TW201033597A - Engine load detection apparatus and engine load detection method - Google Patents

Engine load detection apparatus and engine load detection method Download PDF

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Publication number
TW201033597A
TW201033597A TW098138398A TW98138398A TW201033597A TW 201033597 A TW201033597 A TW 201033597A TW 098138398 A TW098138398 A TW 098138398A TW 98138398 A TW98138398 A TW 98138398A TW 201033597 A TW201033597 A TW 201033597A
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Taiwan
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engine
average
section
rotation speed
load
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TW098138398A
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Chinese (zh)
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TWI464379B (en
Inventor
Yoichi Takahashi
Shiro Kokubu
Naohisa Okawada
Ryosuke Ibata
Kenji Nishida
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Honda Motor Co Ltd
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    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02TCLIMATE CHANGE MITIGATION TECHNOLOGIES RELATED TO TRANSPORTATION
    • Y02T10/00Road transport of goods or passengers
    • Y02T10/10Internal combustion engine [ICE] based vehicles
    • Y02T10/40Engine management systems

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  • Combined Controls Of Internal Combustion Engines (AREA)
  • Electrical Control Of Ignition Timing (AREA)

Abstract

Provided is an engine load detection apparatus which has considered the rotary variation of the engine and has reduced the affection of dimensional tolerance of the pulse rotor, and can detect more correctly engine load state. In the present invention, the detection interval for detecting average engine rotary speed (NeA) is setup as a length of crankshaft rotating two loops starting from the begin point (G3) of the second magnetic drag rotor (12). The detection interval is divided into four intervals, the four intervals are composed of a first magnetic drag rotor and a second magnetic drag rotor interval corresponding to the position that the second magnetic drag rotor (12) passing through the pick-up device (20), and a first interval and a second interval corresponding to the position that the second magnetic drag rotor (12) not passing through. The first mean value (H1) of averaging the first rotary speed <omega>4 (n-1) and the second rotary speed <omega>4 (n) is calculated, and the second mean value (H2) of averaging the first magnetic drag rotor rotary speed <omega> tdc1 and the second magnetic drag rotor rotary speed <omega> tdc2 is calculated. Then, the NeA is obtained by dividing the first mean value (H1) from the value of the first rotary speed <omega> 4(n-1) and then multiplying the second mean value (H2).

Description

201033597 六、發明說明: 【發明所屬之技術領域】 本發明是關於引擎負載檢測裝置及引擎負載檢測方法 ,特別是根據「與曲柄軸同步旋轉」之脈衝轉子的輸出訊 號,來檢測引擎之負載狀態的引擎負載檢測裝置及引擎負 載檢測方法。 9 【先前技術】 傳統以來,具備「與引擎的曲柄軸同步旋轉」的脈衝 轉子、及檢測「被設在該脈衝轉子之磁阻的通過狀態」的 拾取器線圈,並根據由該拾取器線圈所輸出的脈衝訊號, 來檢測引擎之負載狀態的引擎負載檢測裝置已爲大眾所知 悉。 在專利文獻1中揭示一種技術:將脈衝轉子的磁阻設 在「對應於引擎之上死點」的位置附近,且於每旋轉1次 ® 或每旋轉2次時,計算脈衝轉子旋轉1次的時間與磁阻通 過的時間之比率,並根據該比率的變動程度來檢測引擎的 負載狀態。 [專利文獻] [專利文獻1]日本特開2002-115598號公報 【發明內容】 [發明欲解決之課題] 話雖如此’專利文獻1所記載的技術,是用來檢測以 -5&quot; 201033597 「曲柄軸旋轉1次期間所需的時間」作爲基準之磁阻的通 過時間,並未考慮以更長的區間,譬如以「曲柄軸旋轉2 次期間所需的時間」作爲基準,來檢測更適切的負載狀態 。不僅如此,即使是曲柄軸旋轉1次期間,也未對應於4 行程引擎的4個行程(進氣、壓縮、燃燒一膨脹、排氣)來 檢討引擎旋轉速度的變動。 此外,由於專利文獻1所記載的技術,是用來檢測以 「曲柄軸旋轉1次期間所需的時間」作爲基準之磁阻的通 @ 過時間,因此一旦磁阻之圓周方向的長度等存有「因尺寸 公差所衍生的尺寸偏移」時,計算所得的比率也可能殘存 有尺寸公差的影響,而具有無法正確地檢測引擎之負載狀 態的可能性。此外,曲柄軸的旋轉速度(角速度),容易受 到「從曲柄軸到後輪爲止」之扭力傳動系統的影響,這點 已爲大眾所知悉,因此,期待一種考慮到上述狀況且能計 算負載計算的構造。 本發明的目的是提供一種:能解決上述習知技術的課 @ 題,考慮到因應於4行程引擎之4個行程所產生的旋轉變 動,且降低脈衝轉子之尺寸公差的影響,而能更正確地檢 測引擎之負載狀態的負載檢測裝置及負載檢測方法。 [解決課題手段] 爲了達成前述目的,本發明是具備:脈衝轉子,該脈 衝轉子是與引擎的曲柄軸同步旋轉;和磁阻,該磁阻被設 在該脈衝轉子,並位在對應於前述引擎之上死點附近的曲 -6- 201033597 柄角度;及拾取器,該拾取器是用來檢測該磁阻的 並根據該拾取器的輸出訊號,來檢測引擎之負載狀 擎負載檢測裝置,本發明的第1特徵爲具備:將用 平均引擎旋轉速度的特定區間分割成複數,並根據 取器的輸出訊號,分別計算該經分割的複數個區間 區間的引擎旋轉速度的手段;和加權手段,該加權 對前述複數個區間的引擎旋轉速度執行不同的加權 • 及負載狀態計算手段,該負載狀態計算手段是根據 理後之複數區間引擎旋轉速度的平均値,計算前述 擎旋轉速度,並使用該該平均引擎旋轉速度來執行 負載狀態的計算。 此外,第2特徵爲以下的技術點:前述加權處 在前述被分割成複數的區間中,將包含燃燒-膨脹 區間的加權比率,設定成較其他區間更大。 此外,第3特徵爲以下的技術點:前述特定區 Φ 根據前述脈衝轉子的輸出訊號所偵測。 此外,第4特徵爲以下的技術點:前述特定區 將前述曲柄軸之2次旋轉量的長度2等分爲第1區 2區間,並設定成前述第1區間包含進氣行程,前 區間包含燃燒-膨脹行程。 此外,第5特徵爲以下的技術點:前述引擎的 態,是「前述磁阻通過前述拾取器期間」的旋轉速 以前述平均引擎轉數所算出的負載率。 此外,第6特徵爲以下技術點:前述磁阻是被 通過; 態的引 來檢測 前述拾 之各個 手段是 處理; 加權處 平均引 引擎之 理,是 行程之 間,是 間,是 間與第 述第2 負載狀 度,除 配設在 201033597 即將到達引擎上死點時的位置,前述負載率,是採用「在 即將到達壓縮側的上死點時,前述磁阻通過前述拾取器期 間」的旋轉速度所算出。 此外’第7、8特徵爲以下的技術點:對應於前述所 算出的負載率,至少對前述引擎的點火時期進行反饋控制 〇 此外,本發明是具備:脈衝轉子,該脈衝轉子是與引 擎的曲柄軸同步旋轉;和磁阻,該磁阻被設在該脈衝轉子 @ ,並位在對應於前述引擎之上死點附近的曲柄角度;及拾 取器,該拾取器是用來檢測該磁阻的通過;並根據該拾取 器的輸出訊號,來檢測引擎之負載狀態的引擎負載檢測方 法,本發明的第9特徵爲以下的技術點:在計算檢測前述 引擎的負載狀態之際所採用的平均引擎旋轉速度時,具備 :將用來檢測前述平均引擎旋轉速度的特定區間分割成複 數的步驟;和用來計算前述經分割之複數個區間的各個區 間引擎旋轉速度的步驟;和對前述複數個區間引擎旋轉速 @ 度執行不同加權處理的步驟;及藉由求出前述加權處理後 之複數個區間引擎旋轉速度的平均値,來計算前述平均引 擎旋轉速度的步驟。 此外,本發明是具備:脈衝轉子,該脈衝轉子是與引 擎的曲柄軸同步旋轉;和磁阻,該磁阻被設在該脈衝轉子 ,並位在對應於前述引擎之上死點附近的曲柄角度;及拾 取器,該拾取器是用來檢測該磁阻的通過;並根據該拾取 器的輸出訊號,來檢測引擎之負載狀態的引擎負載檢測裝 -8- 201033597 置,本發明的第10特徵爲以下的技術點:將用來檢測平 均引擎旋轉速度的檢測區間,設定成從前述磁阻的通過開 始點起計算的前述曲柄軸之2次旋轉量的長度,前述檢測 區間設成由以下所形成的4個區間:第1磁阻區間與第2 磁阻區間,該第1磁阻區間與第2磁阻區間是分別對應於 在前述曲柄軸之2次旋轉的每一次旋轉中,前述磁阻通過 前述拾取器的位置;及第1區間與第2區間,該第1區間 φ 與第2區間是分別對應於前述磁阻未通過前述拾取器的位 置;本發明的引擎負載檢測裝置具備:求取第1平均値的 手段,該第1平均値是由前述第1區間所檢測的第1旋轉 速度、與由前述第2區間所檢測之第2旋轉速度的平均値 :和求取第2平均値的手段,該第2平均値爲由前述第1 磁阻區間所檢測的第1磁阻旋轉速度、與由前述第2磁阻 區間所檢測之第2磁阻旋轉速度的平均値;和計算前述平 均引擎旋轉速度的手段,該前述平均引擎旋轉速度是藉由 ® 對前述第1平均値除以前述第1旋轉速度的値,乘以前述 第2平均値所求出;及負載狀態計算手段,該負載狀態計 算手段是使用前述平均引擎旋轉速度來計算前述引擎的負 載狀態。 此外,第1 1特徵爲以下的技術點:用來計算前述平 均引擎旋轉速度的手段,是當前述第1旋轉速度以®4(n_l) 表示、前述第2旋轉速度以ω4(η)表示、前述第1磁阻旋 轉速度以cotdcl表示、前述第2磁阻旋轉速度以c〇tdc2表 示、前述加權處理的加權係數以α表示時,藉由以下的計 -9 - 201033597 算式來計算 [計算式1] NeA' 此外, 第1區間包 行程,當求 速度與前述 權係數α設 此外, 的位置,前 度,除以前 第14 少對前述引 此外, 擎的曲柄軸 ,並位在對 取器,該拾 器的輸出訊 法,本發明 檢測平均引 通過開始點 驟;和將前 前述平均引擎旋轉速度NeA。 _ (ΐ-α)χί〇4 + («-ΐ)+αχβ;4(«) ωίάεΐ + wtdcl ωΑ(η -1) 2 第12特徵爲以下的技術點:被設定成:前述 含進氣行程,且前述第2區間包含燃燒-膨脹 取前述第1平均値之際,是將在前述第1旋轉 第2旋轉速度之間執行不同加權處理的前述加 定成大於〇. 5。 前述磁阻是被配設在即將到達引擎之上死點時 述引擎的負載狀態,是將前述第2磁阻旋轉速 述平均引擎轉數所算出的負載率。 特徵爲以下的技術點:對應於前述負載率,至 擎的點火時期執行反饋控制。 本發明是具備:脈衝轉子,該脈衝轉子是與引 同步旋轉;和磁阻,該磁阻被設在該脈衝轉子 應於前述引擎之上死點附近的曲柄角度;及拾 取器是用來檢測該磁阻的通過;並根據該拾取 號,來檢測引擎之負載狀態的引擎負載檢測方 的第15特徵爲以下的技術點:包含:將用來 擎旋轉速度的檢測區間,設定成從前述磁阻的 起計算之前述曲柄軸的2次旋轉量之長度的步 述檢測區間設成由以下所形成之4個區間的步 -10- 201033597 驟:第1磁阻區間與第2磁阻區間,該第1磁阻區間與第 2磁阻區間是分別對應於在前述曲柄軸之2次旋轉的每一 次旋轉中,前述磁阻通過前述拾取器的位置、和第1區間 與第2區間,該第1區間與第2區間是分別對應於前述磁 阻未通過前述拾取器的位置;和求取第1平均値的步驟’ 該第1平均値是由前述第1區間所檢測的第1旋轉速度、 與由前述第2區間所檢測之第2旋轉速度的平均値;和求 • 取第2平均値的步驟,該第2平均値是由前述第1磁阻區 間所檢測的第1磁阻旋轉速度、與由前述第2磁阻區間所 檢測之第2磁阻旋轉速度的平均値;及計算前述平均引擎 旋轉速度的步驟,該前述平均引擎旋轉速度是藉由對前述 第1平均値除以前述第1旋轉速度的値,再乘以前述第2 平均値所獲得。 此外,本發明是具備:脈衝轉子,該脈衝轉子是與引 擎的曲柄軸同步旋轉;和磁阻,該磁阻被設在該脈衝轉子 ® ,並位在對應於前述引擎之上死點附近的曲柄角度;及拾 取器,該拾取器是用來檢測該磁阻的通過;並根據該拾取 器的輸出訊號,來檢測引擎之負載狀態的引擎負載檢測裝 置,本發明的第1 6特徵爲以下的技術點:具備用來偵測 變速機之變速比的變速比偵測手段,前述引擎的負載狀態 被設成:將前述磁阻通過前述拾取器期間'的旋轉速度,除 以前述平均引擎轉數所算出的負載率,前述磁阻通過前述 拾取器期間的旋轉速度,是根據前述變速比所修正。 此外,第1 7特徵爲以下的技術點:前述變速比偵測 -11 - 201033597 手段,是用來檢測有段變速機之變速檔位的齒輪位置感應 器。 此外,第18特徵爲以下的技術點:前述磁阻通過前 述拾取器期間之旋轉速度的修正,是藉由對該旋轉速度乘 以修正係數的方式所執行,前述修正係數,是當前述有段 變速機的齒輪檔數較低時設定成較大。 不僅如此,第19特徵爲以下的技術點:前述變速比 偵測手段,是根據車速與引擎轉數來求取變速比。 @ [發明效果] 根據第1特徴,由於在計算「用於引擎之負載狀態的 計算」的平均引擎旋轉速度之際,是將用來檢測引擎旋轉 速度的特定區間分割成複數個,並分別計算該經分割之複 數個區間中之每一個區間引擎旋轉速度,而對該複數個區 間引擎旋轉速度執行不同的加權處理,不僅如此,來藉由 求取經該加權處理後之複數個區間引擎旋轉速度的平均値 來計算平均引擎旋轉速度,因此在特定區間内,即使具有 不同於一般運轉時之大量旋轉變動的場合,也能執行已考 慮該旋轉變動的加權,來計算適當的平均引擎旋轉速度。 如此一來,即使在因「加速時或行走於凹凸路面等」而導 致特定區間内之引擎旋轉速度的變動增大的場合中,也能 利用計算來求取對應於上述狀況的引擎負載狀態。 根據第2特徴,由於加權處理,是將被分割成複數個 區間中,含有燃燒-膨脹行程之區間的加權比率設定成大 -12- 201033597 於其他區間,因此即使在因「加速時或行走於凹凸路面等 」,而特別使燃燒-膨脹行程中之引擎旋轉速度的上升程 度變大的場合中,也能利用計算來求取對應於上述狀況的 引擎負載。 根據第3特徴,由於特定區間是根據脈衝轉子的輸出 訊號所檢測,因此可採用檢測「用來驅動引擎的點火裝置 或燃料噴射裝置之時機」的脈衝轉子,設定「用來檢測平 φ 均引擎旋轉速度」的特定區間。如此一來,可在不額外設 置新感應器等的狀態下,利用計算求取引擎負載狀態。 根據第4特徴,由於特定區間是將曲柄軸之2次旋轉 量的長度2等分爲第1區間與第2區間,且設定成第1區 間包含進氣行程,第2區間包含燃燒-膨脹行程,因此能 以簡單的方法執行特定區間的分割。此外,藉由將包含燃 燒-膨脹行程之第2區間的加權設定成較大,能以計算來 求取已考慮了在燃燒-膨脹行程中引擎旋轉速度之變動的 ^ 負載狀態。此外,藉由以最小的分割數來分割特定區間, 既能抑制計算負擔的增加又能獲得加權處理的効果。 根據第5特徴,由於引擎的負載狀態,是藉由將磁阻 通過拾取器期間的旋轉速度除以平均引擎轉數所算出的負 載率,故能藉由簡單的計算式來求取引擎的負載狀態。 根據第6特徴,由於磁阻被配設在即將到達引擎之上 死點時的位置,且負載率是採用「在即將到達壓縮側之上 死點時,磁阻通過拾取器期間之旋轉速度」所算出,因此 可適當地檢測從壓縮行程的尾段到燃燒-膨脹行程期間之 -13- 201033597 大量的引擎旋轉變動,而可求取已考慮了該旋轉變動之引 擎的負載率。 根據第7特徴,由於是對應於所計算的負載率’而至 少對引擎的點火時期執行反饋控制,因此無需額外設置新 的感應器等,僅需採用脈衝轉子的輸出訊號,至少使點火 時期的修正控制變的可能。 根據第8特徴,由於具備:將用來檢測平均引擎旋轉 速度的特定區間分割成複數的步驟;和用來計算經分割之 © 複數個區間的各個區間引擎旋轉速度的步驟;和對複數個 區間引擎旋轉速度執行不同加權處理的步驟;和藉由求出 加權處理後之複數個區間引擎旋轉速度的平均値,來計算 平均引擎旋轉速度的步驟;使用平均引擎旋轉速度來執行 引擎之負載狀態的計算的步驟,因此即使在特定區間的引 擎旋轉速度中,具有不同於一般運轉時的大幅變動時,也 能藉由執行已考慮了該旋轉變動的加權,來計算適當的平 均引擎旋轉速度,並據此來計算引擎的負載狀態。 @ 根據第9特徴,由於將用來檢測平均引擎旋轉速度的 檢測區間,設定成從磁阻的通過開始點起計算的曲柄軸之 2次旋轉量的長度,檢測區間設成由以下所形成的4個區 間:第1磁阻區間與第2磁阻區間,該第1磁阻區間與第 2磁阻區間是分別對應於在曲柄軸之2次旋轉的每一次旋 轉中,磁阻通過拾取器的位置;及第1區間與第2區間, 該第1區間與第2區間是分別對應於磁阻未通過拾取器的 位置;且具備:求取第1平均値的手段,該第1平均値是 -14- 201033597 由第1區間所檢測的第1旋轉速度、與由第2區間所檢測 之第2旋轉速度的平均値;和求取第2平均値的手段’該 第2平均値爲由第1磁阻區間所檢測的第1磁阻旋轉速度 、與由第2磁阻區間所檢測之第2磁阻旋轉速度的平均値 ;和計算平均引擎旋轉速度的手段,該平均引擎旋轉速度 是藉由述第1平均値除以第1旋轉速度的値,再乘以第2 平均値所求出;及負載狀態計算手段,該負載狀態計算手 • 段是使用平均引擎旋轉速度來計算引擎的負載狀態,因此 能在計算平均引擎旋轉速度的計算式中含有:將磁阻部分 的旋轉速度,除以與其相同之磁阻部分的旋轉速度的關係 。如此一來,即使在磁阻的圓周方向長度等中存有尺寸公 差的場合中,也能降低在計算式中該尺寸公差的影響,而 計算更適當的平均引擎旋轉速度。此外,可採用檢測「用 來驅動引擎的點火裝置或燃料噴射裝置之時機」的脈衝轉 子,來設定「用來檢測平均引擎旋轉速度」的特定區間。 • 根據第10特徴,可降低在平均引擎旋轉速度的計算 式中,降低磁阻的尺寸公差對平均引擎旋轉速度之計算値 所造成的影響。 根據第11的特徴,由於設定成:第1區間包含進氣 行程’且第2區間包含燃燒一膨脹行程,當求取第1平均 値之際,是將在第1旋轉速度與第2旋轉速度之間執行不 同加權處理的加權係數α設定成大於0.5,因此在特定區 間的引擎轉速中,即使具有不同於一般運轉時之大量變動 的場合,也能計算「已考慮了燃燒-膨脹行程中之引擎旋 -15- 201033597 轉速度的上升程度」的平均引擎旋轉速度。如此一來’即 使在因「加速時或行走於凹凸路面等」而導致引擎旋轉速 度的變動增大的場合中,也能計算更適當的引擎負載狀態 〇 根據第12特徴,由於磁阻被配設在即將到達引擎上 死點時的位置,且引擎的負載狀態,是將第2磁阻旋轉速 度除以平均引擎轉數所算出的負載率,故能藉由簡單的計 算式來檢測引擎負載。此外,可適當地檢測「從壓縮行程 © 的後半段到燃燒-膨脹行程期間」之引擎的旋轉變動,而 求取引擎的負載率。 根據第13特徴,由於對應於負載率並至少對引擎的 點火時期執行反饋控制,故能僅採用脈衝轉子的輸出訊號 來計算引擎的負載率,並根據該負載率而至少修正控制引 擎的點火時期。如此一來,無需設置用來檢測引擎之負載 狀態的感應器等,便可執行適當的點火時期控制。 根據第14特徴,由於包含:將用來檢測平均引擎旋 @ 轉速度的檢測區間,設定成從磁阻的通過開始點起計算之 曲柄軸的2次旋轉量之長度的步驟;和將檢測區間設成由 以下所形成之4個區間的步驟:第1磁阻區間與第2磁阻 區間,該第1磁阻區間與第2磁阻區間是分別對應於在曲 柄軸之2次旋轉的每一次旋轉中,磁阻通過拾取器的位置 、和第1區間與第2區間,該第1區間與第2區間是分別 對應於磁阻未通過拾取器的位置;和求取第1平均値的步 驟,該第1平均値是由第1區間所檢測的第1旋轉速度、 -16- 201033597 與由第2區間所檢測之第2旋轉速度的平均値;和求取第 2平均値的步驟,該第2平均値是由第1磁阻區間所檢測 的第1磁阻旋轉速度、與由第2磁阻區間所檢測之第2磁 阻旋轉速度的平均値;及計算平均引擎旋轉速度的步驟, 該平均引擎旋轉速度是藉由對第1平均値除以第1旋轉速 度的値,再乘以第2平均値所獲得,因使即使在磁阻之圓 周方向長度等中具有尺寸公差時,也能將低計算式中磁阻 φ 之尺寸公差的影響,而計算更正確的平均引擎旋轉速度。 如此一來,可計算更適當的引擎負載。 根據第1 5特徴,由於具備用來偵測變速機之變速比 的變速比偵測手段,且引擎的負載狀態,是將磁阻通過拾 取器期間的旋轉速度,除以平均引擎轉數所算出的負載率 ,並根據變速比來修正磁阻通過拾取器期間的旋轉速度, 因此可將「從曲柄軸起到後輪爲止」之扭力傳動系統的影 響列入考慮,來計算引擎的負載狀態。具體地說,可處理 Φ 「當變速機的變速比越大,導致將磁阻通過拾取器期間的 旋轉速度計算成越小」的現象,如此一來,能更正確地計 算引擎的負載狀態。 根據第1 6特徴,由於變速比偵測手段,是用來檢測 有段變速機之變速檔位的齒輪位置感應器,故能以簡單的 構造來檢測有段變速機的變速比,並修正磁阻通過拾取器 期間的旋轉速度。 根據第17特徴,由於磁阻通過拾取器期間之旋轉速 度的修正,是藉由對該旋轉速度乘以修正係數的方式執行 -17- 201033597 ,且修正係數是設成當有段變速機的齒輪檔數越低時則越 大,因此當變速機的變速比變的越大,越容易受到「從曲 柄軸到後輪爲止之扭力傳動系統」的影響,換言之,即使 實際的引擎負載狀態相同,也能配合「變速比變的越大時 ,磁阻通過拾取器期間之旋轉速度變小」的傾向,來執行 適當的修正。 根據第18特徴,由於變速比偵測手段是根據車速與 引擎轉數來求取變速比,因此不需要用來檢測變速檔位的 @ 位置感應器,而能期待成本的降低。 【實施方式】 以下,參考圖面來詳細地說明本發明的最佳實施形態 。第1圖,是採用「本發明其中一種實施形態的引擎負載 檢測裝置」之引擎1的構造圖。引擎1爲4行程單汽缸的 内燃機’並具有透過連桿,使「在汽缸8的内部往復移動 」的活塞7連結於曲柄軸9的構造。在汽缸8的上部設有 @ :進氣管2與排氣管4;及「與曲柄軸9的旋轉同步執行 開閉動作」的進氣閥3與排氣閥5。此外,在汽缸8的上 端部,安裝有作爲點火裝置的火星塞6。 在曲柄軸9安裝有:與該曲柄軸9同步旋轉的脈衝轉 子1 〇。在脈衝轉子1 0的外周部,安裝有朝徑方向外側僅 突出特定量的磁阻。在脈衝轉子10的附近,配置有被固 定於引擎1之曲柄箱等的磁性拾取器20,該磁性拾取器 20可反應磁阻「隨著脈衝轉子10之旋轉」的通過,而輸 -18- 201033597 出曲柄脈衝訊號。 在作爲引擎控制裝置的ECU30處包含:用來檢測來 自於磁性拾取器20之脈衝訊號的曲柄脈衝檢測部40 ;和 作爲引擎1之負載狀態檢測手段的負載率計算部50 ;和對 應於引擎的負載狀態,來計算點火時期之修正量的控制修 正量計算部60 ;和控制火星塞6之點火的點火控制部70 ;及至少根據節流閥開度與引擎轉數Ne的資訊來決定點 φ 火時期的點火圖形80。本實施形態的ECU30,是根據被 輸入曲柄脈衝檢測部40的脈衝訊號,求取引擎1的負載 狀態(負載率F),並對應於該負載狀態來修正控制火星塞 6的點火時期。 在此,所謂引擎1的負載率F是指:譬如引擎轉數即 使爲相同狀態,由於在以一定的速度行走於平坦路的場合 、與上坡路段中加速的場合中,作用於引擎1的負載狀態 不同,而以數値表示「用於修正控制上述情形」之負載的 9 大小。前述的點火控制部70,在負載率F較大,也就是 指作用於引擎的負載較大的場合中可以:稍微修正點火時 期的減速角而防止爆震等、對應於負載狀態而獲得適當的 點火時期。負載率F的計算方法將於稍後詳細地說明。 而在本實施形態中,雖然採用負載率F而僅執行點火 時期的修正控制,但亦可由ECU30執行「對引擎1供給 燃料之燃料噴射裝置(圖面中未顯示)」的控制,並對應於 負載率F來執行燃料噴射控制。 第2圖,是顯示「被設於ECU30的負載率計算部50 -19- 201033597 之細部」的塊狀圖。負載率計算部50,是根據由前述曲柄 脈衝檢測部40所輸入的曲柄脈衝訊號、及由計時器51所 計測的時間,來計算引擎1的負載率F。負載率計算部50 中除了計時器51之外,還包含Ne計算手段52、Αω計算 手段53、(otdc計算手段54、磁阻電氣角決定手段55、負 載率計算手段5 6。201033597 VI. Description of the Invention: [Technical Field] The present invention relates to an engine load detecting device and an engine load detecting method, and more particularly to detecting an engine load state based on an output signal of a pulse rotor that "rotates synchronously with a crankshaft" Engine load detection device and engine load detection method. [Prior Art] Conventionally, a pulse rotor having "synchronous rotation with the crankshaft of the engine" and a pickup coil for detecting "passing state of the magnetic resistance of the pulse rotor" are provided, and according to the pickup coil The output of the pulse signal to detect the load state of the engine engine load detection device has been known to the public. Patent Document 1 discloses a technique in which the magnetic resistance of the pulse rotor is set near the position corresponding to the "top dead center of the engine", and the pulse rotor is rotated once per revolution or once per rotation. The ratio of the time to the time the magnetoresistance passes, and the load state of the engine is detected based on the degree of variation of the ratio. [Patent Document 1] [Patent Document 1] JP-A-2002-115598 [Summary of the Invention] [Problems to be Solved by the Invention] The technique described in Patent Document 1 is for detecting -5&quot; 201033597 " "The time required for the crankshaft to rotate once" "The passage time of the reluctance as the reference is not considered to be longer. For example, the "time required for the crankshaft to rotate twice" is used as a reference to detect the more appropriate. Load status. In addition, even when the crankshaft rotates once, the fluctuation of the engine rotation speed is not evaluated in accordance with the four strokes of the four-stroke engine (intake, compression, combustion-expansion, and exhaust). In addition, the technique described in Patent Document 1 is for detecting the on-time of the reluctance based on the "time required for the crankshaft to rotate once," so that the length of the magnetic resistance in the circumferential direction remains. When there is a "size offset due to dimensional tolerance", the calculated ratio may also have the effect of dimensional tolerance, and there is a possibility that the load state of the engine cannot be detected correctly. In addition, the rotational speed (angular velocity) of the crankshaft is easily affected by the torque transmission system from "crankshaft to rear wheel", which is known to the public. Therefore, it is expected that a load calculation can be calculated in consideration of the above situation. Construction. SUMMARY OF THE INVENTION It is an object of the present invention to provide a method for solving the above-mentioned prior art, which is more correct in view of the rotational variation caused by the four strokes of the 4-stroke engine and the effect of reducing the dimensional tolerance of the pulse rotor. A load detecting device and a load detecting method for detecting the load state of the engine. [Means for Solving the Problems] In order to achieve the above object, the present invention includes a pulse rotor that rotates in synchronization with a crankshaft of an engine, and a magnetoresistance that is provided in the pulse rotor and that corresponds to the aforementioned a -6-201033597 shank angle near the dead point of the engine; and a picker for detecting the reluctance and detecting the load of the engine based on the output signal of the pickup, A first feature of the present invention includes means for dividing a specific section of an average engine rotation speed into a plurality of numbers, and calculating an engine rotation speed of the divided plurality of section sections based on an output signal of the extractor; and weighting means The weighting performs different weighting and load state calculation means on the engine rotation speed of the plurality of sections, and the load state calculation means calculates the engine rotation speed based on the average 値 of the complex interval engine rotation speed, and uses The average engine rotational speed is used to perform calculation of the load state. Further, the second feature is a technique in which the weighting ratio is set to be larger than the other sections in the section divided into the plurality of sections, and the weighting ratio including the combustion-expansion section is set. Further, the third feature is a technical point in which the specific region Φ is detected based on the output signal of the pulse rotor. Further, the fourth feature is a technical point in which the length 2 of the second rotation amount of the crankshaft is equally divided into the first zone 2 section, and the first section includes the intake stroke, and the front section includes Combustion-expansion stroke. Further, the fifth feature is a technical point in which the state of the engine is a rotation rate calculated by the average engine revolution number in the "rotation speed of the magnetoresistor passing through the pickup period". In addition, the sixth feature is the following technical point: the aforementioned magnetic resistance is passed; the detection of the state is to detect the respective means of the pick-up; the weighting is the average of the engine, which is between the strokes, between, and between The second load level is set at a position when the engine top dead center is reached at 201033597, and the load factor is "the period during which the magnetic resistance passes through the pick-up device when the top dead center of the compression side is reached". The rotation speed is calculated. Further, the '7th and 8th features are the following technical points: at least the ignition timing of the engine is feedback-controlled in accordance with the calculated load factor. Further, the present invention includes a pulse rotor that is coupled to the engine. The crankshaft rotates synchronously; and the magnetoresistance is set at the pulse rotor @ and is located at a crank angle corresponding to the top dead center of the engine; and a pickup for detecting the magnetoresistance And the engine load detecting method for detecting the load state of the engine based on the output signal of the picker, the ninth feature of the present invention is the following technical point: the average adopted when calculating the load state of the engine The engine rotation speed includes: a step of dividing a specific section for detecting the average engine rotation speed into a complex number; and a step of calculating a rotation speed of each section engine of the plurality of divided sections; and the plurality of The interval engine rotation speed is a step of performing different weighting processes; and the plurality of interval engines after the weighting process is obtained The average 旋转 of the rotational speed is used to calculate the aforementioned average engine rotational speed. Further, the present invention is provided with: a pulse rotor that rotates in synchronization with a crankshaft of the engine; and a magnetoresistance that is disposed in the pulse rotor and is located at a crank corresponding to the top dead center of the engine Angle; and a pickup, the pickup is used to detect the passage of the reluctance; and the engine load detection device for detecting the load state of the engine according to the output signal of the pickup, -8-201033597, the 10th of the present invention The technique is characterized in that the detection section for detecting the average engine rotation speed is set to the length of the second rotation amount of the crankshaft calculated from the start point of the magnetic resistance, and the detection section is set to be The four sections formed are: a first magnetoresistive section and a second magnetoresistive section, wherein the first magnetoresistive section and the second magnetoresistive section correspond to each of the two rotations of the crankshaft, respectively The magnetic resistance passes through the position of the pickup; and the first interval and the second interval, wherein the first interval φ and the second interval respectively correspond to positions where the magnetic resistance does not pass through the pickup; the engine of the present invention is negative The load detecting device includes means for obtaining a first average value , which is an average value of the first rotation speed detected by the first section and the second rotation speed detected by the second section: And a means for obtaining the second average 値, wherein the second average 値 is the first reluctance rotational speed detected by the first reluctance section and the second reluctance rotational speed detected by the second reluctance section And a means for calculating the average engine rotation speed, wherein the average engine rotation speed is obtained by multiplying the first average 値 by the 旋转 of the first rotation speed by the second average 値And a load state calculation means for calculating a load state of the engine using the average engine rotation speed. Further, the first feature is a technique for calculating the average engine rotational speed when the first rotational speed is represented by ®4 (n_1) and the second rotational speed is represented by ω4 (η). When the first reluctance rotational speed is represented by cotdcl, the second reluctance rotational speed is represented by c〇tdc2, and the weighting coefficient of the weighting process is represented by α, the calculation formula is calculated by the following formula -9 - 201033597 [calculation formula] 1] NeA' In addition, the first section of the package stroke, when the speed and the aforementioned weight coefficient α are set, the position of the front degree, except for the previous 14th less for the aforementioned reference, the engine's crankshaft, and the position of the clutch The output signal of the pickup, the present invention detects the average lead through the starting point; and the aforementioned average engine rotation speed NeA. _ (ΐ-α) χί〇4 + («-ΐ)+αχβ; 4(«) ωίάεΐ + wtdcl ωΑ(η -1) 2 The twelfth feature is the following technical point: set to: the aforementioned intake stroke And the second section includes the combustion-expansion when the first average enthalpy is taken, and the addition of the different weighting process between the first rotation and the second rotation speed is greater than 〇. The magnetic resistance is a load state of the engine when it is about to reach the top dead center of the engine, and is a load ratio calculated by rotating the second magnetic reluctance speed by the average engine revolution number. The feature is the following technical point: feedback control is performed at the ignition timing of the engine corresponding to the aforementioned load rate. The invention is provided with: a pulse rotor which rotates synchronously with the lead; and a magnetic resistance which is set at a crank angle of the pulse rotor which is near the top dead center of the engine; and the pickup is used for detecting The 15th characteristic of the engine load detecting means for detecting the load state of the engine based on the pickup number is the following technical point: including: setting the detection section for the rotational speed of the engine to be from the aforementioned magnetic The step detection section for calculating the length of the second rotation amount of the crankshaft from the resistance is set to step 10-201033597 of the four sections formed as follows: the first magneto-resistance section and the second magneto-resistance section, The first magneto-resistance section and the second magneto-resistance section respectively correspond to a position of the pick-up device and a first section and a second section in each of the two rotations of the crankshaft. The first interval and the second interval correspond to a position at which the magnetic resistance does not pass through the pickup, and a step of obtaining a first average '. The first average 値 is a first rotational speed detected by the first interval. With the foregoing The average 値 of the second rotation speed detected in the two sections; and the step of obtaining the second average 値, the second average 値 is the first reluctance rotation speed detected by the first magnetoresistive section, and An average 値 of the second reluctance rotational speed detected by the second magnetic resistance section; and a step of calculating the average engine rotational speed, wherein the average engine rotational speed is divided by the first rotational speed by the first rotational speed The 値 is then multiplied by the aforementioned 2nd average 获得. Further, the present invention is provided with: a pulse rotor that rotates in synchronization with a crankshaft of the engine; and a magnetoresistance that is disposed in the pulse rotor® and is located near the top dead center of the engine a crank angle; and a pickup for detecting the passage of the magnetic resistance; and an engine load detecting device for detecting a load state of the engine based on an output signal of the pickup, the 16th feature of the present invention is as follows Technical point: a gear ratio detecting means for detecting a gear ratio of the transmission, wherein the load state of the engine is set to: divide the rotation speed of the magnetoresistor through the pickup period by the average engine speed The calculated load factor is corrected by the above-described gear ratio by the rotational speed of the above-mentioned reluctance passing through the pickup. Further, the 17th feature is the following technical point: the above-described gear ratio detection -11 - 201033597 means a gear position sensor for detecting a shift position of a segmented transmission. Further, the eighteenth feature is the technical point that the correction of the rotational speed of the magnetic resistance during the passage of the pickup is performed by multiplying the rotational speed by a correction coefficient, and the correction coefficient is When the number of gears of the transmission is low, it is set to be large. Furthermore, the 19th feature is a technical point in which the gear ratio detecting means obtains the gear ratio based on the vehicle speed and the number of engine revolutions. @ [Invention Effect] According to the first feature, when calculating the average engine rotation speed for "calculation of the load state of the engine", the specific section for detecting the engine rotation speed is divided into a plurality of pieces and calculated separately. The interval engine rotation speed of each of the divided plurality of sections is performed, and different weighting processing is performed on the plurality of section engine rotation speeds, not only to obtain the plurality of interval engine rotation speeds after the weighting process The average 値 is used to calculate the average engine rotation speed. Therefore, even if there is a large number of rotation variations different from the normal operation in a certain interval, the weighting of the rotation variation can be performed to calculate an appropriate average engine rotation speed. In this case, even when the fluctuation of the engine rotational speed in the specific section is increased due to "acceleration or traveling on the uneven road surface or the like", the engine load state corresponding to the above situation can be obtained by calculation. According to the second feature, since the weighting process is divided into a plurality of sections, the weighting ratio of the section including the combustion-expansion stroke is set to be larger -12-201033597 in other sections, so even when "accelerating or walking" In the case where the degree of increase in the engine rotational speed in the combustion-expansion stroke is increased, in particular, the engine load corresponding to the above situation can be obtained by calculation. According to the third feature, since the specific interval is detected based on the output signal of the pulse rotor, the pulse rotor for detecting the "time for driving the ignition device or the fuel injection device of the engine" can be used to set "to detect the flat φ engine. The specific range of the rotation speed. In this way, the engine load state can be calculated by calculation without additionally setting a new sensor or the like. According to the fourth feature, the specific section divides the length 2 of the second rotation amount of the crankshaft into the first section and the second section, and sets the first section to include the intake stroke, and the second section includes the combustion-expansion stroke. Therefore, the segmentation of a specific section can be performed in a simple manner. Further, by setting the weight of the second section including the combustion-expansion stroke to be large, the load state in which the fluctuation of the engine rotation speed in the combustion-expansion stroke is considered can be calculated by calculation. Further, by dividing a specific section by the minimum number of divisions, it is possible to suppress the increase in the calculation load and obtain the effect of the weighting processing. According to the fifth feature, since the load state of the engine is the load ratio calculated by dividing the rotational speed of the magnetic resistance during the pickup by the average engine revolution, the load of the engine can be obtained by a simple calculation formula. status. According to the sixth feature, since the reluctance is set at a position just before reaching the top dead center of the engine, and the load factor is "the rotational speed of the reluctance passing through the pickup when the dead point is reached to the upper side of the compression side" Since it is calculated, it is possible to appropriately detect a large number of engine rotation fluctuations from the end of the compression stroke to the combustion-expansion stroke period -13 to 201033597, and to obtain the load factor of the engine in which the rotation variation has been considered. According to the seventh feature, since the feedback control is performed on at least the ignition timing of the engine corresponding to the calculated load rate', there is no need to additionally set a new inductor or the like, and only the output signal of the pulse rotor is required, at least the ignition timing. Correct the possibility of control changes. According to the eighth feature, there is a step of dividing a specific section for detecting an average engine rotation speed into a complex number; and a step of calculating a rotation speed of each section engine of the divided plurality of sections; and a plurality of sections a step of performing different weighting processing by the engine rotation speed; and a step of calculating an average engine rotation speed by calculating an average 値 of a plurality of interval engine rotation speeds after the weighting process; and performing an engine load state using the average engine rotation speed The calculation step, so that even if the engine rotation speed of the specific section has a large variation from the normal operation time, the appropriate average engine rotation speed can be calculated by performing the weighting that has considered the rotation variation, and Based on this, the load status of the engine is calculated. @ According to the ninth feature, the detection interval for detecting the average engine rotation speed is set to the length of the second rotation amount of the crankshaft calculated from the start point of the reluctance, and the detection interval is set to be formed as follows Four sections: a first magnetoresistive section and a second magnetoresistive section, wherein the first magnetoresistive section and the second magnetoresistive section correspond to each of the two rotations of the crankshaft, and the reluctance passes through the pickup And a first interval and a second interval, wherein the first interval and the second interval correspond to a position at which the magnetic resistance does not pass through the pickup, and a means for obtaining a first average ,, the first average 値Yes-14- 201033597 The first rotation speed detected by the first section and the average rotation speed of the second rotation speed detected by the second section; and the means for obtaining the second average ' 'The second average 値 is The first reluctance rotation speed detected by the first magnetoresistive section and the average enthalpy of the second reluctance rotation speed detected by the second reluctance section; and means for calculating the average engine rotation speed, the average engine rotation speed is By dividing the first average 値 by the first rotational speed And multiplied by the second average ;; and the load state calculation means, the load state calculation hand segment uses the average engine rotational speed to calculate the load state of the engine, and thus can be used in the calculation formula for calculating the average engine rotational speed Contains: the relationship between the rotational speed of the magnetoresistive portion divided by the rotational speed of the same magnetoresistive portion. As a result, even in the case where the dimensional tolerance is present in the circumferential length of the magnetic resistance or the like, the influence of the dimensional tolerance in the calculation formula can be reduced, and a more appropriate average engine rotational speed can be calculated. Further, a pulse interval for detecting "the timing of the ignition device or the fuel injection device for driving the engine" can be used to set a specific interval for "detecting the average engine rotation speed". • According to the 10th feature, the effect of reducing the dimensional tolerance of the reluctance on the calculation of the average engine rotation speed can be reduced in the calculation formula of the average engine rotation speed. According to the eleventh aspect, the first section includes the intake stroke 'the second section includes the combustion-expansion stroke, and when the first average 値 is obtained, the first rotation speed and the second rotation speed are set. The weighting coefficient α between which the different weighting processing is performed is set to be larger than 0.5, so that in the engine speed of the specific section, even if there is a large variation from the normal operation, it can be calculated that "the combustion-expansion stroke has been considered. The average engine rotation speed of the engine spin -15- 201033597. In this way, even in the case where the fluctuation of the engine rotation speed is increased due to "acceleration or walking on the uneven road surface, etc.", it is possible to calculate a more appropriate engine load state. According to the twelfth feature, the magnetic resistance is matched. It is located at the position when the engine is at the top dead center, and the load state of the engine is the load rate calculated by dividing the second reluctance rotation speed by the average engine revolution. Therefore, the engine load can be detected by a simple calculation formula. . Further, the engine rotation load rate can be obtained by appropriately detecting the rotation variation of the engine from the second half of the compression stroke © to the combustion-expansion stroke period. According to the thirteenth feature, since the feedback control is performed corresponding to the load factor and at least the ignition timing of the engine, the output signal of the pulse rotor can be used only to calculate the load rate of the engine, and at least the ignition timing of the control engine can be corrected according to the load rate. . In this way, it is possible to perform appropriate ignition timing control without providing an inductor or the like for detecting the load state of the engine. According to the fourteenth aspect, the detection section for detecting the average engine rotation speed is set to a length of the second rotation amount of the crankshaft calculated from the start point of the reluctance; and the detection section is to be detected. The steps of the four sections formed by the first magnetoresistive section and the second magnetoresistive section, the first magnetoresistive section and the second magnetoresistive section respectively correspond to the second rotation of the crankshaft In one rotation, the magnetic resistance passes through the position of the pickup, and the first section and the second section, which correspond to positions where the reluctance does not pass through the pickup, and the first average 値Step, the first average 値 is a first rotation speed detected by the first section, -16-201033597 and an average 値 of the second rotation speed detected by the second section; and a step of obtaining the second average 値The second average 値 is an average 値 of the first reluctance rotational speed detected by the first reluctance section and the second reluctance rotational speed detected by the second reluctance section; and a step of calculating the average engine rotational speed The average engine rotation speed is determined by the first average By dividing the 旋转 of the first rotation speed by the second average 値, the dimensional tolerance of the magnetic resistance φ in the low calculation formula can be made even if there is a dimensional tolerance in the circumferential length of the magnetic resistance or the like. The effect, while calculating the more accurate average engine rotation speed. In this way, a more appropriate engine load can be calculated. According to the fifteenth aspect, since the gear ratio detecting means for detecting the gear ratio of the transmission is provided, and the load state of the engine is calculated by dividing the rotational speed of the reluctance through the pickup by the average engine revolutions The load rate and the rotation speed of the reluctance during the passage of the pickup are corrected according to the gear ratio, so that the influence of the torque transmission system "from the crankshaft to the rear wheel" can be considered to calculate the load state of the engine. Specifically, Φ "the smaller the gear ratio of the transmission, the smaller the rotation speed during the passage of the reluctance through the pickup" can be handled, so that the load state of the engine can be calculated more accurately. According to the first aspect, since the gear ratio detecting means is a gear position sensor for detecting the shift position of the stepped shifting machine, the gear ratio of the stepped shifting machine can be detected with a simple configuration, and the magnetic field can be corrected. The speed of rotation during the passage of the pickup. According to the seventeenth feature, the correction of the rotational speed during the passage of the reluctance by the pickup is performed by multiplying the rotational speed by the correction coefficient, and the correction coefficient is set to be the gear of the stepped transmission. The lower the number of shifts, the larger the shift ratio of the transmission becomes, the more susceptible it is to the "torque transmission system from the crankshaft to the rear axle", in other words, even if the actual engine load state is the same, It is also possible to perform an appropriate correction in accordance with the tendency that the rotation speed of the reluctance is reduced during the pickup is increased as the shift ratio becomes larger. According to the eighteenth feature, since the speed ratio detecting means obtains the speed ratio based on the vehicle speed and the number of engine revolutions, the @ position sensor for detecting the shift position is not required, and cost reduction can be expected. [Embodiment] Hereinafter, preferred embodiments of the present invention will be described in detail with reference to the drawings. Fig. 1 is a structural diagram of an engine 1 using an "engine load detecting device of one embodiment of the present invention". The engine 1 is a four-stroke single-cylinder internal combustion engine, and has a structure in which a piston 7 that is "reciprocally moved inside the cylinder 8" is coupled to the crankshaft 9 through a connecting rod. The intake valve 3 and the exhaust valve 5 of @: the intake pipe 2 and the exhaust pipe 4; and "the opening and closing operation in synchronization with the rotation of the crankshaft 9" are provided in the upper portion of the cylinder 8. Further, at the upper end portion of the cylinder 8, a spark plug 6 as an ignition device is attached. A pulse rotor 1 旋转 that rotates in synchronization with the crankshaft 9 is attached to the crankshaft 9. In the outer peripheral portion of the pulse rotor 10, a specific amount of magnetic resistance is protruded outward in the radial direction. In the vicinity of the pulse rotor 10, a magnetic pickup 20 fixed to a crank case or the like of the engine 1 is disposed, and the magnetic pickup 20 can respond to the passage of the magnetic resistance "with the rotation of the pulse rotor 10", and loses -18- 201033597 The crank pulse signal. The ECU 30 as an engine control device includes: a crank pulse detecting portion 40 for detecting a pulse signal from the magnetic pickup 20; and a load factor calculating portion 50 as a load state detecting means of the engine 1; and an engine corresponding to the engine a load correction state calculation unit 60 for calculating the correction amount of the ignition timing; an ignition control unit 70 for controlling the ignition of the spark plug 6; and a point φ based on at least the information of the throttle opening degree and the number of engine revolutions Ne Ignition pattern 80 during the fire period. The ECU 30 of the present embodiment obtains the load state (load factor F) of the engine 1 based on the pulse signal input to the crank pulse detecting unit 40, and corrects the ignition timing of the control spark plug 6 in accordance with the load state. Here, the load factor F of the engine 1 means that, for example, if the number of revolutions of the engine is in the same state, the load acting on the engine 1 is applied when the vehicle travels on a flat road at a constant speed and accelerates in an uphill section. The state is different, and the number of 9 indicates the size of the load used to correct the above situation. In the above-described ignition control unit 70, when the load factor F is large, that is, when the load acting on the engine is large, the deceleration angle of the ignition timing can be slightly corrected to prevent knocking, etc., and appropriate for the load state. Ignition period. The calculation method of the load factor F will be described in detail later. In the present embodiment, the correction control of the ignition timing is performed only by the load factor F. However, the ECU 30 may perform control of "the fuel injection device that supplies fuel to the engine 1 (not shown in the drawing)", and corresponds to The fuel injection control is performed at the load factor F. In the second drawing, a block diagram showing "the details of the load factor calculation unit 50 -19 - 201033597 provided in the ECU 30" is displayed. The load factor calculation unit 50 calculates the load factor F of the engine 1 based on the crank pulse signal input from the crank pulse detecting unit 40 and the time measured by the timer 51. The load factor calculation unit 50 includes an Ne calculation means 52, a Αω calculation means 53, an otdc calculation means 54, a reluctance electrical angle determination means 55, and a load ratio calculation means 56 in addition to the timer 51.

Ne計算手段52,是用來計算檢測區間中的引擎轉數 Ne(平均引擎轉數NeA)。此外,磁阻電氣角決定手段55, Q 是根據磁阻通過磁性拾取器20時的脈衝訊號,來檢測「 以電氣性檢測的磁阻」之圓周方向的角度。(otdc計算手段 54,是用來計算磁阻通過磁性拾取器20期間之脈衝轉子 10的旋轉速度(角速度),也就是僅計算磁阻部分的角速度 cotdc(rad/s) 〇 此外,Δω計算手段53,是藉由從「由前述Ne計算 手段52所計算」的引擎轉數Ne,減去「由前述cotdc計算 手段所計算」之磁阻部分的角速度cotdc,來計算曲柄角速 Θ 度的變動量Aco(Aco = Ne-Q)tdc)。而Αω計算手段53的減法 運算,是將引擎轉數Ne(rpm)轉換成引擎旋轉速度(rad/s) 而執行。接著,在負載率計算手段56中,是採用「由Δ® 計算手段53所計算」之角速度的變動量Αω、與「由Ne 計算手段52所計算」的引擎轉數Ne,並藉由Δω + Νεχ100(%) 的計算式來計算引擎負載率F。該負載率F成爲:引擎負 載越大時則越大的數値。 第3圖,是脈衝轉子10的放大正視圖。在本實施形 -20- 201033597 態的脈衝轉子10,設有第i磁阻n與第2磁阻12。在第 3圖中’脈衝轉子1〇是朝逆時計方向旋轉,而來自於磁性 拾取器20的曲柄脈衝訊號,是形成以第1磁阻u的起點 G1、第1磁阻1 1的終點G2、第2磁阻12的起點G3、第 2磁阻1 2的終點G4的順序所輸出。 第2磁阻12是構成具有:從起源於引擎之上死點 (TDC)的第4角度Θ4的略前方位置起,形成第i角度01 Φ 的圓周方向長度。此外,第1磁阻11具有形成第3角度 Θ3的圓周方向長度,並在第1磁阻n的起點G1、與第2 磁阻12的起點G3之間設有第2角度Θ2。在本實施形態 中是分別設定成:第1角度Θ1=45度,第2角度Θ2 = 22.5 度’第3角度Θ3 = 11·25度,第4角度Θ4=15度。而在該 圖中’雖然是顯示脈衝轉子10與磁性拾取器20分離一段 距離,但磁阻1 1、1 2之外周面與磁性拾取器20的間隔, 是被設定成譬如〇.5mm。 ® 第4圖,是顯示「由磁性拾取器20所輸出」的曲柄 脈衝訊號、與曲柄軸每1次旋轉的平均引擎轉數NeA、與 曲柄軸的角速度ω間之關係的圖表。圖中的A-B區間,是 表示「包含進氣行程之曲柄軸的1次旋轉量」的長度。圖 表(a),是顯示引擎轉數Ne形成一定,而行走於平坦路的 一般時期,而圖表(b),則顯示因加速中或節流閥操作而使 引擎轉數Ne上升中的過渡時期。圖表(c),僅顯示行走於 波狀路面(凹凸路面)時之角速度ω的變位運動。 根據該圖表可得知,無論引擎轉數呈一定或上升中, -21 - 201033597 曲柄角速度ω將重複「配合引擎之1個週期的週期性變動 」。此外,在波狀路面中,由於「因凹凸路面而作用了使 驅動輪加減速」的力量,倘若長期地觀察角速度ω的變動 ,將產生整體性的減緩或起伏。但是’即使在波狀路面中 ,在曲柄軸的每1次旋轉單位中,反覆「配合引擎之1個 週期的週期性變動」這點是不變的。此外’可以確認的是 無論哪一種行走條件,在包含進氣行程的Α-Β區間中’角 速度ω均呈直線性變動。接著,Α-Β區間中之角速度ω的 春 直線性軌跡,在(a)的一般時期中形成大幅的右端下降,在 (b)的過渡期間該右端下降的角度則大幅降低。 第5圖,是顯示在1個週期中曲柄脈衝訊號與角速度 ω間之關係的圖表。與前述相同的圖號,是表示相同或相 等的部分。如以上所述,角速度ω是配合4行程中的各個 行程而週期性地變動。在「從壓縮行程的後半段起、至燃 燒-膨脹行程間之區間D 1」中的減少(下降),是起因於汽 缸内壓的上升而產生的壓縮抵抗。此外,在燃燒-膨脹行 @ 程之區間D2中的增加(上升),則是起因於「因燃燒所造 成之汽缸内壓的上升,而產生的曲柄旋轉能量」。 接著,在「從區間D2結束後,直到進氣行程結束爲 止」之區間D3中的減少(下降),是起因於「在燃燒結束 而曲柄角速度ω達到峰値之後,所產生之引擎1的機械性 摩擦抵抗或燃燒氣體的排出抵抗」。而區間D4,是表示 「將第2磁阻12的起點G3作爲起始點」之曲柄1次旋轉 量的長度。 -22- 201033597 在該圖中,在引擎轉數(旋轉速度)Ne相同的場合中, 一般時期的曲柄角速度ω是以實線表示,而高負載時的曲 柄角速度ω則以虛線表示。如同圖面所顯示,當高負載時 角速度ω的變動增大。這是由於:即使在引擎旋轉速度 Ne相同的場合中,輸出扭力越高將使角速度ω的峰値變 大,而在此之後的下降量,是吸入空氣量越多時則變大的 緣故。 φ 而該曲柄角速度ω的變動,是越趨近「曲柄軸之慣性 力變小的低旋轉區域」則變大,此外,如同本實施形態的 單汽缸引擎1,在汽缸數量少且爆發間隔大的引擎中,更 具有容易變大的傾向。 第6圖,是第5圖的局部放大圖。如以上所述,引擎 1的負載狀態,是藉由引擎的負載率F所檢測。該負載率 F,是在包含壓縮上死點的區間D1内,相對於引擎轉數 Ne之角速度ω的減少程度,換言之,是將壓縮行程中之 • 壓縮抵抗的大小予以數値化後的値。在本實施形態中構成 :第2磁阻12是位於區間D1内,將該第2磁阻12通過 磁性拾取器20時的角速度rotdc與引擎旋轉速度Ne間的 差異値,作爲角速度ω的變動量Δω來計算。圖中的cotdc 區間,是對應於從第2磁阻12的起點G3起,到終點G4 爲止的通過時間。 以下,參考第7、8、9圖,說明「用來正確地檢測過 渡時之負載率F」的加權處理。該加權處理爲以下的方法 :當計算檢測區間内的引擎旋轉速度Ne時,將該檢測區 -23- 201033597 間分割成複數個,計算每一個分割區間的區間引擎旋轉速 度,在將上述複數個區間引擎旋轉速度予以平均之際,加 大某特定分割區間的加權,而將NeA調整成適當値。 第7圖,是顯示一般時期及過渡時期中角速度ω之變 動的圖表。圖中的Τ是表示TDC(上死點)。(a)所顯示之一 般時期的角速度ω,是在各行程中相同的上限値與下限値 之間變動。因此,用來計算「前述Δω的計算所採用之引 擎旋轉速度Ne」的檢測區間,只要設成1個週期量的區 @ 間便十分足夠。即使是該圖的範例,也是將曲柄軸從第1 磁阻11之起點G1起的2次旋轉期間,也就是指1個週期 量的區間作爲檢測區間。 但是,相對於(a)的一般時期,儘管(b)所示之過渡時 期的角速度ω是在每1個週期中產生大致相同的變動(形 成大致相同的波形),但在角速度ω到達峰値後、些微的 下降變動後,將朝向下一個峰値地連續性上升。如此一來 ,過渡時期之角速度ω的波形將形成朝右側上升的階梯形 © 狀。此時,譬如當一般時期與過渡時期中的引擎旋轉速度 相同時,一旦對上述兩者執行前述引擎負載率F的計算, 過渡時期的負載率F將會被計算成較一般時期更小’而衍 生出無法實際地對應於引擎所產生之負載狀態的現象。這 是由於:相較於實際的引擎負載狀態’過渡時期的Δω被 計算成較小的緣故,在稍後將作更詳細的說明。 爲了因應上述的問題’在本實施形態中’前提條件是 將前述的檢測區間分割成:從第1磁阻1 1的起點G 1起、 -24- 201033597 到曲柄軸旋轉1次爲止的N e 1區間;和從該N e 1區間的結 束點起、到曲柄軸再次旋轉1次爲止的Ne2區間,而構成 ••藉由該Nel區間的區間引擎旋轉速度Nel (以下’以Nel 表示)、與Ne2區間的區間引擎旋轉速度Ne2(以下,以 Ne2表示)之間的平均値,來計算檢測區間全體的平均引擎 旋轉速度Ne(以下,以NeA表示)。上述的計算處理,是 由前述Ne計算手段52所執行。 第8圖,是顯示過渡時期中之角速度ω與檢測區間 之間的關係的圖表。與前述相同的圖號,是表示相同或 者同等的部分。如先前所述,在過渡時期中,從進氣行 程到壓縮行程之前半段的區間,也就是指N e 1區間內之 角速度ω的減少量變少,在該圖所示的範例中是呈幾乎 水平地推移。相對於此,在壓縮行程的後半段中’在角 速度ω大幅降低後,於燃燒-膨脹行程中大幅增加而達 到峰値。 在此,如先前所述·,引擎負載率F是根據「曲柄軸 角速度ω在壓縮行程的後半段中相對於引擎旋轉速度Ne 的減少程度」所計算的結果。但是,在該計算方法中, 當一般時期與過渡時期內的引擎旋轉速度Ne相同時’引 擎旋轉速度 Ne與 〇)tdc之間的差異値’也就是指 A(〇(A〇i&gt; = Ne-G)tdc)是具有··相較於一般時期,過渡時期將被 計算成較小的傾向。 這是由於:含有cotdc區間之Ne2區間的Ne2 ’相較 於一般時期而言是非常的大,而計算負載率F時應該重視 -25- 201033597 的要素,卻因爲Nel與Ne2之平均値的計算而被抵銷。如 此一來,在過渡時期中所計算的負載率F,將被計算成小 於實際的引擎負載狀態。 因此,在過渡時期中,當計算平均引擎旋轉速度NeA 時,最好是反映引擎旋轉速度Ne2的大小。如此一來,在 該圖的範例中,當計算NeA時,是在Nel與Ne2之間執 行不同的加權處理。在圖示的範例中,是將1個週期間之 平均引擎旋轉速度 NeA的計算式設成:NeA = Nel x(l- Q a) + Ne2xa,並藉由將該加權係數α設定成大於0.5,使 Ne2的加權大於Nel而使NeA整體提升。而執行加權處理 的加權手段,是由負載率計算部50的Ne計算手段52(請 參考第2圖)所含括。 在此,一倂參考第9圖之加權處理的槪念圖。在圖示 的範例中,未執行加權處理時的平均引擎旋轉速度是以 NeAO(虛線)表示,而已執行加權處理時(譬如,α = 0·55)的 平均引擎旋轉速度則以NeA(實線)來表示。此時,曲柄角 Θ 速度ω的變動量,相對於未執行加權處理的場合中所計算 出的ΔωΟ,在已執行加權處理的場合中則增加成Δω(請參 考第8圖)。如此一來,引擎負載率F的計算値也將增加 ,而形成可在過渡時期中,計算出對應於實際之引擎負載 狀態的負載率F。 而在一般時期中,即使在已執行上述加權處理的場合 中,由於Nel與Ne2間的差異甚小,故對負載率F的影響The Ne calculation means 52 is for calculating the engine revolution number Ne (average engine revolution number NeA) in the detection section. Further, the reluctance electrical angle determining means 55 and Q detect the angle in the circumferential direction of the "magnetoresistance electrically detected" based on the pulse signal when the magnetic resistance passes through the magnetic pickup 20. (The otdc calculation means 54 is for calculating the rotational speed (angular velocity) of the pulse rotor 10 during the passage of the magnetic resistance through the magnetic pickup 20, that is, calculating only the angular velocity cotdc(rad/s) of the magnetoresistive portion. Further, the Δω calculation means 53. The change of the crank angular velocity is calculated by subtracting the angular velocity cotdc of the magnetoresistive portion calculated by the cotdc calculation means from the engine revolution number Ne calculated by the Ne calculation means 52. Aco(Aco = Ne-Q)tdc). The subtraction operation of the Αω calculating means 53 is performed by converting the engine revolution number Ne (rpm) into the engine rotation speed (rad/s). Next, the load factor calculation means 56 uses the fluctuation amount Αω of the angular velocity calculated by the Δ® calculation means 53 and the engine rotation number Ne calculated by the "Ne calculation means 52", and is Δω + The calculation formula of Νεχ100(%) is used to calculate the engine load factor F. The load factor F becomes: the larger the engine load, the larger the number. Fig. 3 is an enlarged front elevational view of the pulse rotor 10. In the pulse rotor 10 of the embodiment -20-201033597, the ith magnetic resistance n and the second magnetic resistance 12 are provided. In Fig. 3, 'pulse rotor 1 旋转 is rotated in the counterclockwise direction, and the crank pulse signal from the magnetic pickup 20 is the end point G1 of the first reluctance u and the end point G2 of the first reluctance 11 The starting point G3 of the second reluctance 12 and the end point G4 of the second reluctance 12 are output in the order. The second magnetic resistance 12 is configured to have a circumferential length in which the i-th angle 01 Φ is formed from a slightly forward position from the fourth angle Θ4 originating from the top dead center (TDC) of the engine. Further, the first magnetic resistance 11 has a circumferential length in which the third angle Θ3 is formed, and a second angle Θ2 is provided between the start point G1 of the first magnetic resistance n and the start point G3 of the second magnetic resistance 12. In the present embodiment, the first angle Θ1 = 45 degrees, the second angle Θ 2 = 22.5 degrees 'the third angle Θ 3 = 11 · 25 degrees, and the fourth angle Θ 4 = 15 degrees are set. In the figure, although the pulse rotor 10 is separated from the magnetic pickup 20 by a distance, the interval between the outer peripheral surface of the magnetic resistances 1 1 and 12 and the magnetic pickup 20 is set to, for example, 〇5 mm. Fig. 4 is a graph showing the relationship between the crank pulse signal "output by the magnetic pickup 20", the average engine revolution number NeA for each rotation of the crankshaft, and the angular velocity ω of the crankshaft. The A-B section in the figure is the length indicating the "one rotation amount of the crankshaft including the intake stroke". The graph (a) is a general period in which the engine revolution number Ne is formed to be constant while walking on a flat road, and the graph (b) shows a transition period in which the engine revolution number Ne rises due to acceleration or throttle operation. . The graph (c) shows only the displacement motion of the angular velocity ω when traveling on a corrugated road surface (convex road surface). According to the chart, the crank angular velocity ω will repeat "the periodic variation of one cycle of the engine" regardless of whether the number of engine revolutions is constant or rising. Further, in the undulating road surface, the force that causes the driving wheel to accelerate and decelerate due to the uneven surface is caused to cause a gradual decrease or fluctuation of the angular velocity ω. However, even in the wavy road surface, the "periodical change of one cycle of the engine" is repeated for every rotation unit of the crankshaft. Further, it can be confirmed that the angular velocity ω varies linearly in the Α-Β interval including the intake stroke regardless of the running condition. Then, the spring linear trajectory of the angular velocity ω in the Α-Β interval forms a large right end drop in the general period of (a), and the angle at which the right end descends during the transition period of (b) is greatly reduced. Fig. 5 is a graph showing the relationship between the crank pulse signal and the angular velocity ω in one cycle. The same reference numerals as described above are the same or equivalent parts. As described above, the angular velocity ω is periodically changed in accordance with each stroke in the four strokes. The decrease (fall) in "from the second half of the compression stroke to the interval D 1 between the combustion and expansion strokes" is a compression resistance caused by an increase in the internal pressure of the cylinder. Further, the increase (rise) in the section D2 of the combustion-expansion flow is caused by the "crank rotational energy generated by the increase in the internal pressure of the cylinder caused by the combustion". Then, the decrease (fall) in the section D3 of "from the end of the section D2 until the end of the intake stroke" is caused by the "machine of the engine 1 generated after the crank angular velocity ω reaches the peak after the combustion ends. Sexual friction resistance or discharge resistance of combustion gases." On the other hand, the interval D4 is the length of the first rotation of the crank which indicates "the starting point G3 of the second reluctance 12 is used as the starting point". -22- 201033597 In the figure, in the case where the engine revolutions (rotation speed) Ne are the same, the crank angular velocity ω in the normal period is indicated by a solid line, and the crank angular velocity ω at a high load is indicated by a broken line. As shown in the figure, the variation of the angular velocity ω increases when the load is high. This is because, even in the case where the engine rotational speed Ne is the same, the higher the output torque, the larger the peak speed of the angular velocity ω, and the larger the amount of the subsequent increase is when the intake air amount is larger. φ, the fluctuation of the angular velocity ω of the crank becomes larger as the "lower rotation region where the inertial force of the crankshaft becomes smaller" becomes larger, and the number of cylinders is smaller and the burst interval is larger as in the single cylinder engine 1 of the present embodiment. In the engine, there is a tendency to become bigger. Fig. 6 is a partially enlarged view of Fig. 5. As described above, the load state of the engine 1 is detected by the load rate F of the engine. The load factor F is a degree of reduction in the angular velocity ω with respect to the engine revolution Ne in the section D1 including the compression top dead center, in other words, the magnitude of the compression resistance in the compression stroke is reduced. . In the present embodiment, the second magnetic resistance 12 is a variation between the angular velocity rotdc and the engine rotational speed Ne when the second magnetic reluctance 12 passes through the magnetic pickup 20 in the section D1, and is a variation of the angular velocity ω. Δω is calculated. The cotdc section in the figure corresponds to the transit time from the start point G3 of the second reluctance 12 to the end point G4. Hereinafter, referring to Figures 7, 8, and 9, the weighting process for "correctly detecting the load factor F at the time of transition" will be described. The weighting process is a method of dividing the detection area -23-201033597 into a plurality of pieces when calculating the engine rotation speed Ne in the detection section, and calculating the section engine rotation speed of each of the division sections, When the interval engine rotation speed is averaged, the weighting of a certain segmentation interval is increased, and NeA is adjusted to an appropriate frame. Fig. 7 is a graph showing changes in the angular velocity ω in the general period and the transition period. The Τ in the figure is the TDC (top dead center). (a) The angular velocity ω of one of the general periods shown is the same between the upper limit 値 and the lower limit 各 in each stroke. Therefore, the detection section for calculating "the engine rotation speed Ne used in the calculation of the aforementioned Δω" is sufficient as long as it is set to a period of one cycle amount. Even in the example of the figure, the crankshaft is rotated twice from the start point G1 of the first magnetic resistance 11, that is, the interval of one cycle is used as the detection section. However, with respect to the general period of (a), although the angular velocity ω of the transition period shown in (b) is substantially the same variation (forms substantially the same waveform) every one cycle, the angular velocity ω reaches the peak. After a slight downward change, the continuity will increase toward the next peak. As a result, the waveform of the angular velocity ω of the transition period will form a stepped shape that rises toward the right side. At this time, for example, when the engine rotation speed is the same in the general period and the transition period, once the aforementioned engine load factor F is calculated for the above two, the load factor F of the transition period will be calculated to be smaller than the normal period' A phenomenon that does not actually correspond to the load state generated by the engine is derived. This is due to the fact that Δω of the transition period compared to the actual engine load state is calculated to be smaller, as will be explained in more detail later. In order to cope with the above problem, in the present embodiment, the premise is that the detection section is divided into N e from the start point G 1 of the first reluctance 1 1 and -24-201033597 to the crankshaft rotation once. 1 interval; and Ne2 interval from the end point of the N e 1 section to the crankshaft rotating once again, and the section engine rotation speed Nel (hereinafter referred to as "Nel") in the Nel section The average engine rotation speed Ne (hereinafter referred to as NeA) of the entire detection section is calculated by the average 値 between the interval engine rotation speed Ne2 (hereinafter referred to as Ne2) in the Ne2 section. The above calculation processing is executed by the aforementioned Ne calculation means 52. Fig. 8 is a graph showing the relationship between the angular velocity ω in the transition period and the detection interval. The same reference numerals as described above are the same or equivalent parts. As described earlier, in the transition period, the interval from the intake stroke to the first half of the compression stroke, that is, the decrease in the angular velocity ω in the Ne 1 interval is small, which is almost in the example shown in the figure. Move horizontally. On the other hand, in the latter half of the compression stroke, after the angular velocity ω is greatly lowered, the peak value is greatly increased in the combustion-expansion stroke. Here, as described earlier, the engine load factor F is a result calculated based on "the degree of decrease of the crankshaft angular velocity ω with respect to the engine rotational speed Ne in the latter half of the compression stroke". However, in this calculation method, the difference ' ' between the engine rotation speed Ne and 〇) tdc when the general period is the same as the engine rotation speed Ne in the transition period is also referred to as A (〇(A〇i&gt; = Ne -G)tdc) is a tendency that the transition period will be calculated to be smaller than the general period. This is because the Ne2' of the Ne2 interval containing the cotdc interval is very large compared to the general period, and the calculation of the load factor F should pay attention to the elements of -25-201033597, but because of the calculation of the average 値 of Nel and Ne2 And was offset. As a result, the load factor F calculated during the transition period will be calculated to be less than the actual engine load state. Therefore, in the transition period, when calculating the average engine rotation speed NeA, it is preferable to reflect the magnitude of the engine rotation speed Ne2. Thus, in the example of the figure, when NeA is calculated, different weighting processing is performed between Nel and Ne2. In the illustrated example, the calculation formula of the average engine rotational speed NeA between one cycle is set to: NeA = Nel x(l - Q a) + Ne2xa, and by setting the weighting coefficient α to be greater than 0.5. So that the weight of Ne2 is greater than Nel and the NeA is raised as a whole. The weighting means for performing the weighting processing is included in the Ne calculating means 52 (refer to Fig. 2) of the load factor calculating unit 50. Here, a glimpse of the weighting process of FIG. 9 is referred to. In the illustrated example, the average engine rotation speed when the weighting process is not performed is represented by NeAO (dashed line), and the average engine rotation speed when the weighting process has been performed (for example, α = 0·55) is NeA (solid line) )To represent. At this time, the amount of fluctuation of the crank angle ω speed ω is increased by Δω when the weighting process is performed with respect to ΔωΟ calculated in the case where the weighting process is not performed (refer to Fig. 8). As a result, the calculation of the engine load factor F will also increase, and the load rate F corresponding to the actual engine load state can be calculated during the transition period. In the general period, even in the case where the above-described weighting processing has been performed, the influence on the load factor F is small because the difference between Nel and Ne2 is small.

不大。因此,無須在一般時期與過渡時間中變換負載率F -26- 201033597 的計算方法,不會增加計算處理的負擔。 第10圖,是顯示加權係數α之導出方法的圖表。如 先前所述,在一般時期中,即使令加權係數α變動,Αω 的値也幾乎不會改變。相對於此,在過渡時期中,Δω將 隨著加權係數α的增大而增加。此時,一旦將加權係數α 設置在「過渡時期的Δω與一般時期的Δω —致的點」時 ,在cotdc爲相同値的場合中,可使一般時期與過渡時期 φ 的負載率F形成相同的値。 如上所述,根據本發明的引擎負載檢測裝置,由於當 求取「用於負載率F(F = Aco + NeAxl00)之計算」的平均引擎 旋轉速度NeA時,是將用來檢測NeA的特定區間設成1 個週期量的長度,並將該特定區間分割成:包含進氣行程 的Nel區間、與包含燃燒-膨脹行程的Ne2區間,而計算 各個的區間引擎旋轉速度Nel、Ne2,採用「對Ne2的加 權大於Nel」的方式來執行加權處理並計算兩個値的平均 Φ 値,因此可使「計算負載率F時應被重視的Ne2區間之區 間引擎旋轉速度Ne2」的大小反映於負載率F的計算値, 而能計算適當的引擎負載。如此一來,即使在因加速中或 行走於凹凸路面時而使引擎旋轉速度的變動增大的場合中 ,也能利用計算來求取對應於上述狀況的引擎負載。 而引擎與脈衝轉子的構造、磁阻的尺寸或數量、磁阻 相對於脈衝轉子的位置、磁阻相對於TDC位置的位置、 加權係數α的値、用來檢測平均引擎旋轉速度NeA之特定 期間的設定等,並不侷限於上述的實施形態,可以有各種 -27- 201033597 的變更。此外,本發明的引擎負載偵測裝置’除了機車之 類的車輛用引擎以外,也能適用於各種汎用引擎等。 接著,說明本發明之引擎負載檢測裝置所採用的磁阻 公差消除方法。該磁阻公差消除方法,是藉由利用上述的 加權處理、及在包含進氣行程的區間內曲柄角速度ω直線 性的推移(請參考第4圖),而在計算平均引擎旋轉速度 NeA的計算式内,降低磁阻部分之尺寸公差的影響’換言 之,可降低尺寸公差對「最終所算出之負載率F」的影響 。以下,採用第10〜13圖來說明具體的手法。 第11圖,是顯示使用磁阻公差消除方法時的檢測區 間、與前述Ne 1區間及Ne2區間之間的關係的說明圖。在 本實施形態中,是將從第2磁阻的起點G3起直到曲柄旋 轉1次爲止的範圍設成D4區間,並計算該D4區間中的 平均引擎旋轉速度NeA。D4區間是位在:相對於前述的 Nel及Ne2,僅向後偏移第3角度Θ3(在本實施形態中爲 22.5度)的位置。在本實施形態中,該D4區間更進一步被 被分割爲®tdc區間(45度)與ω4區間(3 1 5度)。上述的區 間設定,是由前述的Ne計算手段52所執行。 第12圖,是顯示過渡時期中的角速度ω與檢測區間 之關係的圖表。與前述相同的圖號,是表是相同或者相等 的部分。在該圖中,是將包含燃燒-膨脹行程的D4區間 作爲 D4(n)區間,並將該曲柄旋轉1次前的區間作爲 D4(n-1)區間。換言之,用來計算平均引擎旋轉速度NeA 的檢測區間,爲D4(n-1)區間及D4(n)區間。此外,相對於 201033597 此’ ω4區間是分別設定於:作爲第2區間的ω4(η)區間、 及作爲第1區間的ω4(η-1)區間。不僅如此,(〇tdc區間是 分別設定於:作爲第2磁阻區間的c〇tdC2區間、及作爲第 1磁阻區間的ω t d c 1區間。 在此,於上述的區間設定中,是考察了用來計算檢測 區間内之平均引擎旋轉速度NeA的方法。最好是執行可適 當地反應下述特性的區間設定,而前面所述的特性是指: # 如先前所描述,在過渡時期的加權處理中,「曲柄角速度 ω,在從進氣行程起,到壓縮行程之前半段的範圍間,形 成直線性且幾乎不會減少的推移,而在燃燒-膨脹行程中 則急速地上升」的特性。如此一來,平均引擎旋轉速度 NeA便形成:藉由ω4(η-1)區間的區間引擎旋轉速度ω4(η-1) 、與ω4(η)區間的區間引擎旋轉速度ω4(η)之間的平均値, 所算出的結果。 根據以上所述,已考慮了加權之NeA的計算式便成爲 • : ΝβΑ = (1-α)χω4(η-1) + αχω4(η)。在本實施形態中,該 NeA並非「最後所算出的平均引擎旋轉速度NeA」,而是 被定義爲第1平均値H1。雖然加權係數a的値可任意設 定,但在一般時期中,即使變動加權係數α,Αω的値也幾 乎不會改變。相對於此,在過渡時期中,Δω將隨著加權 係數a的增大而增加。此時,加權係數a爲:倘若將過渡 時期的Δω設定在與一般時期之Αω —致的點,在totdc爲 相同値的場合中,可使負載率F形成相同値。 接下來,一倂參考第13圖來說明計算Δω的計算式。 -29- 201033597 如同先前所描述,由於A(〇=Ne-〇)tdc,一旦將該關係應用 於第12圖所示的範例中,便形成A(〇 = NeA-(〇tdc2。在此, 機械零件容許尺寸公差(譬如,±1%),而使第2磁阻12的 圓周方向尺寸中產生因尺寸公差所造成的尺寸偏移。以下 ,說明該圓周方向尺寸的偏移對Δω的計算値所造成的影 響。 在第2磁阻12之圓周方向長度已形成偏移的場合中 ,雖然前述NeA的計算値中也產生偏移,但在此是假定 ❹ NeA中不包含尺寸公差的影響。在上述的條件中,於 NeA = 2000(rpm)、(〇tdc2=1800(rpm)的場合中,第 2 磁阻 12 的圓周方向尺寸爲基準値之場合中的Αω形成:^(〇 = 2000-1 8 00 = 2 00(rpm)。相對於此,第2磁阻12的圓周方向尺寸 是較基準値大1 %,如此一來在ω t d c 2小1 %的場合中,便 形成A(〇 = 2000-1782 = 218(rpm)。換言之,在第2磁阻12之 圓周方向尺寸中產生1 %的偏移,將導致在Αω的計算値中 被增幅(放大)成10%的明顯差異。 β 爲了避免上述尺寸公差的增幅,採用「在與ωί(1&lt;ϊ2相 同的45度區間所計算」的旋轉速度來表示NeA即可。只 要實現該條件,由於A®的計算式是形成「在相同的45度 區間內所計算之旋轉速度間的減法運算」,而消除「Δω 的計算値對基準値形成1 %以上偏移」的情況。根據以上 的說明,在本實施形態中’是對N e Α的計算式稍作修正’ 而能兼顧以下3點:極力延長用來計算N e A的檢測區間’ 而提高NeA的正確性;和藉由加權處理,將NeA調整爲 -30- 201033597 適當値;及降低第2磁阻12的尺寸公差對Δω所造成的影 響。 具體地說,是對「已考慮了加權的®4(η-1)區間、與 ω4(η)區間」的Ne平均値(第1平均値Η1)乘以「通常是形 成1的値」。而該所謂「通常是形成1的値」是指: ω4(η-1)區間的旋轉速度的近似値K,除以在ω4(η-1)區間 所實際計測的旋轉速度co4(n-l)的値。 前述的近似値K,是利用「在進氣行程中,曲柄角速 度ω直線性推移」的特性所算出。換言之,所謂的近似値 Κ是採用下述的旋轉速度來表示,前述的旋轉速度是藉由 「在(otdcl區間(45度區間)所計算的第1磁阻旋轉速度 ootdcl、與在cotdc2區間(45度區間)所計算的第2磁阻旋 轉速度(〇tdc2」的平均値,並以45度區間來計算「3 15度 區間之ω4(η-1)區間的旋轉速度」的旋轉速度。在本實施 形態中,該近似値Κ被定義爲第2平均値Η2。 接著,近似値Κ(第2平均値Η2)爲:一旦除以「在 ω4(η-1)區間所計算的第1旋轉速度ω4(η-1)」,便成爲「1 」的値。換言之,圖面中框内的NeA是成爲:對第1平均 値Η1乘以「形成1的値」的計算値。 接著,在執行NeA的計算時,第1平均値Η1所包含 的ω4,是除以分母中的ω4而被消除。換言之,315度區 間的尺寸公差形成:從圖示的框中消滅。如此一來,雖然 在NeA中僅殘存著45度區間的尺寸公差,但由於該尺寸 公差,是與圖示中框外的cot dc2相同之45度區間的尺寸 -31 - 201033597 公差,因此Aco=NeA-cotdc2的計算式,便形成相同的45 度區間內的減法運算。因此,尺寸公差的影響將由於減法 運算而不會被增幅,如此一來可計算出尺寸公差之影響極 小的Δω及負載率F。 而上述Δω的計算方法,並不僅限於過渡時期,一般 時期也同樣能適用。此外,在上述Αω及負載率F的計算 中,亦可不設置脈衝轉子10的第1磁阻11 (請參考第3圖 ❿ : 的 於差 由公 , 寸 置尺 裝有 測具 檢中 載度 負長 擎向 引方 的周 明圓 發的 本阻 據磁 根之 ’ 子 述轉 所衝 上脈 如是 使 即 場合,在計算NeA的計算式中,是藉由對315度區間的旋 轉速度乘以「通常是形成1」的値,並將該結果轉換成45 度區間的旋轉速度,並在該轉換之際,藉由除法運算而將 315度區間的尺寸公差予以消除,因此可防止計算 △ («(△i〇 = NeA-G)tdC2)時尺寸公差的影響被增幅(放大)。如此 一來,可以將磁阻之公差尺寸對「引擎之負載率F的計算 値」的影響抑制成最小限度。 具體地說,首先,在求取「計算負載率F(F = Ao^NeAxl00) 所使用之平均引擎旋轉速度NeA」之際,是將用來計算該 NeA的檢測區間設定成:曲柄軸從第2磁阻1 2之通過開 始點G3起開始旋轉2次的量的長度。接著,將該檢測區 間分割成4個區間,而該4個區間是由以下所形成:分別 對應於第2磁阻12通過磁性拾取器20之位置的第1磁阻 區間(totdcl區間)與第2磁阻區間(〇)tdC2區間);及分別對 -32- 201033597 應於第2磁阻1 2未通過磁性拾取器20之位置的第1區間 (ω4(η-1)區間)與第2區間(ω4(η)區間)。 在此,參考第14圖。該圖是以塊狀圖的方式來表示 平均引擎旋轉速度NeA的計算步驟。在第1平均値計算部 104中,計算「由第1旋轉速度偵測部1 〇〇所檢測的第1 旋轉速度ω4(η-1 )、與由第2旋轉速度偵測部1 0 1所檢測 的第2旋轉速度ω4(ιι)」之平均値的第1平均値Η1。另外 φ ,在第2平均値計算部1〇5中’計算「由第1磁阻旋轉速 度偵測部102所檢測的第1磁阻旋轉速度〇)tdCl、與由第 2磁阻旋轉速度偵測部1 〇3所檢測的第2磁阻旋轉速度 〇)tdc2」之平均値的第2平均値H2(近似値K)。接下來, 在平均引擎旋轉速度計算部中,採用由第1平均値計 算部104所計算的第1平均値H1、和由第2平均値計算 部105所計算的第2平均値H2、及第1旋轉速度ω4(η-1) ,來計算平均引擎旋轉速度NeA。如此一來,可在NeA的 Φ 計算式中將315度區間的尺寸公差予以消除,並在計算 Αω時(Δω = ΝεΑ-ωί(1ς2)避免尺寸公差增幅(放大)。 再者,曲柄角速度的變動狀態,容易受到「從曲柄軸 直到後輪爲止之扭力傳動系統」的影響,這點可藉由實驗 等而獲得證明。因此,爲了更精確地計算引擎負載率,最 好將該扭力傳動系統的影響列入考慮。以下,說明已將「 曲柄角速度的變動狀態,特別是變速機的變速比受到影響 的狀態」列入考慮之引擎負載率的計算方法(修正方法)。 第圖,是顯示引擎旋轉速度Ne與Δω的計算値 -33- 201033597 (△to = Ne-totdc)間之關係的圖表。該圖表是根據「具有4段 變速式之變速機」的引擎所做的實測試驗而作成的圖表。 如先前所述,曲柄角速度的變動量Αω’是當引擎轉數Ne 越小時,也就是當越靠近「曲柄軸的慣性力變小」的低旋 轉區域時則變大。而具有以下的傾向:特別是越靠近低旋 轉區域時,因變速比的差異所造成的影響將變大。在該圖 表的範例中,將隨著變速比從「變速比最低」的4檔齒輪 (實線)起、3檔齒輪(一點鎖線)、2檔齒輪(虛線)、1檔齒 ❹ 輪(二點鎖線)的變大,而使Αω的計算値變小。這是表示 :譬如引擎轉數Ne爲相同的値,且即使引擎的實際負載 狀態相同,變速比越大的話,Δω將被計算成越小的傾向 。因此,當變速機的變速比越大,且引擎轉數Ne越低時 ,當計算引擎負載率之際,產生了所謂「所計算的結果低 於實際的負載狀態」的課題。 有鑑於此,本實施形態的特徵在於:爲了降低上述變 速比的差異對Αω所造成的影響,而構成對應於變速機的 @ 變速比來修正Αω的値。在本實施形態中,是藉由作爲變 速比偵測手段的齒輪位置感應器,來檢測現今所選擇的變 速比(變速檔位),並藉由將對應於該變速比的修正係數, 應用於「計算Δω時所使用的(〇tdc」而執行修正。更具體 地說,是藉由對Δω之計算式(Aco = Ne-(〇tdc)所包含的cotdc 乘以修正係數K,來執行修正(A(〇 = Ne-Kxcotdc)。 第16圖,是顯示引擎轉數Ne及變速檔位(齒輪位置) 、與修正係數K間之關係的修正係數圖。在本實施形態中 -34- 201033597 ,當選擇「變速比最小的4檔齒輪」時不執行(otdc的修 正,且不管引擎轉數Ne的値爲多少,而將修正係數K設 定爲1.0。另外,將修正係數K設定成:隨著變速檔位3 、2、1檔而使變速比變大,修正係數K的値也變大。 在此,如第15圖所示,變速比的差異對Δω所造成的 影響,是隨著引擎轉數Ne的增加而變小。如此一來,修 正係數K的値也被設定成:隨著引擎轉數Ne的增加而變 φ 小。該修正係數圖,除了是根據預先實驗等所設定之外, 還被記憶在前述ECU30内的負載率計算部50(請參考第2 圖)。 第17圖,是顯示採用修正係數K之Αω的修正控制 之步驟的流程圖。在步驟S200中,是由齒輪位置感應器 來檢測齒輪位置GP。接著在步驟S201中,檢測引擎轉數 Ne。在步驟S202中,採用齒輪位置GP與引擎轉數Ne, 從修正係數圖(請參考第16圖)導出修正係數K。接著,在 ® 步驟S203中,將所導出的修正係數K應用於Δω的計算 (Δω=Νβ-Κχ rotdc) &gt;如此一來,便形成Δω修正値的計算 。根據上述Δω的修正控制,可形成較對應於變速機之變 速比更精確的引擎負載予測,可更緊密且更精確地執行點 火時期控制等,而達成燃料費用的降低、有害之排放氣體 的降低等。 然而,雖然在上述實施形態中,是利用齒輪位置感應 器來檢測有段變速機的變速檔位而導出修正係數Κ,但譬 如在「利用皮帶轉換器(belt converter)之無段變速機」的 -35- 201033597 場合中,也可以構成:爲了變更變速比,根據所驅動之皮 帶輪的移動量來檢測變速比,並對應於該變速比來導出修 正係數K。 此外,也可以根據車速與引擎轉數來計算變速比,並 對應於該變速比來導出修正係數。根據該構造,可以不需 要用來檢測變速檔位的位置感應器,而可期待成本的降低 〇 而引擎與脈衝轉子的構造、磁阻的尺寸或數量、磁阻 ® 相對於脈衝轉子的位置、磁阻相對於TDC位置的位置、 加權係數α的値、用來檢測平均引擎旋轉速度NeA之特定 期間的設定等,並不侷限於上述的實施形態,可以有各種 的變更。此外,本發明之引擎負載偵測裝置所採用的磁阻 公差消除方法,除了機車之類的車輛用引擎以外,也能適 用於各種汎用引擎等。 【圖式簡單說明】 Θ 第1圖:是採用「本發明其中一種實施形態的引擎負 載檢測裝置」之引擎1的構造圖。 第2圖:是顯示「被設於ECU的負載率計算部50之 細部」的塊狀圖。 第3圖:是脈衝轉子10的放大正視圖。 第4圖:是顯示曲柄脈衝訊號、與引擎轉數Ne、與 角速度ω間之關係的圖表。 第5圖:是顯示在1個週期中曲柄脈衝訊號與角速度 -36- 201033597 ω間之關係的圖表。 第6圖:是第5圖的局部放大圖。 第7圖:是顯示一般時期及過渡時期中角速度ω之變 動的圖表。 第8圖:是顯示過渡時期中角速度ω與檢測區間之間 的關係的圖表。 第9圖:爲加權處理的槪念圖。 第10圖:是顯示加權係數α之導出方法的圖表。 第11圖:是顯示使用磁阻公差消除方法時的檢測區 間、與Nel區間及Ne2區間之間的關係的說明圖。 第12圖:是顯示過渡時期中角速度ω與檢測區間之 關係的圖表。 第13圖:是顯示用來計算Δω之計算式的說明 第14圖:是顯示平均引擎旋轉速度NeA之計算步驟 的塊狀圖。 ® 第15圖:是顯示引擎旋轉速度Ne與Δω的計算値 (Aco = Ne-a)tdc)間之關係的圖表。 第1 6圖:是顯示引擎轉數Ne及變速檔位、與修正係 數K間之關係的修正係數圖。 第17圖:是顯示採用修正係數K之Λω的修正控制 之步驟的流程圖。 【主要元件符號說明】 1 :引擎 -37- 201033597 6 :點火裝置 7 :活塞 8 :汽缸 9 :曲柄軸 10 :脈衝轉子(pulsar rotor) 1 1 :第1磁阻 12 :第2磁阻Not big. Therefore, it is not necessary to change the calculation method of the load factor F -26- 201033597 in the general period and the transition time, and the burden of the calculation processing is not increased. Fig. 10 is a graph showing a method of deriving the weighting coefficient α. As described earlier, in the general period, even if the weighting coefficient α is changed, the Α Α 値 is hardly changed. In contrast, in the transition period, Δω will increase as the weighting coefficient α increases. In this case, when the weighting coefficient α is set to "the point of Δω in the transition period and the point Δω in the normal period", when the cotdc is the same, the load rate F of the general period and the transition period φ can be made the same. Hey. As described above, the engine load detecting device according to the present invention is a specific section to be used for detecting NeA when the average engine rotational speed NeA for "calculation of the load factor F (F = Aco + NeAxl00)" is obtained. The length of one cycle is set, and the specific section is divided into a Nel section including an intake stroke and a Ne2 section including a combustion-expansion stroke, and each section engine rotation speeds Nel and Ne2 are calculated, and "pair" is used. The weighting of Ne2 is greater than Nel" to perform the weighting process and calculate the average Φ 値 of the two 値, so that the magnitude of the interval engine rotation speed Ne2 of the Ne2 interval that should be considered when calculating the load factor F can be reflected in the load ratio. The calculation of F is 値, and the appropriate engine load can be calculated. In this manner, even when the fluctuation of the engine rotational speed is increased during acceleration or when traveling on the uneven road surface, the engine load corresponding to the above situation can be obtained by calculation. The structure of the engine and the pulse rotor, the size or number of reluctances, the position of the reluctance relative to the pulse rotor, the position of the reluctance relative to the TDC position, the 加权 of the weighting coefficient α, and the specific period for detecting the average engine rotational speed NeA The setting and the like are not limited to the above-described embodiments, and various changes can be made to -27-201033597. Further, the engine load detecting device of the present invention can be applied to various general-purpose engines and the like in addition to the engine for a vehicle such as a locomotive. Next, a method of eliminating the magnetoresistance tolerance employed in the engine load detecting device of the present invention will be described. The magnetoresistance tolerance elimination method calculates the average engine rotation speed NeA by using the above-described weighting processing and linearity of the crank angular velocity ω linearity in the section including the intake stroke (refer to FIG. 4). In the formula, the influence of the dimensional tolerance of the magnetoresistive portion is reduced. In other words, the influence of the dimensional tolerance on the "final calculated load factor F" can be reduced. Hereinafter, specific methods will be described using Figs. 10 to 13. Fig. 11 is an explanatory view showing the relationship between the detection area and the Ne 1 section and the Ne2 section when the magnetoresistive tolerance elimination method is used. In the present embodiment, the range from the start point G3 of the second reluctance until the crank is rotated once is set to the D4 section, and the average engine rotation speed NeA in the D4 section is calculated. The D4 section is located at a position shifted by the third angle Θ3 (22.5 degrees in the present embodiment) with respect to Nel and Ne2 described above. In the present embodiment, the D4 section is further divided into a ®tdc section (45 degrees) and an ω4 section (3 1 5 degrees). The above-described interval setting is performed by the aforementioned Ne calculating means 52. Fig. 12 is a graph showing the relationship between the angular velocity ω and the detection interval in the transition period. The same figure numbers as described above are the parts in which the tables are the same or equal. In the figure, the D4 section including the combustion-expansion stroke is referred to as the D4(n) section, and the section before the crank is rotated once is referred to as the D4(n-1) section. In other words, the detection interval for calculating the average engine rotation speed NeA is the D4 (n-1) interval and the D4 (n) interval. Further, the 'ω4 section is set to the ω4 (η) section as the second section and the ω4 (η-1) section as the first section, respectively, with respect to 201033597. In addition, the 〇tdc section is set to the c〇tdC2 section which is the second magnetoresistive section and the ωtdc1 section which is the first magnetoresistive section. Here, in the above section setting, it is examined. A method for calculating the average engine rotational speed NeA in the detection interval. It is preferable to perform interval setting that appropriately reflects the following characteristics, and the aforementioned characteristics are: # as previously described, weighting during the transition period During the processing, "the crank angular velocity ω is linearly increased from the intake stroke to the half of the compression stroke, and the transition is almost constant, and the combustion-expansion stroke rises rapidly." In this way, the average engine rotation speed NeA is formed by the interval engine rotation speed ω4(η-1) and the interval engine rotation speed ω4(η) of the ω4(η) interval in the ω4(η-1) interval. The average 値 between the calculated results. According to the above, the calculation formula of the weighted NeA has been considered to become: ΝβΑ = (1−α)χω4(η-1) + αχω4(η). In this implementation In the form, the NeA is not the last calculated The average engine rotation speed NeA" is defined as the first average 値H1. Although the 加权 of the weighting coefficient a can be arbitrarily set, in the general period, even if the weighting coefficient α is changed, the Αω 几乎 is hardly changed. In contrast, in the transition period, Δω will increase as the weighting coefficient a increases. At this time, the weighting coefficient a is: if the Δω of the transition period is set at a point corresponding to Αω of the general period, In the case where totdc is the same ,, the load factor F can be made the same 値. Next, the calculation formula for calculating Δω will be described with reference to Fig. 13. -29- 201033597 As described earlier, since A(〇=Ne- 〇)tdc, once the relationship is applied to the example shown in Figure 12, A is formed (〇= NeA-(〇tdc2. Here, the tolerance tolerance of mechanical parts (for example, ±1%), 2 The dimensional deviation due to the dimensional tolerance occurs in the circumferential dimension of the magnetic resistance 12. Hereinafter, the influence of the deviation of the circumferential dimension on the calculation of Δω will be described. The length of the second magnetic resistance 12 in the circumferential direction In the case where an offset has been formed, although The calculation of NeA also produces an offset, but here it is assumed that ❹ NeA does not contain the influence of dimensional tolerance. In the above conditions, in the case of NeA = 2000 (rpm), (〇tdc2 = 1800 (rpm) In the case where the circumferential dimension of the second reluctance 12 is the reference Α, Α ω is formed: ^ (〇 = 2000-1 8 00 = 2 00 (rpm). In contrast, the circumferential dimension of the second reluctance 12 is It is 1% larger than the reference ,, so that in the case where ω tdc 2 is 1% smaller, A is formed (〇 = 2000-1782 = 218 (rpm). In other words, a 1% offset in the circumferential dimension of the second reluctance 12 results in a significant difference of 10% increase (amplification) in the calculation Α of Αω. β In order to avoid the above-mentioned increase in the dimensional tolerance, it is sufficient to use the "rotation speed calculated by the same 45 degree interval as ωί(1&lt;2) to represent NeA. As long as this condition is achieved, the calculation formula of A® is formed. In the same 45-degree interval, the subtraction between the rotational speeds is calculated, and the case where "the calculation of Δω is performed and the reference 値 is shifted by 1% or more" is eliminated. According to the above description, in the present embodiment, 'is right The calculation formula of N e 稍 is slightly modified 'and can take the following three points: try to extend the detection interval used to calculate N e A to improve the correctness of NeA; and adjust the NeA to -30- 201033597 by weighting It is appropriate to reduce the influence of the dimensional tolerance of the second magnetic resistance 12 on Δω. Specifically, it is the Ne of the "4 (η-1) interval and the ω4 (η) interval in which the weighting has been considered. The average 値 (1st average 値Η 1) is multiplied by "usually the 値 which forms 1", and the so-called "usually the 値 which forms 1" means: the approximate 値K of the rotational speed of the ω4 (η-1) interval, except The 旋转 of the rotational speed co4(nl) actually measured in the ω4(η-1) interval. The approximate 値K described above is calculated by the characteristic of "the crank angular velocity ω linearly shifts during the intake stroke." In other words, the approximate 値Κ is expressed by the following rotational speed, and the aforementioned rotational speed is borrowed. "the average of the first reluctance rotational speed ootdcl calculated in the otdcl interval (45 degree interval) and the second reluctance rotational speed (〇tdc2" calculated in the cotdc2 interval (45 degree interval), and The rotation speed of the "rotation speed of the ω4 (η-1) section of the 3 15 degree section" is calculated in the 45-degree section. In the present embodiment, the approximate 値Κ is defined as the second average 値Η 2. Next, the approximate 値Κ (2nd average 値Η2): When the first rotation speed ω4(η-1) calculated in the ω4(η-1) section is divided, it becomes 1 of "1". In other words, the middle frame of the drawing In the NeA, the calculation is performed by multiplying the first average 値Η1 by "the 形成 which forms one." Next, when the calculation of NeA is performed, ω4 included in the first average 値Η1 is divided by ω4 in the denominator. And is eliminated. In other words, the dimensional tolerance of the 315 degree interval is formed: it is eliminated from the box in the illustration As a result, although the dimensional tolerance of the 45-degree interval remains in the NeA, since the dimensional tolerance is the same as the size of the 45-degree interval of the cot dc2 outside the frame shown in the figure -31 - 201033597, the Aco= The calculation formula of NeA-cotdc2 forms the same subtraction in the 45 degree interval. Therefore, the influence of the dimensional tolerance will not be increased due to the subtraction operation, so that the influence of the dimensional tolerance on the Δω and the load can be calculated. The rate F. The calculation method of the above Δω is not limited to the transition period, and the general period is also applicable. Further, in the calculation of the above Αω and the load factor F, the first magnetoresistive resistor 11 of the pulse rotor 10 may not be provided (please refer to FIG. 3: the difference is from the public, and the inch is equipped with the gauge to check the medium load. In the calculation formula of the NeA, the rotation speed of the 315 degree interval is multiplied by the rotation speed of the 315 degree interval. "Normally forming a 1", and converting the result into a rotation speed of 45 degrees, and at the time of the conversion, the dimensional tolerance of the 315 degree interval is eliminated by the division operation, thereby preventing the calculation of Δ ( «(△i〇= NeA-G)tdC2) The influence of the dimensional tolerance is increased (amplified). In this way, the influence of the tolerance of the magnetic resistance on the "calculation of the load factor F of the engine" can be minimized. Specifically, first, when the "average engine rotational speed NeA used for calculating the load factor F (F = Ao^NeAxl00)" is obtained, the detection interval for calculating the NeA is set to: crank axis Rotating from the start point G3 of the second reluctance 1 2 The length of the second time is divided into four sections, and the four sections are formed by the first magnetoresistance corresponding to the position of the second magnetoresistive resistor 12 passing through the magnetic pickup 20, respectively. Interval (totdcl interval) and second magnetoresistive interval (〇) tdC2 interval); and respectively -32-201033597 should be in the first interval of the position where the second magnetoresistive resistor 12 does not pass the magnetic pickup 20 (ω4(η- 1) Interval) and the second interval (ω4(η) interval). Here, reference is made to Fig. 14. This figure is a calculation step of representing the average engine rotation speed NeA in the form of a block diagram. The first average chirp calculating unit 104 calculates "the first rotational speed ω4 (η-1) detected by the first rotational speed detecting unit 1" and the second rotational speed detecting unit 1 0 1 The first average 値Η1 of the average 値 of the detected second rotational speed ω4(ιι). Further, φ is 'calculated by the second average 値 calculating unit 1〇5', the first magnetic reluctance rotational speed detected by the first reluctance rotational speed detecting unit 102, tdCl, and the second reluctance rotational speed. The second average 値H2 (approx. 値K) of the average 値 of the second reluctance rotational speed 〇)tdc2" detected by the measuring unit 1 〇3. Next, the average engine rotation speed calculation unit uses the first average 値H1 calculated by the first average 値 calculation unit 104 and the second average 値H2 and the second average 値 calculation unit 105 calculated by the second average 値 calculation unit 105. 1 The rotational speed ω4(η-1) is used to calculate the average engine rotational speed NeA. In this way, the dimensional tolerance of the 315 degree interval can be eliminated in the Φ calculation formula of NeA, and the dimensional tolerance increase (amplification) is avoided when calculating Αω (Δω = ΝεΑ-ωί(1ς2). The state of change is easily affected by the "torque transmission system from the crankshaft to the rear wheel", which can be proved by experiments, etc. Therefore, in order to calculate the engine load rate more accurately, it is preferable to use the torque transmission system. The following is a description of the calculation method of the engine load factor (correction method) in which the "state of the angular velocity of the crank, especially the state in which the speed ratio of the transmission is affected" has been included. A graph showing the relationship between the engine rotation speed Ne and Δω, 値-33- 201033597 (△to = Ne-totdc). This chart is based on the actual test conducted by the engine of the "four-speed shifting machine". As described earlier, the variation of the crank angular velocity Αω' is the low rotation when the number of engine revolutions Ne is small, that is, the inertia force closer to the crankshaft becomes smaller. When the area is turned, it becomes larger. The tendency is that the closer to the low-rotation area, the influence due to the difference in the gear ratio becomes larger. In the example of the chart, the shift ratio is changed from "shifting" Compared with the lowest 4th gear (solid line), 3rd gear (one point lock line), 2nd gear (dashed line), 1st gear wheel (two point lock line), the calculation of Αω is reduced. This means that if the number of engine revolutions Ne is the same, and even if the actual load state of the engine is the same, the larger the gear ratio, the smaller the Δω will be calculated. Therefore, the gear ratio of the transmission is larger. When the engine revolution number Ne is lower, when the engine load factor is calculated, there is a problem that "the calculated result is lower than the actual load state". In view of this, the present embodiment is characterized in that in order to reduce the above The difference in the gear ratio affects Αω, and constitutes a 变速 corresponding to the @ gear ratio of the transmission to correct Αω. In the present embodiment, it is detected by a gear position sensor as a gear ratio detecting means. now The selected gear ratio (shift gear position) is applied to "(ttdc) used in the calculation of Δω by applying a correction coefficient corresponding to the gear ratio. More specifically, by Δω The calculation formula (Aco = Ne-(〇tdc) is multiplied by the correction coefficient K to perform the correction (A(〇= Ne-Kxcotdc). Figure 16 shows the engine revolution Ne and the shift position ( Correction coefficient diagram of the relationship between the gear position and the correction coefficient K. In the present embodiment -34-201033597, when the "fourth gear with the smallest gear ratio" is selected, the correction is not performed (the correction of otdc, regardless of the number of engine revolutions) The correction coefficient K is set to 1.0, and the correction coefficient K is set such that the gear ratio becomes larger as the shift position 3, 2, and 1 shifts, and the correction coefficient K becomes larger. . Here, as shown in Fig. 15, the influence of the difference in the gear ratio on Δω becomes smaller as the number of engine revolutions Ne increases. As a result, the 修 of the correction coefficient K is also set to become smaller as the number of engine revolutions Ne increases. The correction coefficient map is stored in the load factor calculation unit 50 (see FIG. 2) stored in the ECU 30 in addition to the preset experiment or the like. Fig. 17 is a flow chart showing the steps of the correction control using 修正ω of the correction coefficient K. In step S200, the gear position GP is detected by the gear position sensor. Next, in step S201, the engine revolution number Ne is detected. In step S202, the correction coefficient K is derived from the correction coefficient map (please refer to Fig. 16) using the gear position GP and the engine revolution number Ne. Next, in the step S203, the derived correction coefficient K is applied to the calculation of Δω (Δω = Νβ - Κχ rotdc) &gt; Thus, the calculation of the Δω correction 値 is formed. According to the above-described correction control of Δω, it is possible to form a more accurate engine load prediction corresponding to the speed ratio of the transmission, and it is possible to perform ignition timing control and the like more closely and more accurately, thereby achieving a reduction in fuel cost and a reduction in harmful exhaust gas. Wait. However, in the above embodiment, the gear position sensor is used to detect the shift position of the stepped transmission to derive the correction coefficient Κ, but for example, in the "segmentless transmission using a belt converter" In the case of changing the speed ratio, the speed ratio is detected based on the amount of movement of the driven pulley, and the correction coefficient K is derived in accordance with the speed ratio. Further, the gear ratio may be calculated based on the vehicle speed and the engine revolution number, and the correction coefficient may be derived corresponding to the gear ratio. According to this configuration, the position sensor for detecting the shift position can be eliminated, and the cost reduction can be expected, and the configuration of the engine and the pulse rotor, the size or the number of the reluctance, the position of the reluctance® with respect to the pulse rotor, The position of the magnetic resistance with respect to the TDC position, the 加权 of the weighting coefficient α, the setting of the specific period for detecting the average engine rotational speed NeA, and the like are not limited to the above-described embodiments, and various modifications are possible. Further, the reluctance tolerance eliminating method employed in the engine load detecting device of the present invention can be applied to various general-purpose engines in addition to a vehicle engine such as a locomotive. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a structural diagram of an engine 1 using an "engine load detecting device of one embodiment of the present invention". Fig. 2 is a block diagram showing "details of the load factor calculation unit 50 provided in the ECU". Fig. 3 is an enlarged front elevational view of the pulse rotor 10. Fig. 4 is a graph showing the relationship between the crank pulse signal, the engine number Ne, and the angular velocity ω. Fig. 5 is a graph showing the relationship between the crank pulse signal and the angular velocity -36- 201033597 ω in one cycle. Fig. 6 is a partial enlarged view of Fig. 5. Fig. 7 is a graph showing changes in the angular velocity ω in the general period and the transition period. Fig. 8 is a graph showing the relationship between the angular velocity ω and the detection interval in the transition period. Figure 9: A mourning diagram for weighting. Fig. 10 is a graph showing a method of deriving the weighting coefficient α. Fig. 11 is an explanatory view showing the relationship between the detection area and the Nel section and the Ne2 section when the magnetoresistive tolerance elimination method is used. Fig. 12 is a graph showing the relationship between the angular velocity ω and the detection interval in the transition period. Fig. 13 is a view showing a calculation formula for calculating Δω Fig. 14 is a block diagram showing a calculation procedure of the average engine rotation speed NeA. ® Figure 15 is a graph showing the relationship between the engine rotation speed Ne and the calculation of Δω (Aco = Ne-a)tdc). Fig. 6 is a correction coefficient diagram showing the relationship between the engine revolution number Ne and the shift position and the correction coefficient K. Fig. 17 is a flow chart showing the steps of correction control using 修正ω of the correction coefficient K. [Main component symbol description] 1 : Engine -37- 201033597 6 :Ignition device 7 :Piston 8 : Cylinder 9 : Crankshaft 10 :Pulsar rotor 1 1 : 1st reluctance 12 : 2nd reluctance

20 :磁性拾取器(magnetic pickup) Q20 : Magnetic pickup Q

30 : ECU 40 :曲柄脈衝(crank pulse)檢測部 50 :負載率計算部 5 1 :計時器 52 : Ne計算手段 53 : Αω計算手段 54: (〇tdc計算手段 5 6 :負載率計算手段 © 60 :控制修正量計算部 7 0 :點火控制部 1〇〇 :第1旋轉速度偵測部 101 :第2旋轉速度偵測部 1 02 :第1磁阻旋轉速度偵測部 1 03 :第2磁阻旋轉速度偵測部 104 :第1平均値計算部 105 :第2平均値計算部 -38 201033597 部 算 計 度 速 轉 旋 擎 弓 均率 平載 : 負 G G G G Η Η K) 値 占 占 占 占 ^ 羅 a® sM aM 起終起終(¾ 的的的的値値 阻阻阻阻均均數 磁磁磁磁平平係 112 2 12ffi 第第第第第第加 度 速 角 柄 曲 ω 度 速 角 柄 曲 的 時 過 通 阻 磁 C d t ω30 : ECU 40 : crank pulse detecting unit 50 : load factor calculating unit 5 1 : timer 52 : Ne calculating means 53 : Α ω calculating means 54 : (〇tdc calculating means 5 6 : load factor calculating means © 60 : Control correction amount calculation unit 70: Ignition control unit 1A: First rotation speed detection unit 101: Second rotation speed detection unit 102: First reluctance rotation speed detection unit 103: Second magnetic Resistance rotation speed detecting unit 104: First average 値 calculation unit 105: Second average 値 calculation unit - 38 201033597 Partial calculation speed rotation rudder bow average rate flat load: Negative GGGG Η Η K) 値占占占占Luo a® sM aM from the end to the end (3⁄4 of the 値値 値値 阻 均 均 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 112 Time-varying magnetic resistance C dt ω

度度 速速 轉轉 旋旋 擎敬手 弓 弓 間間 區區 4,/- 間間 區區 1 2 e e N N 1 2 e e N NSpeed, speed, rotation, whirl, jingjing, bow, bow, room, area, 4, /-, area, 1 2 e e N N 1 2 e e N N

Ne A :特定區間的平均引擎旋轉速度 Αω :角速度變動量 • ω4(η-1):第1旋轉速度 ω4(η):第2旋轉速度 cotdcl :第1磁阻旋轉速度 cotdc2 :第2磁阻旋轉速度 NeA :檢測區間的平均引擎旋轉速度 -39 -Ne A : average engine rotation speed in a specific section Α ω : angular velocity variation amount • ω4 (η-1): first rotation speed ω4 (η): second rotation speed cotdcl : first reluctance rotation speed cotdc2 : second reluctance Rotation speed NeA: average engine rotation speed of the detection interval -39 -

Claims (1)

201033597 七、申請專利範圍: 1. 一種引擎負載檢測裝置,是具備:脈衝轉子,該脈 衝轉子是與引擎的曲柄軸同步旋轉;和磁阻,該磁阻被設 在該脈衝轉子,並位在對應於前述引擎之上死點附近的曲 柄角度;及拾取器,該拾取器是用來檢測該磁阻的通過; 並根據該拾取器的輸出訊號,來檢測引擎之負載狀態的引 擎負載檢測裝置, 其特徵爲: ⑩ 具備: 將用來檢測平均引擎旋轉速度的特定區間分割成複數 個,並根據前述拾取器的輸出訊號,分別計算該經分割的 複數個區間之各個區間的引擎旋轉速度的手段:和 加權手段,該加權手段是對前述複數個區間的引擎旋 轉速度執行不同的加權處理;及 負載狀態計算手段,該負載狀態計算手段是根據加權 處理後之複數區間引擎旋轉速度的平均値,計算前述平均 G 引擎旋轉速度,並使用該平均引擎旋轉速度來執行引擎之 負載狀態的計算。 2. 如申請專利範圍第1項所記載的引擎負載檢測裝置 ,其中前述加權處理,是在前述被分割成複數個的區間中 ,將包含燃燒一膨脹行程之區間的加權比率,設定成較其 他區間更大。 3 .如申請專利範圍第1或2項所記載的引擎負載檢測 裝置,其中前述特定區間,是根據前述脈衝轉子的輸出訊 -40- 201033597 號所檢測。 4. 如申請專利範圍第丨或2項所記載的引擎負載檢測 裝置’其中前述特定區間,是將前述曲柄軸之2次旋轉量 的長度2等分爲第1區間與第2區間,並設定成前述第! 區間包含進氣行程,前述第2區間包含燃燒一膨脹行程。 5. 如申請專利範圍第〗或2項所記載的引擎負載檢測 裝置’其中前述引擎的負載狀態,是前述磁阻通過前述拾 Φ 取器期間的旋轉速度,除以前述平均引擎轉數所算出的負 載率。 6. 如申請專利範圍第5項所記載的引擎負載檢測裝置 ’其中前述磁阻是被配設在即將到達引擎之上死點時的置 &gt; 前述負載率’是採用在即將到達壓縮側的上死點時, 前述磁阻通過前述拾取器期間的旋轉速度所算出。 7·如申請專利範圍第5項所記載的引擎負載檢測裝置 φ ,其中對應於前述所算出的負載率,至少對前述引擎的點 火時期進行反饋控制。 8.如申請專利範圍第6項所記載的引擎負載檢測裝置 ’其中對應於前述所算出的負載率,至少對前述引擎的點 火時期進行反饋控制。 9·—種引擎負載檢測方法,是具備:脈衝轉子,該脈 衝轉子是與引擎的曲柄軸同步旋轉;和磁阻,該磁阻被設 在該脈衝轉子’並位在對應於前述引擎之上死點附近的曲 柄角度;及拾取器’該拾取器是用來檢測該磁阻的通過; &quot;41 - 201033597 並根據該拾取器的輸出訊號,來檢測引擎之負載狀態的引 擎負載檢測方法, 其特徵爲: 具備: 將用來檢測平均引擎旋轉速度的特定區間分割成複數 個的步驟;和 用來計算前述經分割之複數個區間的各個區間引擎旋 轉速度的步驟;和 © 對前述複數個區間引擎旋轉速度執行不同加權處理的 步驟;和 藉由求出前述加權處理後之複數個區間引擎旋轉速度 的平均値,來計算前述平均引擎旋轉速度的步驟;及 使用前述平均引擎旋轉速度來執行前述引擎之負載狀 態的計算的步驟。 10.—種引擎負載檢測裝置,是具備:脈衝轉子’該 脈衝轉子是與引擎的曲柄軸同步旋轉;和磁阻’該磁阻被 ® 設在該脈衝轉子,並位在對應於前述引擎之上死點附近的 曲柄角度;及拾取器,該拾取器是用來檢測該磁阻的通過 •,並根據該拾取器的輸出訊號’來檢測引擎之負載狀態的 引擎負載檢測裝置, 其特徵爲: 將用來檢測平均引擎旋轉速度的檢測區間’設定成從 前述磁阻的通過開始點起所開始的前述曲柄軸之2次旋轉 量的長度, -42- 201033597 前述檢測區間設成由以下所形成的4個區 阻區間與第2磁阻區間,該第1磁阻區間與第 是分別對應於在前述曲柄軸之2次旋轉的每一 前述磁阻通過前述拾取器的位置;及第1區間 ,該第1區間與第2區間是分別對應於前述磁 述拾取器的位置; 並具備: 求取第1平均値的手段,該第1平均値是 區間所檢測的第1旋轉速度、與由前述第2區 第2旋轉速度的平均値;和 求取第2平均値的手段,該第2平均値爲 磁阻區間所檢測的第1磁阻旋轉速度、與由前 區間所檢測之第2磁阻旋轉速度的平均値;和 計算前述平均引擎旋轉速度的手段’該前 旋轉速度是藉由對前述第1平均値除以前述第 的値,乘以前述第2平均値所求出;及 負載狀態計算手段’該負載狀態計算手段 平均引擎旋轉速度來計算前述引擎的負載狀態 1 1.如申請專利範圍第1 〇項所記載的引擎 置,其中用來計算前述平均引擎旋轉速度的手 述第1旋轉速度以®4(n-l)表示、前述第2 ω4(η)表示、前述第1磁阻旋轉速度以 第2磁阻旋轉速度以®tdc2表示、前述加權處 數以α表示時,藉由以下的計算式來計算前述 間:第1磁 2磁阻區間 次旋轉中, 與第2區間 阻未通過前 由前述第1 間所檢測之 由前述第1 述第2磁阻 述平均引擎 1旋轉速度 是使用前述 〇 負載檢測裝 段,是當前 旋轉速度以 表示、前述 理的加權係 平均引擎旋 -43- 201033597 轉速度NeA [計算式1 ] NeA ~ α)χ ω4 + (η - ί)+ α χ ω4(η) ^ atdcl + ωίάοΐ ωΑ(η -1) 2 1 2 .如申請專利範圍第1 1項所記載的引擎負載檢測裝 置,其中被設定成:前述第1區間包含進氣行程,且前述 第2區間包含燃燒-膨脹行程, 當求取前述第1平均値之際,是將在前述第1旋轉速 度與前述第2旋轉速度之間執行不同加權處理的前述加權 係數α設定成大於0.5。 13. 如申請專利範圍第10、1 1或12項所記載的引擎 負載檢測裝置,其中前述磁阻是被配設在即將到達引擎之 上死點時的位置, 前述引擎的負載狀態,是將前述第2磁阻旋轉速度, 除以前述平均引擎轉數所算出的負載率。 14. 如申請專利範圍第13項所記載的引擎負載檢測裝 置,其中對應於前述負載率,至少對前述引擎的點火時期 執行反饋控制。 15. —種引擎負載檢測方法,是具備:脈衝轉子,該 被的過的 阻近通態 磁附的狀 該點阻載 , 死磁負 阻上該之 磁之測擎 和擎檢引 ; 弓 來if 轉述用檢 旋前是來 步於器, 同應取號 軸對拾訊 柄在該出 曲位,輸 的並器的 擎,取器 引子拾取 與轉及拾 是衝.,該 子脈度據 轉該角根 衝在柄並 脈設曲; -44 - 201033597 引 刖 之 Φ 由 阻 旋 和 應 第 磁 區 旋 的 脈 設 擎負載檢測方法, 其特徵爲: 包含: 將用來檢測平均引擎旋轉速度的檢測區間,設定成從 述磁阻的通過開始點起計算之前述曲柄軸的2次旋轉量 長度的步驟;和 將前述檢測區間設成4個區間的步驟,該4個區間是 以下所形成:第1磁阻區間與第2磁阻區間,該第1磁 區間與第2磁阻區間是分別對應於在前述曲柄軸之2次 轉的每一次旋轉中,前述磁阻通過前述拾取器的位置、 第1區間與第2區間,該第1區間與第2區間是分別對 於前述磁阻未通過前述拾取器的位置;和 求取第1平均値的步驟,該第1平均値是由前述第1 間所檢測的第1旋轉速度、與由前述第2區間所檢測之 2旋轉速度的平均値;和 求取第2平均値的步驟,該第2平均値是由前述第1 阻區間所檢測的第1磁阻旋轉速度、與由前述第2磁阻 間所檢測之第2磁阻旋轉速度的平均値;及 計算前述平均引擎旋轉速度的步驟,該前述平均引擎 轉速度是藉由對前述第1平均値除以前述第1旋轉速度 値,再乘以前述第2平均値所獲得。 16· —種引擎負載檢測裝置,是具備:脈衝轉子,該 衝轉子是與引擎的曲柄軸同步旋轉;和磁阻,該磁阻被 在該脈衝轉子,並位在對應於前述引擎之上死點附近的 -45- 201033597 曲柄角度;及拾取器,該拾取器是用來檢測該磁阻的通過 ;並根據該拾取器的輸出訊號,來檢測引擎之負載狀態的 引擎負載檢測裝置, 其特徵爲: 具備用來偵測變速機之變速比的變速比偵測手段, 前述引擎的負載狀態被設成:將前述磁阻通過前述拾 取器期間的旋轉速度,除以前述平均引擎轉數所算出的負 載率, © 前述磁阻通過前述拾取器期間的旋轉速度,是根據前 述變速比所修正。 17.如申請專利範圍第16項所記載的引擎負載檢測裝 置’其中前述變速比偵測手段,是用來檢測有段變速機之 變速檔位的齒輪位置感應器。 1 8 .如申請專利範圍第1 7項所記載的引擎負載檢測裝 置,其中前述磁阻通過前述拾取器期間之旋轉速度的修正 ,是藉由對該旋轉速度乘以修正係數的方式所執行, G 前述修正係數,是當前述有段變速機的齒輪檔數較低 時設定成較大。 1 9.如申請專利範圍第1 6項所記載的引擎負載檢測裝 置,其中前述變速比偵測手段,是根據車速與引擎轉數來 求取變速比。 -46-201033597 VII. Patent application scope: 1. An engine load detecting device is provided with: a pulse rotor which rotates synchronously with a crank shaft of an engine; and a magnetic resistance, which is set in the pulse rotor and is located at Corresponding to the crank angle near the top dead center of the engine; and the picker, the picker is used to detect the passage of the magnetic resistance; and the engine load detecting device for detecting the load state of the engine according to the output signal of the picker The method is characterized in that: 10 is: dividing a specific interval for detecting an average engine rotation speed into a plurality of pieces, and calculating an engine rotation speed of each section of the divided plurality of intervals according to an output signal of the picker Means: and weighting means, wherein the weighting means performs different weighting processing on the engine rotation speed of the plurality of sections; and load state calculation means, the load state calculation means is based on an average of the plurality of interval engine rotation speeds after the weighting process , calculating the aforementioned average G engine rotation speed and using the average engine rotation Speed to perform calculations of the load state of the engine. 2. The engine load detecting device according to claim 1, wherein the weighting process is to set a weighting ratio including a section of the combustion-expansion stroke to a plurality of sections divided into a plurality of sections. The interval is larger. 3. The engine load detecting device according to claim 1 or 2, wherein the specific section is detected based on the output of the pulse rotor - 40-201033597. 4. In the engine load detecting device described in the second or second aspect of the patent application, in the specific section, the length 2 of the second rotation amount of the crankshaft is equally divided into the first section and the second section, and is set. Into the above! The section includes an intake stroke, and the second section includes a combustion-expansion stroke. 5. The engine load detecting device of the invention of claim </ RTI> wherein the load state of the engine is calculated by dividing the rotational speed of the magnetic resistance during the passage of the pick-up device by the average engine revolution number. Load rate. 6. The engine load detecting device according to claim 5, wherein the magnetic resistance is set to be near the top dead center of the engine; the foregoing load rate is adopted at the compression side. At the top dead center, the aforementioned magnetic resistance is calculated by the rotational speed during the aforementioned pickup. 7. The engine load detecting device φ according to claim 5, wherein at least the ignition timing of the engine is feedback-controlled in accordance with the calculated load factor. 8. The engine load detecting device described in claim 6 wherein feedback control is performed on at least the ignition timing of the engine in accordance with the calculated load factor. 9. The engine load detecting method is provided with: a pulse rotor that rotates synchronously with a crankshaft of the engine; and a magnetic resistance that is set in the pulse rotor 'coordinated to correspond to the aforementioned engine The crank angle near the dead point; and the picker 'the picker is used to detect the passage of the magnetic resistance; &quot;41 - 201033597 and according to the output signal of the pickup, the engine load detection method for detecting the load state of the engine, The method is characterized by: a step of dividing a specific section for detecting an average engine rotation speed into a plurality of steps; and a step of calculating a rotation speed of each section engine of the plurality of divided sections; and © for the plurality of a step of performing a different weighting process on the interval engine rotation speed; and a step of calculating the average engine rotation speed by determining an average value of the plurality of interval engine rotation speeds after the weighting process; and performing the foregoing average engine rotation speed The step of calculating the load state of the aforementioned engine. 10. An engine load detecting device comprising: a pulse rotor 'the pulse rotor is rotated synchronously with a crankshaft of the engine; and a magnetic resistance 'the magnetic resistance is set in the pulse rotor, and is located in the engine corresponding to the aforementioned a crank angle near the top dead center; and a picker, the pick-up device is an engine load detecting device for detecting the passage of the magnetic resistance and detecting the load state of the engine according to the output signal of the pickup, characterized by : The detection interval 'for detecting the average engine rotation speed' is set to the length of the second rotation amount of the crankshaft from the start point of the magnetic resistance, and the detection interval is set to be as follows Forming four block resistance sections and a second magnetoresistive section, the first magnetoresistive section and the first corresponding to each of the magnetoresistances of the second rotation of the crankshaft passing through the pickup; and the first In the section, the first section and the second section respectively correspond to positions of the magnetic pickup; and: means for obtaining a first average ,, the first average 値 is the first detected by the section a rotation speed, an average 値 of the second rotation speed of the second zone, and a means for obtaining a second average 値, wherein the second average 値 is the first reluctance rotation speed detected by the reluctance section and the lapse interval The average 値 of the detected second reluctance rotational speed; and means for calculating the average engine rotational speed 'the front rotational speed is obtained by dividing the first average 値 by the aforementioned 値 and multiplying the second average 値And the load state calculation means 'the load state calculation means average engine rotation speed to calculate the load state of the engine 1 1. The engine set as described in the first application of the patent scope, wherein the average engine is used to calculate The first rotation speed of the rotation speed is represented by ®4 (nl), the second ω4 (η), the first reluctance rotation speed is represented by the second reluctance rotation speed by ®tdc2, and the weighting number is In the case of α, the first magnetic field is detected by the following calculation formula: the first magnetic second magnetic reluctance interval is detected by the first interval before the second interval resistance is not passed. Resisting average engine 1 The rotation speed is the use of the aforementioned load detection section, which is the current rotation speed to represent, the above-mentioned weighted system average engine rotation -43- 201033597 rotation speed NeA [calculation formula 1] NeA ~ α) χ ω4 + (η - ί The engine load detecting device according to the first aspect of the invention, wherein the first section includes the intake air, wherein the engine load detecting device according to the first aspect of the invention is set in the first aspect of the invention. In the stroke, the second section includes a combustion-expansion stroke, and when the first average enthalpy is obtained, the weighting coefficient α is set to perform a different weighting process between the first rotation speed and the second rotation speed. The ratio is greater than 0.5. 13. The engine load detecting device according to claim 10, wherein the magnetic resistance is disposed at a position immediately before the engine top dead center, and the load state of the engine is The second reluctance rotational speed is divided by the load ratio calculated by the average engine revolution number. 14. The engine load detecting device according to claim 13, wherein the feedback control is performed on at least the ignition timing of the engine corresponding to the load ratio. 15. An engine load detection method, comprising: a pulse rotor, the damped near-state magnetically attached shape, the point resistance load, the dead magnetic negative resistance on the magnetic engine and the engine inspection; To if the paraphrase is to come to the device before the inspection, the same axis should be the pair of the pickup handle in the exit position, the output of the parallelizer, the picker pick and turn and the pick is punched. According to the rotation of the corner root in the shank of the shank; -44 - 201033597 Φ 由 阻 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由 由The detection range of the engine rotation speed is set to a step of calculating the length of the second rotation amount of the crankshaft from the start point of the reluctance, and the step of setting the detection section to four sections, wherein the four sections are The first magnetic resistance section and the second magnetic resistance section are formed in each of the first magnetic section and the second magnetic resistance section in each of two rotations of the crankshaft, and the magnetic resistance passes through the foregoing Picker position, first interval and second interval, The first interval and the second interval are steps for respectively preventing the magnetic resistance from passing through the pickup; and obtaining a first average 値, wherein the first average 値 is the first rotational speed detected by the first interval, And an average 2 of the two rotational speeds detected by the second interval; and a step of obtaining the second average 値, the second average 値 is the first reluctance rotational speed detected by the first resisting interval, and An average 値 of the second reluctance rotational speed detected between the second reluctances; and a step of calculating the average engine rotational speed, wherein the average engine rotational speed is divided by the first rotation by the first rotation The speed is 値, and multiplied by the aforementioned second average 値. 16) an engine load detecting device comprising: a pulse rotor that rotates synchronously with a crankshaft of the engine; and a magnetoresistance that is placed in the pulse rotor and is positioned above the engine Near the point -45- 201033597 crank angle; and picker, the picker is used to detect the passage of the reluctance; and according to the output signal of the pickup, the engine load detecting device for detecting the load state of the engine, its characteristics a speed ratio detecting means for detecting a speed ratio of the transmission, wherein the load state of the engine is set to be obtained by dividing the rotational speed of the magnetic resistance during the pick-up by the average engine revolution The load factor, © the rotational speed of the aforementioned magnetic resistance during the passage of the aforementioned pickup, is corrected according to the aforementioned gear ratio. 17. The engine load detecting device according to claim 16, wherein the gear ratio detecting means is a gear position sensor for detecting a shift position of the stepped shifter. The engine load detecting device according to claim 17, wherein the correction of the rotational speed of the magnetic resistance during the passage of the pick-up is performed by multiplying the rotational speed by a correction coefficient. G The aforementioned correction coefficient is set to be large when the number of gears of the above-described partial transmission is low. The engine load detecting device according to claim 16, wherein the gear ratio detecting means obtains the gear ratio based on the vehicle speed and the number of engine revolutions. -46-
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TWI498536B (en) * 2013-01-09 2015-09-01 Univ Nat Taipei Technology Method and device for diagnosing misfire in single-cylinder engine

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5292262B2 (en) * 2009-11-24 2013-09-18 株式会社ケーヒン Engine acceleration / deceleration state discrimination device
JP5328757B2 (en) * 2010-12-17 2013-10-30 本田技研工業株式会社 Engine control device
JP5750019B2 (en) * 2011-09-29 2015-07-15 本田技研工業株式会社 Motorcycle
CN104568445A (en) * 2013-10-18 2015-04-29 镇江中研电控有限公司 Engine load detection device and engine load detection method
JP5995894B2 (en) * 2014-03-18 2016-09-21 本田技研工業株式会社 Ignition control device for vehicle engine
CN113933012B (en) * 2021-10-14 2024-01-30 西安现代控制技术研究所 Propeller rotating speed measuring method based on K-means clustering

Family Cites Families (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4398259A (en) * 1980-08-01 1983-08-09 Harris Corporation Snap acceleration method of diagnosing faults in internal combustion engines
JP2893233B2 (en) * 1993-12-09 1999-05-17 株式会社ユニシアジェックス Diagnostic device for in-cylinder pressure sensor
JPH0932613A (en) * 1995-07-20 1997-02-04 Mitsubishi Motors Corp Idle speed controller for vehicule engine
JP3758236B2 (en) * 1995-10-09 2006-03-22 株式会社デンソー Misfire detection device for internal combustion engine
JPH10148153A (en) * 1996-11-20 1998-06-02 Fuji Heavy Ind Ltd Misfire diagnostic device for engine
CN2404113Y (en) * 2000-01-13 2000-11-01 重庆滇渝高科技机电研究所 Motorcycle engine performance detection microcomputer apparatus
EP1197656B1 (en) * 2000-10-12 2008-02-20 Kabushiki Kaisha Moric Engine control method and apparatus
TW539806B (en) * 2001-08-10 2003-07-01 Moric Kabushiki Kaisha Engine control method and device for a vehicle
JP2003056438A (en) * 2001-08-10 2003-02-26 Moric Co Ltd Vehicular engine control method and system
JP3768927B2 (en) * 2002-07-10 2006-04-19 三菱電機株式会社 Cylinder discrimination device for internal combustion engine
JP4040530B2 (en) * 2003-05-26 2008-01-30 本田技研工業株式会社 Ignition timing control device for internal combustion engine
JP4380701B2 (en) * 2004-03-08 2009-12-09 トヨタ自動車株式会社 Control device for internal combustion engine with electric supercharger

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI498536B (en) * 2013-01-09 2015-09-01 Univ Nat Taipei Technology Method and device for diagnosing misfire in single-cylinder engine

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