure, While maintaining a relationship in which the measured polar oxygen partial pressure is lower than the oxygen partial pressure in the test gas, the measured polar oxygen partial pressure changes in response to changes in the oxygen partial pressure in the test gas, so the theoretical It becomes possible to detect an air-fuel ratio that is leaner than the fuel ratio. Below, this will be further explained in the 8th section.
This will be explained in detail based on the figures. FIG. 8 is an explanatory functional cross-sectional diagram of an oxygen sensor element used in carrying out the air-fuel ratio detection method of the present invention, and in this case, a porous diaphragm layer 11 whose diffusion coefficient for oxygen is k, a reference A state in which a polar electron conductive layer 14, a solid electrolyte layer 15, a measurement polar electron conductive layer 16, and a diffusion layer 20 having a diffusion coefficient for oxygen of k2 are laminated in this order is shown. Therefore, when the DC power supply 18 is connected and a DC current 1 is applied from the reference electrode electron conduction layer 14 to the measurement electrode electron conduction layer 16, as shown in FIG. Q (mol/
sec) and is expressed by the relationship Q=1/Cape. Furthermore, if the oxygen partial pressure in the test gas is P, then the oxygen partial pressure P2 in the measurement electrode electron conductive layer 16 is Q=k2(P−
P2) ......From the relational expression '21, P2=P-Q/k2...
'3}.
ところで、被検ガスたとえばガソリン内燃機関の排ガス
中の酸素分圧Pと空燃比(A/F)との関係は、第9図
に示す如く、理論空燃比(約14.7)付近から次第に
酸素分圧Pが高くなる。また、前記Q=1/小の関係か
ら、上記式(3’‘ま、P2=P−1/(4F・k2)
……【4)という関係で表わされ、電流1お
よび拡散係数k2を適当な値に選定することによって、
測定極酸素分圧P2と空燃比(A/F)との関係をたと
えば第10図に示すように空燃比(A/F)=16付近
まで測定極酸素分圧P2がほぼ0となるようにすること
ができる。By the way, the relationship between the oxygen partial pressure P in the test gas, for example, the exhaust gas of a gasoline internal combustion engine, and the air-fuel ratio (A/F) is as shown in FIG. Partial pressure P increases. Also, from the relationship of Q=1/small, the above formula (3'', P2=P-1/(4F・k2)
...It is expressed by the relationship [4], and by selecting appropriate values for the current 1 and the diffusion coefficient k2,
For example, as shown in Fig. 10, the relationship between the measured polar oxygen partial pressure P2 and the air-fuel ratio (A/F) is such that the measured polar oxygen partial pressure P2 becomes almost 0 until the air-fuel ratio (A/F) = 16. can do.
換言すれば、測定極酸素分圧P2を排ガス中の酸素分圧
Pよりも低下させることができる。他方、基準極電子伝
導層14における基準極酸素分圧P,は、Q=k,(P
,一P) ……【5’なる関係式からP
,=Q/k,十P …・・・(6}で
表わされる。In other words, the measured polar oxygen partial pressure P2 can be made lower than the oxygen partial pressure P in the exhaust gas. On the other hand, the reference electrode oxygen partial pressure P, in the reference electrode electron conductive layer 14 is Q=k, (P
, 1P) ...[From the relational expression 5', P
, =Q/k, 10P......(6}).
そこで、隔膜層11の拡散係数k,を小さくすればP,
》》Pであり、上記式■はP,=Q/k,
……{7}となる。また、もう一方の基準極電
子伝導層13の基準極酸素分圧P.′はほぼ酸素分圧P
,に等しいので、前記式{7雌P,′=Q/k.
・・・・・・(8}となる。Therefore, by decreasing the diffusion coefficient k, of the diaphragm layer 11, P,
》》P, and the above formula ■ is P, = Q/k,
...{7}. Further, the reference electrode oxygen partial pressure P. of the other reference electrode electron conductive layer 13 is ' is approximately the oxygen partial pressure P
, so the above formula {7feP,'=Q/k.
......(8}.
以上の関係より、第8図に示す酸素センサ素子の起電力
Eは、前記式‘1}と同様に、E=−帯1帯/
.・…側
で表わされ、
E:−帯nP扇Q声K2 .・…側
あるいは
E=−帯ln午糸貴転学 側(・・)
で表わされる。From the above relationship, the electromotive force E of the oxygen sensor element shown in FIG.
..・Represented by the side, E:-band nP fan Q voice K2 .・It is represented by the side or E=-obi ln no go itoki tengaku side (...).
そこで、前記{4}式をもとに述べたように、電流1お
よび拡散係数k2を適当な値に選定することによって第
10図に示す如く空燃比(A/F)=16付近まで測定
極酸素分圧P2がほぼ0になるようにし、一方、前記式
‘8)に示すP,′=Q/k,の関係においてP,′が
10‐latm程度となるように拡散係数k,を調整し
ておけば、前記式‘9}の関係から酸素センサ素子の起
電力Eと空燃比(A/F)との関係は、第11図に示す
如く空燃比(A/F)=16を境いに急激に変化する特
性を示し、したがって、理論空燃比(A/F=14.7
)よりも希薄な空燃比(A/F=16)の検出が可能に
なる。Therefore, as described based on the above formula {4}, by selecting appropriate values for the current 1 and the diffusion coefficient k2, the measurement electrode can be adjusted up to the air-fuel ratio (A/F) = 16 as shown in Figure 10. Adjust the oxygen partial pressure P2 to approximately 0, and adjust the diffusion coefficient k so that P,' is approximately 10-latm in the relationship P,' = Q/k, shown in equation '8) above. Then, from the relationship of Equation '9} above, the relationship between the electromotive force E of the oxygen sensor element and the air-fuel ratio (A/F) will be determined as shown in FIG. Therefore, the stoichiometric air-fuel ratio (A/F=14.7
), it becomes possible to detect an air-fuel ratio (A/F=16) that is leaner than that of A/F=16.
なお、前記式より明らかな如く、電流1を増加すれば、
起電力Eが急激に変化する空燃比(A/F)はより希薄
側にずれ、ガス拡散制御層20の拡散係数k2を小さく
した場合にも同様に起電力Eが急激に変化する空燃比(
A/F)はより希薄側にずれる。Furthermore, as is clear from the above formula, if the current 1 is increased,
The air-fuel ratio (A/F) at which the electromotive force E changes rapidly shifts to the leaner side, and even when the diffusion coefficient k2 of the gas diffusion control layer 20 is made smaller, the air-fuel ratio (A/F) at which the electromotive force E changes rapidly also shifts to the leaner side.
A/F) shifts to the leaner side.
なお、第5図に示す酸素センサ素子10では、二つに分
けた基準極電子伝導層13,14を設け、一方を電圧測
定手段17に接続し、他方を直流電源18に接続してい
る。In the oxygen sensor element 10 shown in FIG. 5, two reference electrode electron conductive layers 13 and 14 are provided, one of which is connected to a voltage measuring means 17 and the other to a DC power source 18.
これは、直流電源18の影響が電圧測定手段17の出力
電圧に影響を及ぼさないようにするためである。すなわ
ち、固体電解質層15の内部抵抗は温度が低下した場合
に増大するために、直流電源18を接続して電流を流す
ことによって両電子伝導層14,16間における電圧が
増大し、基準極電子伝導層13,14が共通の場合には
起電力に上記電圧が加算されて出力電圧が増大して正常
な起電力を測定しがた〈なるためである。また、発熱体
12を設けて酸素センサ素子10の温度を一定(約60
0qo)に保つのは、上記直流電源18からの電流1を
流しやすくするため、ならびに隔膜層11の拡散係数k
.およびガス拡散制御層20の拡散係数k2を一定に保
つためである。This is to prevent the influence of the DC power supply 18 from affecting the output voltage of the voltage measuring means 17. That is, since the internal resistance of the solid electrolyte layer 15 increases when the temperature decreases, by connecting the DC power supply 18 and flowing a current, the voltage between the two electron conductive layers 14 and 16 increases, and the reference electrode electron This is because if the conductive layers 13 and 14 are common, the above voltage is added to the electromotive force and the output voltage increases, making it difficult to measure a normal electromotive force. In addition, a heating element 12 is provided to keep the temperature of the oxygen sensor element 10 constant (approximately 60°C).
The purpose of keeping the current 1 from the DC power source 18 at
.. This is also to keep the diffusion coefficient k2 of the gas diffusion control layer 20 constant.
次に、この発明の実施の一例を示す。表1は酸素センサ
素子10の仕様を示すものである。表1また、表2は温
度60000における酸素に関する拡散係数を示すもの
であり、電流1=500山Aとしたときの起電力Eが急
激に変化する空燃比(A/F)もあわせて示した。Next, an example of implementing the present invention will be shown. Table 1 shows the specifications of the oxygen sensor element 10. Table 1 Table 2 also shows the diffusion coefficient for oxygen at a temperature of 60,000, and also shows the air-fuel ratio (A/F) at which the electromotive force E suddenly changes when the current 1 = 500 peaks A. .
なお、電子伝導層13,14,16の拡散係数k3は、
電子伝導層内における酸素分圧を均一なものとするため
に、ガス拡散制御層20の拡散係数に比べて箸るしく大
きい値であることが必要である。表2
表2に示すように、電流1=500仏A、隔膜層1 1
の拡散係数k.=6×10−9mole/atm・se
c、ガス拡散制御層20の拡散係数k2=6×lo‐8
moleノ′at′m・secとしたときに空燃比(A
/F)=16で起電力Eが急激に変化する特性を示すが
、さらに電流1=750仏Aおよび1000仏Aと変化
した場合には、第12図に示すように、起電力Eが急激
に変化する空燃比(A/F)も変化する。Note that the diffusion coefficient k3 of the electron conductive layers 13, 14, and 16 is
In order to make the oxygen partial pressure in the electron conductive layer uniform, it is necessary that the diffusion coefficient be significantly larger than the diffusion coefficient of the gas diffusion control layer 20. Table 2 As shown in Table 2, current 1 = 500 A, diaphragm layer 1 1
The diffusion coefficient k. =6×10-9mole/atm・se
c, diffusion coefficient k2 of gas diffusion control layer 20=6×lo-8
The air-fuel ratio (A
/F) = 16, the electromotive force E exhibits a characteristic of rapid change, but when the current 1 further changes to 750 and 1000 A, the electromotive force E suddenly changes as shown in Figure 12. The air-fuel ratio (A/F) also changes.
したがって、単一の酸素センサ素子10を便用した内燃
機関の空燃比制御において、内燃機関の出力をあまり低
下させたくないとき(例えば登板時)には上記電流を相
対的に小さくし、出力をあまり必要としない場合(例え
ば定速走行時)に希薄燃焼させて燃料消費効率を高めた
いときには上記電流を相対的に大きくするというような
制御をおこなえば好都合である。なお、従来の酸素セン
サ素子において、測定極電子伝導層の表面に保護層を設
ける場合もあるが、このとき、理論空燃比において起電
力Eが急激に変化する酸素センサ素子を前記表1に示す
寸法で製造した場合には、保護層の拡散係数をk=1×
10‐6mole/atm・sec程度よりも大きくす
る必要があった。Therefore, in air-fuel ratio control of an internal combustion engine using a single oxygen sensor element 10, when it is not desired to reduce the output of the internal combustion engine too much (for example, when climbing up a hill), the above-mentioned current is made relatively small to reduce the output. When it is desired to increase fuel consumption efficiency by performing lean combustion when the fuel is not needed so much (for example, when driving at a constant speed), it is convenient to perform control such that the current is relatively increased. In addition, in some conventional oxygen sensor elements, a protective layer is provided on the surface of the measurement electrode electron conductive layer. When manufactured with dimensions, the diffusion coefficient of the protective layer is k=1×
It was necessary to make it larger than about 10-6 mole/atm·sec.
すなわち、保護層を設けるのはあくまで酸素センサ素子
本体を保護するためであり、保護層において酸素分圧の
勾配を生ずると理論空燃比の検出ができなくなるので、
保護層の拡散係数の値を上述の如くある程度以上に大き
くしておく必要がある。一方、この発明による酸素セン
サ素子10では、表1で示す寸法で製造した場合に、ガ
ス拡散制御層20の拡散係数k2=2×10‐7mol
e/atm・sec程度以下の比較的小さな値とし、ガ
ス拡散制御層201こおいて酸素分圧の勾配を生じさせ
るようにして希薄空燃比の検出を可能としている。In other words, the purpose of providing the protective layer is to protect the main body of the oxygen sensor element, and if a gradient of oxygen partial pressure occurs in the protective layer, the stoichiometric air-fuel ratio cannot be detected.
As mentioned above, the value of the diffusion coefficient of the protective layer needs to be larger than a certain level. On the other hand, in the oxygen sensor element 10 according to the present invention, when manufactured with the dimensions shown in Table 1, the diffusion coefficient k2 of the gas diffusion control layer 20 is 2×10-7 mol.
The value is set to a relatively small value of approximately e/atm·sec or less, and a gradient of oxygen partial pressure is generated in the gas diffusion control layer 201, thereby making it possible to detect a lean air-fuel ratio.
しかしながら、拡散係数k2が小さければ良いとうこと
でもなく、6×10‐9mole/atm・sec程度
よりも小さくなると応答性に悪影響を及ぼすようになる
。したがって、表1に示す寸法のものにおいては、ガス
拡散制御層20の拡散係数k2がおよそ6×10‐9な
し、し2×10‐7mole/atm・secの範囲と
なるようにするのがよいといえる。以上のように、この
発明によれば、測定極電子伝導層の表面に、酸素に関す
る拡散係数が所定の範囲内にあって酸素分子の拡散を制
御しうるガス拡散制御層を設けて被検ガスと接触可能に
した酸素センサ素子を用い、直流電源により供給される
電流によって測定極電子伝導層から基準極電子伝導層に
向けて酸素イオンの移動を生じさせることにより前記測
定極酸素分圧を被検ガス中の酸素分圧よりも低下させ、
前記低下させた測定極酸素分圧と基準極酸素分圧との差
に対応して発生する起電力を測定するようにしたから、
理論空燃比よりも希薄な空燃比の検出が可能であり、た
とえば内燃機関等において希薄燃焼を可能にして燃料消
費効率を高めることができるなどの非常にすぐれた効果
をもたらす。However, it is not necessarily the case that the diffusion coefficient k2 is small, and if it becomes smaller than about 6×10 −9 mole/atm·sec, it will adversely affect the response. Therefore, in the case of the dimensions shown in Table 1, it is preferable that the diffusion coefficient k2 of the gas diffusion control layer 20 is in the range of approximately 6×10-9 to 2×10-7 mole/atm·sec. It can be said. As described above, according to the present invention, a gas diffusion control layer having a diffusion coefficient for oxygen within a predetermined range and capable of controlling the diffusion of oxygen molecules is provided on the surface of the measurement electrode electron conductive layer to The oxygen partial pressure at the measurement electrode is applied by using an oxygen sensor element which can be brought into contact with the oxygen sensor element, and by causing the movement of oxygen ions from the measurement electrode electron conduction layer to the reference electrode electron conduction layer by means of a current supplied by a DC power source. lower than the oxygen partial pressure in the sample gas,
Since the electromotive force generated in response to the difference between the reduced measured polar oxygen partial pressure and the reference polar oxygen partial pressure is measured,
It is possible to detect an air-fuel ratio that is leaner than the stoichiometric air-fuel ratio, and brings about extremely excellent effects such as enabling lean combustion in internal combustion engines and the like, thereby increasing fuel consumption efficiency.
第1図は従来の空燃比検出に使用される酸素センサ素子
の断面説明図、第2図は空燃比と排ガス中の酸素濃度と
の関係を示すグラフ、第3図は空燃比と第1図の酸素セ
ンサ素子の測定極酸素分圧との関係を示すグラフ、第4
図は空燃比と第1図の酸素センサ素子の起電力との関係
を示すグラフ、第5図および第6図はこの発明の一実施
例における空燃比検出に使用される酸素センサ素子のそ
れぞれ縦断面模型的結線図および分解斜視図、第7図は
第5図の酸素センサ素子の発熱体部分の説明図、第8図
は第5図の酸素センサ素子の作用を示す拡大断面説明図
、第9図は空燃比と被f余ガス中の酸素分圧との関係を
示すグラフ、第10図は空燃比と第5図の酸素センサ素
子の測定極酸素分圧との関係を示すグラフ、第11図は
空燃比と第5図の酸素センサ素子の起電力との関係を示
すグラフ、第12図は電流を変化させた場合の空燃比と
酸素センサ素子の起電力との関係を示すグラフである。
10・・・…酸素センサ素子、11・・・・・・隅膜層
、13,14・・・・・・基準極電子伝導層、15・…
・・酸素イオン伝導性固体電解質層16・・・・・・測
定極電子伝導層、17・・・・・・電圧測定手段、18
・・・・・・直流電源、20・・・・・・ガス拡散制御
層。第1図
第2図
第3図
第4図
第5図
第6図
第7図
第8図
第9図
第10図
第11図
第12図Figure 1 is a cross-sectional explanatory diagram of an oxygen sensor element used for conventional air-fuel ratio detection, Figure 2 is a graph showing the relationship between air-fuel ratio and oxygen concentration in exhaust gas, and Figure 3 is a graph showing the relationship between air-fuel ratio and Figure 1. Graph showing the relationship between the oxygen sensor element and the measured polar oxygen partial pressure, 4th
The figure is a graph showing the relationship between the air-fuel ratio and the electromotive force of the oxygen sensor element shown in FIG. 7 is an explanatory diagram of the heating element portion of the oxygen sensor element in FIG. 5; FIG. 8 is an enlarged sectional explanatory diagram showing the action of the oxygen sensor element in FIG. 5; Figure 9 is a graph showing the relationship between the air-fuel ratio and the oxygen partial pressure in the residual gas; Figure 10 is a graph showing the relationship between the air-fuel ratio and the polar oxygen partial pressure measured by the oxygen sensor element in Figure 5; Figure 11 is a graph showing the relationship between the air-fuel ratio and the electromotive force of the oxygen sensor element shown in Figure 5, and Figure 12 is a graph showing the relationship between the air-fuel ratio and the electromotive force of the oxygen sensor element when the current is changed. be. 10... Oxygen sensor element, 11... Corneal membrane layer, 13, 14... Reference electrode electron conductive layer, 15...
... Oxygen ion conductive solid electrolyte layer 16 ... Measurement electrode electron conductive layer, 17 ... Voltage measuring means, 18
...DC power supply, 20... Gas diffusion control layer. Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 6 Figure 7 Figure 8 Figure 9 Figure 10 Figure 11 Figure 12
Claims (1)
電解質層および測定極電子伝導層を積層し、前記隔膜層
および酸素イオン伝導性固体電解質層のうち少なくとも
いずれか一方がガス透過性であり、前記基準極電子伝導
層と測定電子伝導層との間に直流電源を接続する酸素セ
ンサ素子の前記測定極電子伝導層の表面に、酸素に関す
る拡散係数が6×10^−^9ないし2×10^−^7
mole/atm・secの範囲であつて酸素分子の拡
散を制御しうるガス拡散制御層を設けて被検ガスと接触
可能にした酸素センサ素子を用い、前記直流電源により
供給される電流によて前記測定電子伝導層から基準極電
子伝導層に向けて酸素イオンの移動を生じさせることに
より前記測定極酸素分圧を前記被検ガス中の酸素分圧よ
りも低下させ、前記低下させた測定極酸素分圧と基準極
酸素分圧との差に対応して発生する起電力を測定するこ
とによつて理論空燃比よりも希薄な空燃比の検出を可能
にしたことを特徴とする空燃比検出方法。 2 基準極電子伝導層を二つお電子伝導層から形成し、
一方の基準極電子伝導層と測定極電子伝導層との間に起
電力の測定手段を接続すると共に、他方の基準極電子伝
導層と測定極電子伝導層との間に直流電源を接続した特
許請求の範囲第1項記載の空燃比検出方法。 3 隔膜層に多孔性物質を用いて酸素分子の拡散を可能
にした特許請求の範囲第1項または第2項記載の空燃比
検出方法。[Scope of Claims] 1. A diaphragm layer, a reference electrode electron conductive layer, an oxygen ion conductive solid electrolyte layer, and a measurement electrode electron conductive layer are laminated, and at least one of the diaphragm layer and the oxygen ion conductive solid electrolyte layer is laminated. is gas permeable, and the surface of the measurement electrode electron conduction layer of the oxygen sensor element, in which a DC power source is connected between the reference electrode electron conduction layer and the measurement electrode electron conduction layer, has a diffusion coefficient of 6×10^ for oxygen. -^9 or 2×10^-^7
An oxygen sensor element is provided with a gas diffusion control layer capable of controlling the diffusion of oxygen molecules in the range of mole/atm sec, and is capable of contacting the test gas, and is operated by the current supplied by the DC power supply. The measurement electrode oxygen partial pressure is lowered than the oxygen partial pressure in the test gas by causing the movement of oxygen ions from the measurement electron conduction layer toward the reference electrode electron conduction layer, and the reduced measurement electrode Air-fuel ratio detection characterized by making it possible to detect an air-fuel ratio leaner than the stoichiometric air-fuel ratio by measuring the electromotive force generated in response to the difference between the oxygen partial pressure and the reference polar oxygen partial pressure. Method. 2. Forming a reference electrode electron conductive layer from two electron conductive layers,
A patent in which an electromotive force measuring means is connected between one reference electrode electron conductive layer and a measurement electrode electron conductive layer, and a DC power source is connected between the other reference electrode electron conductive layer and the measurement electrode electron conductive layer. An air-fuel ratio detection method according to claim 1. 3. The air-fuel ratio detection method according to claim 1 or 2, wherein a porous material is used in the diaphragm layer to enable diffusion of oxygen molecules.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP54164822A JPS6034065B2 (en) | 1979-12-20 | 1979-12-20 | Air fuel ratio detection method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP54164822A JPS6034065B2 (en) | 1979-12-20 | 1979-12-20 | Air fuel ratio detection method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5689051A JPS5689051A (en) | 1981-07-20 |
| JPS6034065B2 true JPS6034065B2 (en) | 1985-08-06 |
Family
ID=15800569
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP54164822A Expired JPS6034065B2 (en) | 1979-12-20 | 1979-12-20 | Air fuel ratio detection method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6034065B2 (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5934442A (en) * | 1982-08-23 | 1984-02-24 | Hitachi Ltd | Air-fuel ratio feedback controller |
| JPS61129445A (en) * | 1984-11-26 | 1986-06-17 | Nissan Motor Co Ltd | Air fuel ratio controller |
| JP5867357B2 (en) * | 2012-02-03 | 2016-02-24 | 株式会社デンソー | Exhaust gas purification device for internal combustion engine |
| JP5904172B2 (en) * | 2013-08-09 | 2016-04-13 | 株式会社デンソー | Gas sensor control device |
-
1979
- 1979-12-20 JP JP54164822A patent/JPS6034065B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5689051A (en) | 1981-07-20 |
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