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TW201239190A - Engine and the vehicles/ships equipped thereof - Google Patents

Engine and the vehicles/ships equipped thereof Download PDF

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Publication number
TW201239190A
TW201239190A TW100110853A TW100110853A TW201239190A TW 201239190 A TW201239190 A TW 201239190A TW 100110853 A TW100110853 A TW 100110853A TW 100110853 A TW100110853 A TW 100110853A TW 201239190 A TW201239190 A TW 201239190A
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Taiwan
Prior art keywords
passage
exhaust
engine
downstream
air
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TW100110853A
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Chinese (zh)
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TWI444534B (en
Inventor
Tsugunori Konakawa
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Yamaha Motor Co Ltd
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Priority to TW100110853A priority Critical patent/TWI444534B/en
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Publication of TWI444534B publication Critical patent/TWI444534B/en

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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
    • Y02ATECHNOLOGIES FOR ADAPTATION TO CLIMATE CHANGE
    • Y02A50/00TECHNOLOGIES FOR ADAPTATION TO CLIMATE CHANGE in human health protection, e.g. against extreme weather
    • Y02A50/20Air quality improvement or preservation, e.g. vehicle emission control or emission reduction by using catalytic converters

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  • Exhaust Gas After Treatment (AREA)

Abstract

An engine includes: an air exhaust device having an air exhaust outlet for introducing exhaust gas from a combustion chamber; an air supply device for supplying air. The air exhaust outlet is disposed with a convergent portion, a divergent portion and a branch portion. The branch portion allows the impact wave propagated in the downstream direction from more upstream than the said divergent portion to branch off from said air exhaust channel for making said impact wave to propagate to said air exhaust channel again. The air supply device includes: a first channel, having a first reed valve to allow air flow to pass from the direction of upstream to downstream, and the downstream end connected to said air exhaust outlet is more upstream compared to said divergent portion; a second channel, having the upstream end connected to said first outlet is more upstream compared to said first reed valve. Said air exhaust device allowing the exhaust gas to pass through said convergent portion is constituted by an impact method of the impact wave that propagated in said branch portion between said branch portion and said divergent portion.

Description

201239190 六、發明說明: 【發明所屬之技術領域】 本發明係關於引擎(内燃機)以及具備其之車輛與船舶。 【先前技術】 眾所周知的是包括對廢氣進行淨化之觸媒及對排氣通道 供給空氣之二次空氣供給裝置(Sec〇ndary Air Supply System)之引擎(lnternai c〇mbusti〇n ,内燃機)。例 如,專利文獻1之引擎中’於排氣通道設置有三元觸媒。 二次空氣供給裝置以分別對觸媒之上游與下游供給二次空 氣之方式連接於排氣通道。二次空氣係指不通過引擎之燃 燒室而供給之空氣。觸媒主要作為對Ν〇χ進行還原之還原 觸媒發揮功能’但亦作為氧化觸媒發揮功能。#,供給至 較觸媒更為下游之二:欠^氣藉由排氣之脈動而暫時流入至 觸媒之後向下游流動。此時,觸媒亦作為使c〇、thc氧化 之氧化觸媒發揮功能,對自引擎排出之廢氣中之ΝΟχ、 CO、THC進行淨化。 專利文⑴之引擎之二次空氣供給農置以亦向較觸媒更 為上游供給二次空氣之方式構成。其原因在於,當於高速 向負載運行時等將對引擎之供給空燃比設定得較高時,廢 氣:所含之C〇、THC量增多。此時,藉由向觸媒之上游供 -人工孔’可使觸媒主要作為使c〇、而氧化之 媒發揮功能。 乳化順 專利文獻1中,作為向較觸媒更為下游供給二次空氣之 方法而揭示有兩種方法。其一方法係裝備有簧片閱並利用 154997.doc 201239190 排氣通道内之排氣脈動之方法。另一方法係設置空氣泵代 替簧片閥而強制性地將二次空氣供給至排氣通道之方法。 [先前技術文獻] [專利文獻] [專利文獻1]曰本專利特開2006-220019號公報 【發明内容】 [發明所欲解決之問題] 比較向較觸媒更為下游供給二次空氣之上述兩種方法。 利用排氣脈動之方法不同於利用空氣泵之方法,無需驅 動泵,因此引擎輸出之損失較少。然而,該方法存在以下 問題。當引擎於高轉速或高負載狀態下運行時,排氣通道 内之平均塵力變高。又,於排氣通道之較觸媒更為下游之 部分,因觸媒之阻力而導致排氣脈動之振幅較小。引擎越 成為两轉速或高負載狀態,則因該觸媒而產生之阻力之大 小就越大。即,尤其當引擎於高轉速或高負載狀態下運行 時,排氣通道内之平均壓力冑冑,且排氣脈動之振幅變 小。由此,無法於較觸媒更為下游之排氣通道内產生較大 之負壓。由此,尤其當引擎於高轉速或高負載狀態下運行 時,無法向較觸媒更為下游之排氣通道内供給足量之二次 空氣。 、另方面’利用空氣系之方法中,即便於引擎以高轉速 或高負載狀態運行時亦可供給二次空氣。但引擎越成為高 轉速或高負載狀態則空氣栗之負載就越大。由於以引擎驅 動。玄二氣泵’故而引擎越成為高轉速或高負載狀態,引擎 154997.doc 201239190 輸出之損失會越大。 本案發明者發現於排氣Π打開時在排氣通道中朝向下游 專播之衝擊波n考慮若利用於衝擊波之後方產生負 壓則即便於高負載狀態下亦可供給空氣。然而,該衝擊波 係於排氣口附近產生’且隨著向下游傳播而衰減、消失。 因此,無法用於在較觸媒更為下游產生負壓。 由此,本案發明者考慮於排氣通道内產生其他新的衝擊 波以產生新的負壓。將通常為人所周知之漸縮-漸擴喷嘴 (c〇nvergent_Divergent N〇zzle)即通稱為德拉瓦嘴嘴取 Law N〇zzle)之原理應用於包括二次空氣供給裝置之引 擎。該喷嘴包括:漸縮部,其隨著朝向流路之下游側而流 路剖面積變小;漸擴部,其於該漸縮部之下游流路剖面積 變大;及喉部,其位於該漸縮部與漸擴部之間。當漸縮部 之壓力P0與漸擴部之壓力?之壓力比(p/p〇)小於臨界壓力比 (Ο—1 Rati〇。若為空氣則為約0.528)時,於漸 擴部流體之流速超過音速β 由此’產线的衝擊波,故職料設置下游端之 流路剖面積小於上游端之流路剖面積之漸縮部,進而於較 該漸縮部更為下游之排氣通道設置下游端之流路剖面積大 於上游端之流路刮面積之漸擴部。然而,若僅於排氣通道 設置漸縮部與漸擴部’則漸縮部之屋力抑與漸擴部之塵力 Ρ之麼力比(⑽)無法達到臨㈣力比,從而無法產生新的 衝擊波。 本案發明者對引擎進一步積極地進行研究之結果發現·· 154997.doc 201239190 於排氣口打開時在排氣通道中朝向下游傳播之衝擊波,此 時以較自燃燒室流入至排氣通道之廢氣更高之速度傳播。 進而,發明者關注於該衝擊波速度與廢氣速度之差異而考 慮提高漸縮部之壓力P0之構造。該構造包括使先行之衝擊 波自排氣通道暫時分支後再次返回至排氣通道之分支部。 藉由提高漸縮部之壓力P0而於漸擴部產生新的衝擊波。如 此一來,會於該衝擊波之後方,即於較漸擴部更為上游產 生負壓。 進而,本案發明者考慮,利用於較漸擴部更為上游產生 之上述負壓而供給空氣之構造。該構造包括連接於排氣通 道之較漸擴部更為上游之第丨通道,及連接於第丨通道之第 2通道。 本發明之一實施形態提供一種使用該些構造之引擎。 即:本發明之一實施形態之引擎包括:燃燒室,其形成有 排氣口;排氣閥,其開閉上述排氣口;排氣裝i,其具有 導引自上述燃燒室通過上述排氣口排出之廢氣之排氣通 道;及空氣供給裝置,其供給空氣。上述排氣裝置包括. 漸縮部’其設置於上述排氣通道,且下游端之流路剖面積 小於上游端之流路剖面積;漸擴部,其於上 設置於較上述漸縮部更為下游,且下游端之流路 於上游端之流路剖面積;及分支部,其將以較上 打開時自上述燃燒室流人至上述排氣通道之廢氣更高= 度在上述排氣通道中朝向下游傳播之衝擊波於較 部更為上游自上述排氣通道分支,且將該衝擊㈣ 154997.doc 201239190 述排氣通道傳播。上述空氣供給裝置包括: 具有使自上游端朝向下游端之氣流通過之第i箸片 於上述排氣通道之較上述漸擴部更為上游,·及 I 游端連接於上述第1通道之較上述第!簧片 閥更為下游。進而,上述排氣裝置以如下方式構成:使自 上述燃燒室流人至上述排氣通道之廢氣通過上述漸縮部, 且於上述分支部與上述漸擴部之間與在上述分支部中傳播 之衝擊波衝撞,藉此於上述漸縮部提高廢氣之壓力,並藉 由使該壓力經提高之廢氣通過上述漸擴部而產生新的㈣ 波。又,上述空氣供給裝置以如下方式構成:利用藉由上 述新產生之衝擊波而於較上述漸擴部更為上游之上述排氣 通道内產生之負® ’通過上述第1片閥而將空氣導入上 述第1通道,並利用於較上述漸擴部更為上游之上述排氣 通道内產生之正壓而向上述第2通道供給上述導入之办 氣。 工 根據該構成,較廢“先行之衝擊波於分支部暫時分支 後再次返回至排氣通道。由此,可以分支部使衝擊波在時 間上延遲’從而可使該衝擊波於排氣通道内與廢氣衝撞, 由此可提高廢氣之壓力。該廢氣藉由通過漸縮部而使壓力 進-步提高,Θ而漸縮部之壓力抑與漸擴部之壓之壓 力比(Ρ/Ρ0)易於達到臨界壓力比。即,於高壓之廢氣通過 漸擴部時產生新的衝擊波(與排氣口打開時產生之衝擊波 不同之衝擊波)。於該新的衝擊波之上游,即於漸擴部之 上游產生較大之負Μ。可利用該較大之負壓而自第i通道 154997.doc 201239190 二次空係指不 之上游氣端將二次空氣導入至第1通道内 通過燃燒室之引擎外部之空氣。 ,於較漸擴部更為上游之排氣通道内,藉由排 氣脈動而交替產生正壓與諸。該排氣脈動之振幅因曰於較 漸擴更為上游產生之較大之負壓之影響而變大。於產生 負壓時導人至第1通道内之二次空氣,於產生正塵時被自 第1通道擠出並供給至第2通道内。 上述第2通道之下游端亦可連接於排氣通道。即,自第i 通道擠出之二次空氣亦可經由第2通道供給至排氣通道。 該構成於排氣通道中在較上述漸擴部更為下游配置有觸媒 之情形時尤其有利。即’利用藉由新的衝擊波而產生之較 大之負壓與藉由排氣脈動而產生之正壓,即便於高轉速或 高負載狀態下,亦可向較觸媒更為下游之排氣通道内供給 二次空氣。此時產生之正壓及負壓利用廢氣之能量,因而 可降低引擎輸出之損失。 本發明中之上述之、或進而其他目的、特徵及效果可藉 由以下參照附圖所述之實施形態之說明而變得明瞭。 【實施方式】 本案發明者進行積極研究之結果想到:可利用漸縮-漸 擴喷嘴之原理而如以下般利用先前未採用之方法供給足量 之二次空氣。 該方法係如下所述。(1)使較廢氣而先行傳播之衝擊波 分支。(2)使分支之衝擊波於時間上延遲而與廢氣衝撞來提 商該廢氣之壓力。(3)使壓力提高之廢氣通過漸擴部加速至 154997.doc -10· 201239190 超音速而產线的衝擊^⑷於較漸擴部更為上游之排氣 通道内產生負壓。(5)利用該負壓,向連接於較_部更為 上游之二次空氣供給裝置之第1通道内導入二次空氣。(6) 利用於較漸擴部更為上游之排氣通道内產生之正壓向二次 空氣供給裝置之第2通道供給二次空氣。 &lt;第1實施形態&gt; 以下’使帛(V寸圖對本發明之實施形態進行詳細說明。再 者以下說明t,「上游」、「下游」分別係指與廢氣或二 次空氣之流動方向相關之上游、下游。 圖1係表示本發明之第1實施形態之引擎之構成之剖面 圖。引擎1包括:氣虹體3 ;言免置於該氣紅體3之一端之氣 虹蓋4;及於氣細體3内往返運動之活塞5。於氣紅體3及氣 缸蓋4之内部形成有燃燒室10。更詳細而言,藉由氣缸體3 之内壁、氣缸蓋4之内壁及活塞5之表面(與氣虹蓋4對向之 表面)而劃分燃燒室1Ge活塞5經由連桿15而結合於曲柄轴 16。曲柄軸16收納於與氣缸體3結合之曲柄箱17内。活塞5 之往返運動藉由連桿15而傳遞至曲柄軸16,藉此曲柄軸Μ 鉍轉。引擎1為4循環汽油内燃機。引擎i為單氣缸引擎。 引擎1可為空冷式引擎,亦可為水冷式引擎。 於氣缸蓋4形成有進氣通道6之下游部以及排氣通道了之 上游# 7a於氣缸蓋4⑦置有:對進氣口 8a進行開閉之進 氣閥8;對排氣口 9a進行開閉之排氣閥9 ;以及用以驅動進 氣閥8及排氣闊9之氣門裝置(未圖示)。本實施形態中,進 氣通道6之下游部6a與排氣通道7之上游㈣相對於一個燃 154997.doc 201239190 燒室ίο而分別各設置有一個。然而, 運氣口 8a、進氣閥 8、排氣口 9a及/或排氣閥9亦可相對 &gt;, 個燃燒室而設置 有複數個。於氣缸蓋4安裝有喷射燃料 貰射态2。省略圖 示’於氣缸蓋4設置有點火火花塞。 於進氣通道6之較下游部6a更為h .、佐 ,μ 更為上游配置有節氣門閥 U。該郎氣門,i亦可機械性地結合於由操作者操作之操 作構件(例如經由拉索而結合)…亦可不為該機械性之 結合,而為藉由馬達電子控制節氣門閥丨i。 引擎1進而包括排氣裝置50。排氣裝置5〇包括:連接於 ,缸羞4之第i排氣管51 ;連接於該第i排氣管η之第2排氣 =52 :及連接於該第2排氣管52之第3排氣管μ。第工排氣 管51藉由螺栓12而安裝於氣缸蓋4。第3排氣管辦立内部 形成排氣室55。排氣裝置50於其内部形成自上游部、經由 排氣室55而連接於外部之排氣通道7。 於排氣通道7配置有第!觸媒21及第2觸媒22。第2觸媒Μ 配置於P觸媒21之下游。於第i觸媒21與第㈣肋之間 設置有間隔。 未圖示之消音器(muffler)連接於排氣室55之下游。流入 至排氣室55内部之廢氣通過上述消音^後排出至外部。於 排氣室55設置有檢測廢氣中之氧量之氧濃度感測器… 引擎1包括作為控制裝置之ECU(Eiectr〇nicaIly Controlled Unit,電子控制單元)2〇。ECU2〇根據引擎i之 轉速、上述節氣門閥Η之開度、或由氧濃度感測器19檢測 出之信號而控制噴射器2之燃料噴射量、或上述點火火花 I54997.doc 201239190 塞之點火時間等。ECU20以使例如吸入至引擎1之混合氣 之二燃比成為理論空燃比(stoiciometry)之方式控制噴射号 2之燃料噴射量。 於第1排氣官51之上游部設置有分支管30。分支管3〇之 一端為連接於第1排氣管51之開放端,另一端為封閉之封 閉端。封閉端形成反射後述之衝擊波之反射部31b。 分支管30亦可一體成形於第i排氣管51。又,分支管 亦可與第1排氣管51分開形成且固定於第丨排氣管51。例 如,第1排氣管51與分支管30可焊接於一起,亦可藉由螺 才王、鉚釘等緊固構件(未圖示)而固定於一起。分支管儿之 上述封閉端以使流路剖面積大於上述開放端之方式形成。 ,分支管30之形狀並不限定於圖i所示之形狀。即,分支 :3〇之封閉端之流路剖面積可與其開放端之流路剖面積相 等’亦可小於開放端之流路剖面積。 於分支管30内部形成有分支部31。分支部31之201239190 VI. Description of the Invention: TECHNICAL FIELD OF THE INVENTION The present invention relates to an engine (internal combustion engine) and a vehicle and a ship therewith. [Prior Art] It is known to include a catalyst for purifying exhaust gas and an engine for supplying a secondary air supply device (Sec〇ndary Air Supply System) to the exhaust passage (lnternai c〇mbusti〇n, internal combustion engine). For example, in the engine of Patent Document 1, a three-way catalyst is disposed in the exhaust passage. The secondary air supply means is connected to the exhaust passage so as to supply secondary air to the upstream and downstream of the catalyst, respectively. Secondary air refers to air that is not supplied through the combustion chamber of the engine. The catalyst mainly functions as a reduction catalyst for reducing ruthenium, but it also functions as an oxidation catalyst. #, Supply to the downstream of the catalyst: the gas is temporarily flowing into the catalyst and then flows downstream by the pulsation of the exhaust gas. At this time, the catalyst also functions as an oxidation catalyst for oxidizing c〇 and thc, and purifies the ruthenium, CO, and THC in the exhaust gas discharged from the engine. The secondary air supply to the engine of the patent (1) is also configured to supply secondary air to the upstream of the catalyst. The reason for this is that when the air-fuel ratio to the engine is set to be high when the vehicle is operated at a high speed, the amount of C〇 and THC contained in the exhaust gas is increased. At this time, the catalyst can be mainly used as a medium for causing c〇 to be oxidized by supplying an artificial hole to the upstream of the catalyst. Emulsification In Patent Document 1, two methods are disclosed as a method of supplying secondary air to the downstream of the catalyst. One method is equipped with a reed and uses the pulsation of the exhaust in the exhaust passage of 154997.doc 201239190. Another method is to provide an air pump instead of a reed valve to forcibly supply secondary air to the exhaust passage. [Prior Art] [Patent Document 1] [Patent Document 1] JP-A-2006-220019 SUMMARY OF THE INVENTION [Problems to be Solved by the Invention] The above is to supply the secondary air to the downstream of the catalyst. Two methods. The method of using the exhaust pulsation is different from the method of using the air pump, and there is no need to drive the pump, so the engine output loss is small. However, this method has the following problems. When the engine is operated at high speed or high load, the average dust force in the exhaust passage becomes high. Further, in the portion of the exhaust passage which is further downstream than the catalyst, the amplitude of the exhaust pulsation is small due to the resistance of the catalyst. The more the engine becomes a two-speed or high-load state, the greater the resistance generated by the catalyst. That is, especially when the engine is operated at a high rotation speed or a high load state, the average pressure in the exhaust passage is 胄胄, and the amplitude of the exhaust pulsation becomes small. As a result, a large negative pressure cannot be generated in the exhaust passage downstream of the catalyst. Thus, especially when the engine is operated at a high speed or a high load state, it is not possible to supply a sufficient amount of secondary air to the exhaust passage which is more downstream of the catalyst. In another aspect, the method of using the air system can supply secondary air even when the engine is operated at a high rotational speed or a high load state. However, the higher the engine is at high speed or high load, the greater the load on the air pump. Because it is driven by the engine. Xuan Erqi Pump's, the engine becomes higher speed or high load, the greater the loss of engine output 154997.doc 201239190. The inventors of the present invention have found that the shock wave n which is propagated downstream in the exhaust passage when the exhaust port is opened is considered to be capable of supplying air even under a high load state if a negative pressure is generated after the shock wave is applied. However, the shock wave is generated near the exhaust port and attenuates and disappears as it propagates downstream. Therefore, it cannot be used to generate a negative pressure downstream of the catalyst. Thus, the inventors of the present invention considered generating other new shock waves in the exhaust passage to generate a new negative pressure. The principle of a commonly known gradual-divergent nozzle (c〇nvergent_Divergent N〇zzle), commonly known as Lawr's mouth, is applied to an engine including a secondary air supply device. The nozzle includes a tapered portion that has a smaller cross-sectional area of the flow path toward the downstream side of the flow path, a diverging portion that has a larger cross-sectional area of the flow path downstream of the tapered portion, and a throat portion that is located Between the tapered portion and the diverging portion. When the pressure of the tapered portion P0 and the pressure of the diverging portion? The pressure ratio (p/p〇) is less than the critical pressure ratio (Ο-1 Rati〇. If it is about 0.528 for air), the flow velocity of the fluid in the diverging portion exceeds the speed of sound β, thus the shock wave of the production line. The cross-sectional area of the flow path at the downstream end is smaller than the tapered portion of the cross-sectional area of the flow path at the upstream end, and the flow path of the downstream end of the exhaust passage disposed downstream of the tapered portion is larger than the flow path of the upstream end. Scaling area of the scraping area. However, if the tapered portion and the divergent portion are provided only in the exhaust passage, the ratio of the force of the tapered portion to the dust force of the diverging portion ((10)) cannot reach the ratio of force (4), and thus cannot be produced. New shock wave. As a result of further research on the engine by the inventor of the present invention, it was found that 154997.doc 201239190 shock wave propagating downstream in the exhaust passage when the exhaust port is opened, at this time, exhaust gas flowing from the combustion chamber to the exhaust passage Higher speed spread. Further, the inventors paid attention to the difference between the shock wave velocity and the exhaust gas velocity, and considered the structure for increasing the pressure P0 of the tapered portion. This configuration includes causing the preceding shock wave to temporarily branch from the exhaust passage and return to the branch portion of the exhaust passage again. A new shock wave is generated in the diverging portion by increasing the pressure P0 of the tapered portion. As a result, a negative pressure is generated downstream of the shock wave, i.e., further upstream of the flared portion. Further, the inventors of the present invention have considered a structure in which air is supplied to the negative pressure generated upstream from the gradually expanding portion. The configuration includes a second channel connected further upstream of the diverging portion of the exhaust passage and a second passage connected to the second channel. An embodiment of the present invention provides an engine using the configurations. That is, the engine according to an embodiment of the present invention includes: a combustion chamber formed with an exhaust port; an exhaust valve that opens and closes the exhaust port; and an exhaust device i that is guided from the combustion chamber through the exhaust An exhaust passage of the exhaust gas discharged from the port; and an air supply device that supplies air. The venting device includes: a tapered portion disposed in the exhaust passage, and a cross-sectional area of the flow path at the downstream end is smaller than a cross-sectional area of the flow path at the upstream end; and a diverging portion that is disposed above the tapered portion Is the downstream, and the downstream end of the flow path at the upstream end of the flow path sectional area; and the branch portion, which will be higher than the exhaust gas flowing from the combustion chamber to the exhaust passage when the upper opening is opened = degree in the above exhaust The shock wave propagating downstream in the channel branches from the exhaust channel further upstream and propagates the impact (4) 154997.doc 201239190. The air supply device includes: an imaginary piece having a flow of air passing from the upstream end toward the downstream end upstream of the diverging portion of the exhaust passage, and a connection of the I swim end to the first passage Above! The reed valve is further downstream. Further, the exhaust device is configured such that exhaust gas flowing from the combustion chamber to the exhaust passage passes through the tapered portion, and propagates between the branch portion and the diverging portion and in the branch portion The shock wave collides, thereby increasing the pressure of the exhaust gas at the tapered portion, and generating a new (four) wave by passing the increased exhaust gas through the diverging portion. Further, the air supply device is configured to introduce air into the exhaust passage that is generated in the exhaust passage upstream of the diverging portion by the newly generated shock wave. The first passage is configured to supply the introduced air to the second passage by a positive pressure generated in the exhaust passage upstream of the diverging portion. According to this configuration, the "previous shock wave is temporarily branched in the branch portion and then returned to the exhaust passage again. Thereby, the branch portion can delay the shock wave in time", so that the shock wave can collide with the exhaust gas in the exhaust passage. Therefore, the pressure of the exhaust gas can be increased. The exhaust gas is further increased in pressure by passing through the tapered portion, and the pressure ratio of the pressure of the tapered portion and the pressure of the gradually expanding portion (Ρ/Ρ0) is easily reached. The pressure ratio, that is, when the high-pressure exhaust gas passes through the diverging portion, a new shock wave (a shock wave different from the shock wave generated when the exhaust port is opened) is generated. The upstream of the new shock wave, that is, upstream of the diverging portion The larger negative pressure can be used to introduce secondary air from the upstream air end of the i-channel 154997.doc 201239190 secondary air system to the air outside the engine in the first passage through the combustion chamber. In the exhaust passage which is more upstream than the gradually expanding portion, the positive pressure is alternately generated by the exhaust pulsation. The amplitude of the exhaust pulsation is larger due to the larger and more upstream. Become bigger by the influence of pressure The secondary air that is introduced into the first passage when the negative pressure is generated is extruded from the first passage and supplied to the second passage when the positive dust is generated. The downstream end of the second passage may also be connected to the row. The air passage, that is, the secondary air extruded from the i-th passage may be supplied to the exhaust passage via the second passage. The configuration is such that when the catalyst is disposed downstream of the diverging portion in the exhaust passage It is especially advantageous to use a large negative pressure generated by a new shock wave and a positive pressure generated by the pulsation of the exhaust gas, and even at a high rotational speed or a high load state, it can be further downstream to the catalyst. The secondary air is supplied into the exhaust passage. The positive pressure and the negative pressure generated at this time utilize the energy of the exhaust gas, thereby reducing the loss of engine output. The above, or other objects, features and effects of the present invention may be utilized by The following description of the embodiments of the present invention will be apparent. [Embodiment] As a result of active research, the inventors of the present invention have conceived that the principle of a tapered-smoothing nozzle can be utilized to utilize a previously unused method as follows. Supply sufficient The secondary air. The method is as follows: (1) Branching the shock wave that propagates earlier than the exhaust gas. (2) Delaying the shock wave of the branch to collide with the exhaust gas to increase the pressure of the exhaust gas. The exhaust gas with increased pressure is accelerated to the 154997.doc -10· 201239190 supersonic speed and the impact of the production line ^(4) generates a negative pressure in the exhaust passage which is more upstream than the diverging portion. (5) Negative pressure, introducing secondary air into the first passage of the secondary air supply device connected to the upstream portion of the _ portion. (6) utilizing the positive pressure generated in the exhaust passage further upstream than the gradually expanding portion The second air is supplied to the second passage of the secondary air supply device. <First Embodiment> The following describes the embodiment of the present invention in detail. The following description will be given of t, "upstream" and " “Downstream” refers to the upstream and downstream of the flow direction of the exhaust gas or secondary air, respectively. Fig. 1 is a cross-sectional view showing the configuration of an engine according to a first embodiment of the present invention. The engine 1 includes: a gas rainbow body 3; a gas cap 4 which is placed at one end of the gas red body 3; and a piston 5 which reciprocates in the gas body 3. A combustion chamber 10 is formed inside the gas red body 3 and the cylinder head 4. More specifically, the combustion chamber 1Ge piston 5 is coupled to the crankshaft via the connecting rod 15 by the inner wall of the cylinder block 3, the inner wall of the cylinder head 4, and the surface of the piston 5 (the surface opposite to the gas siphon cover 4). 16. The crankshaft 16 is housed in a crank case 17 that is coupled to the cylinder block 3. The reciprocating motion of the piston 5 is transmitted to the crankshaft 16 by the link 15, whereby the crankshaft 铋 is turned. The engine 1 is a 4-cycle gasoline internal combustion engine. Engine i is a single cylinder engine. Engine 1 can be an air-cooled engine or a water-cooled engine. The cylinder head 4 is formed with a downstream portion of the intake passage 6 and an upstream side of the exhaust passage #7a. The cylinder head 47 is provided with an intake valve 8 that opens and closes the intake port 8a, and opens and closes the exhaust port 9a. An exhaust valve 9; and a valve device (not shown) for driving the intake valve 8 and the exhaust manifold 9. In the present embodiment, one downstream of the downstream portion 6a of the intake passage 6 and the upstream (four) of the exhaust passage 7 is provided for each of the illuminating passages 154997.doc 201239190. However, the air port 8a, the intake valve 8, the exhaust port 9a, and/or the exhaust valve 9 may be provided in plural numbers with respect to each of the combustion chambers. An injection fuel 贳 态 2 is mounted on the cylinder head 4. The illustration is omitted. The ignition head is provided on the cylinder head 4. The throttle valve U is disposed further upstream of the downstream portion 6a of the intake passage 6 than the lower portion. The lang valve, i, may also be mechanically coupled to an operating member operated by an operator (e.g., coupled via a cable) ... or may not be a mechanical combination, but the throttle valve 丨i is electronically controlled by a motor. The engine 1 in turn includes an exhaust device 50. The exhaust device 5 includes: an i-th exhaust pipe 51 connected to the cylinder shark 4; a second exhaust gas 52 connected to the i-th exhaust pipe η: and a second exhaust pipe 52 connected thereto 3 exhaust pipe μ. The first exhaust pipe 51 is attached to the cylinder head 4 by bolts 12. The third exhaust pipe is installed inside to form an exhaust chamber 55. The exhaust device 50 has an exhaust passage 7 connected to the outside from the upstream portion via the exhaust chamber 55. The exhaust channel 7 is configured with the first! Catalyst 21 and second catalyst 22. The second catalyst Μ is disposed downstream of the P catalyst 21. A space is provided between the i-th catalyst 21 and the fourth (fourth) rib. A muffler (not shown) is connected downstream of the discharge chamber 55. The exhaust gas that has flowed into the inside of the exhaust chamber 55 is discharged to the outside through the above-described muffler. An oxygen concentration sensor for detecting the amount of oxygen in the exhaust gas is provided in the exhaust chamber 55. The engine 1 includes an ECU (Eiectr〇nicaIly Controlled Unit) 2 as a control device. The ECU 2 controls the fuel injection amount of the injector 2 or the ignition timing of the ignition spark I54997.doc 201239190 according to the rotation speed of the engine i, the opening degree of the throttle valve 、, or the signal detected by the oxygen concentration sensor 19. Wait. The ECU 20 controls the fuel injection amount of the injection number 2 such that the second combustion ratio of the mixture gas sucked into the engine 1 becomes a stoichiometric. A branch pipe 30 is provided at an upstream portion of the first exhausting officer 51. One end of the branch pipe 3 is connected to the open end of the first exhaust pipe 51, and the other end is a closed closed end. The closed end forms a reflection portion 31b that reflects a shock wave to be described later. The branch pipe 30 may also be integrally formed in the i-th exhaust pipe 51. Further, the branch pipe may be formed separately from the first exhaust pipe 51 and fixed to the second exhaust pipe 51. For example, the first exhaust pipe 51 and the branch pipe 30 may be welded together, or may be fixed together by a fastening member (not shown) such as a screw or a rivet. The closed end of the branch pipe is formed in such a manner that the flow path sectional area is larger than the open end. The shape of the branch pipe 30 is not limited to the shape shown in FIG. That is, the cross-sectional area of the flow path at the closed end of the branch may be equal to the cross-sectional area of the flow path at the open end thereof or smaller than the cross-sectional area of the flow path at the open end. A branch portion 31 is formed inside the branch pipe 30. Branch portion 31

接於排氣通道7之開放端,另-端為封閉端。分支部L 入口 31a(即,與排氣通道7連通之部分),如後述般以且有 :使t排氣通道7内部傳播之衝擊波亦於分支部31内部傳 播之〜路剖面積之方式形成。圖 化之流路剖面之中心線]心線二為…31之入口 心之線。 糸才曰通過流路剖面之重 ㈣:m與第1觸媒2】之間設置有漸縮_漸擴喷嘴4 〇。 漸縮-漸擴噴嘴4〇通稱為德拉瓦噴嘴。 流過排氣通—自次音速成 154997.doc -13- 201239190 式進行加速。漸縮·漸擴喷 擴部彻成。漸縮部41係隨著朝^縮°M1、喉部42及漸 . 現者朝向下游而流路丸丨而接&amp; 減少之部分。漸擴部43係隨著 广面積逐漸 辦女“ V 朝向下游而流路剖面積逐漸 增大之部分。喉部42係配置 狀新 部分,且係流路剖面積最小之:::M1與漸擴部43之間之 二T排氣裝置50之排氣通道7供給空氣之二 -人工虱供給裝置70。二次空&amp; # π # L 人二轧供給裝置7〇包括:簧片閥 74(止回閥):第上二次空氣供认 貢乃阀 々μ狀 轧供給管76;及連接於第1二次空 軋供給管76之第2二次空氣供給管77。 簧片閥74結合於第匕次空氣供給管%之上游端。第匕 次空氣供給管76之下游端連接於第工排氣管Η中之分支管 3〇與漸縮·漸擴喷嘴40之間。第1二次空氣供給管%經由簧 片閥74與空氣量控制閥75而連接於空氣遽清器78。簧片閥 74防止廢氣自第!二次空氣供給管%向其上游流入。簧片 閥74以藉由於排氣通道7產生負壓而打開並使空氣流向第i 二次空氣供給管76之下游之方式構成。 空氣量控制閥75係用以使二次空氣量適於引擎丨之運行 狀態者。空氣量控制閥75包括以進氣負壓等為動力源之致 動器、伺服馬達或螺線管等。空氣量控制閥7 5之開度由 ECU20控制《於節氣門閥丨丨之開度小於特定角度之情形 時,ECU20使空氣量控制閥75進行閉合動作或使上述節氣 門閥11之開度減少。上述特定角度係預先設定並記憶於 ECU20。又,於上述節氣門閥11之開度大於上述特定開度 之情形時’ ECU20使空氣量控制閥75之開度增大。如此, 154997.doc 14 201239190 空氣量控制閥75對應於上述節氣門閥u之開度而使開度增 減。藉由包括空氣量控制閥75,可以不會過低而適當之流 1向排氣通if 7供給二次空氣。自並非必需空氣量控制閥 75,亦可省略。 ^第2一次空氣供給管77之上游端相對於第}二次空氣供給 管76而於其下游端與簧片閥”之間連接。第2二次空氣供 給官77之下游端連接於第2排氣管52中之第i觸媒2ι與第2 觸媒22之間。更詳細而! ’於較第2觸媒22更靠近第1觸媒 21之位置,第2二次空氣供給管”之下游端連接於第2排氣 管52 〇 一次空氣供給裝置70包括第i通道71與第2通道72。第1 通道71為自簧片閥74至排氣通道7為止之通道,且為藉由 第1二次空氣供給管76而形成之通道。,第1通道71連接 簧片閥74、排氣通道7之分支部31之人口 3㈣漸擴部a之 間^部分。第2通道72為自第i通道71至第2排氣扣内之 排氣通道7之通道’且為藉由第2二次空氣供給管77而形成 之通道。即,第2通道72連接第丄通道71、排氣通道7之第ι 觸媒21及第2觸媒22之間之部分。第i通道了丨之「上游」、 「下游」分別係指空氣自簧片閥74(第i通道71之上游」端 仏)向與排氣通道7之連接部71b(以下亦稱作「下游端 7广」)流動之方向所相關之上游、下游。第2通道?!之 上游」、「下游」分別係指空氣自與第〖通道71之連接部 72a(以下亦稱作「上游端心」)向排氣通道7之連接部 72b(以下亦稱作「下游端72b」)流動之方向所相關之上 154997.doc •15- 201239190 游、下游。 於此,將於氣體自簧片閥74至第2通道72之與第1通道71 之連接部72a為止流過第1通道7 1内時,上述氣體損失之能 量之大小(能量損失)設為L1。又,將於氣體自第2通道72 之下游端72b至上游端72a為止流過第2通道72内時,上述 氣體損失能量之大小(能量損失)設為L2。若對該些加以比 較,則以使L1&lt;L2之方式設計第1及第2通道71、72 »能量 損失係與氣體於流路中之壓力損失為同義。 若將第1通道71令之自第2通道72之連接部72a至與排氣 通道7之連接部71b為止之流路中之氣體之能量損失設為 L3,則L1+L3&lt;L2+L3即可。若將第1通道71中之自簧片閥 74至與排氣通道7之連接部71b之流路61之能量損失設為 L11,則L11 =L 1+L3。另一方面,若將自第2通道72之下游 端72b至上游端72a,進而通過第1通道71至其下游端711?之 流路62之能量損失設為L12 ’則L12=L2+L3。因此,以使 L11&lt;L12之方式設計第1及第2通道71、72即可。 該能量損失之關係可以例如以下方式驗證。即,封閉第 2通道72(例如於下游端72b封閉)並於流路61流動空氣計 測於流路61之下游端(連接部71b)之流量係數u。另一方 面,封閉第1通道71(例如於上游端71a封閉)並於流路“流 動空氣,於流路62之下游端(連接部71b)計測流量係數让2。 此時,若滿足kl&gt;k2,則滿足L11&lt;L12。為於流路61、62 中流動空氣’使用以下之任一方法即可。第i方法係將系 連接於流路61、62之上游端而向流路61、62内輸送空氣之 • 16· 154997.docIt is connected to the open end of the exhaust passage 7, and the other end is a closed end. The branch portion L inlet 31a (that is, a portion that communicates with the exhaust passage 7) is formed as follows, such that the shock wave propagating inside the exhaust passage 7 is also propagated through the inside of the branch portion 31. . The center line of the flow path section of the map] The heart line 2 is the entrance of the heart of 31.糸 曰 曰 曰 曰 曰 ( ( ( ( 流 流 流 流 流 流 流 流 流 流 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 The tapered-divergent nozzle 4 is known as a delta nozzle. Flow through the exhaust - from the subsonic speed to 154997.doc -13- 201239190. The gradual and progressive expansion of the spray is completed. The tapered portion 41 is connected to the lower portion of the throat portion 42 and the gradual portion toward the downstream. The gradually expanding part 43 is a part of the flow path that gradually increases with the wide area, and the section of the flow path is gradually increased. The throat 42 is a new part of the configuration, and the cross-sectional area of the flow path is the smallest: :: M1 and gradually The exhaust passage 7 of the two T exhaust device 50 between the expansion portions 43 is supplied to the air two-artificial enthalpy supply device 70. The secondary air &amp;# π # L human two-roll supply device 7 includes: a reed valve 74 (check valve): a second secondary air supply tributary valve 々μ-shaped rolling supply pipe 76; and a second secondary air supply pipe 77 connected to the first secondary empty rolling supply pipe 76. The reed valve 74 is combined At the upstream end of the second air supply pipe %, the downstream end of the second air supply pipe 76 is connected between the branch pipe 3〇 in the first exhaust pipe and the tapered/diverging nozzle 40. The secondary air supply pipe % is connected to the air cleaner 78 via the reed valve 74 and the air amount control valve 75. The reed valve 74 prevents the exhaust gas from flowing inward from the second secondary air supply pipe %. The reed valve 74 It is constituted by opening a negative pressure by the exhaust passage 7 and flowing the air downstream of the i-th secondary air supply pipe 76. The valve 75 is for adapting the amount of secondary air to the operating state of the engine cymbal. The air amount control valve 75 includes an actuator, a servo motor or a solenoid, etc., which is powered by an intake negative pressure or the like. When the degree of opening of the valve 75 is controlled by the ECU 20, when the opening degree of the throttle valve is less than a specific angle, the ECU 20 closes the air amount control valve 75 or reduces the opening degree of the throttle valve 11. The specific angle is The ECU 20 increases the opening degree of the air amount control valve 75 when the opening degree of the throttle valve 11 is larger than the specific opening degree. Thus, 154997.doc 14 201239190 air volume control valve 75 corresponds to the opening degree of the above-described throttle valve u to increase or decrease the opening degree. By including the air amount control valve 75, it is possible to supply the secondary air to the exhaust air supply if 7 without excessively low. The air amount control valve 75 may be omitted. The upstream end of the second primary air supply pipe 77 is connected to the reed valve at its downstream end with respect to the second secondary air supply pipe 76. The downstream end of the second secondary air supply officer 77 is connected between the i-th catalyst 2ι and the second catalyst 22 in the second exhaust pipe 52. More detailed! The downstream end of the second secondary air supply pipe is connected to the second exhaust pipe 52 at a position closer to the first catalyst 21 than the second catalyst 22, and the primary air supply device 70 includes the i-th channel 71 and The second passage 72. The first passage 71 is a passage from the reed valve 74 to the exhaust passage 7, and is a passage formed by the first secondary air supply pipe 76. The first passage 71 is connected to the reed valve. 74. The population of the branch portion 31 of the exhaust passage 7 is 3 (four) between the gradually expanding portions a. The second passage 72 is the passage of the exhaust passage 7 from the i-th passage 71 to the second exhaust button and is borrowed The passage formed by the second secondary air supply pipe 77. That is, the second passage 72 is connected to the second passage 71, the portion between the first catalyst 21 and the second catalyst 22 of the exhaust passage 7. The i-th passage "Upstream" and "downstream" refer to the connection portion 71b of the air reed valve 74 (upstream of the i-th channel 71) to the exhaust passage 7, respectively (hereinafter also referred to as "the downstream end 7" ") upstream and downstream related to the direction of flow. The "upstream" and "downstream" of the second channel are the connection portions 72b of the air from the connection portion 72a (hereinafter also referred to as "upstream end") of the passage 71 to the exhaust passage 7, respectively (hereinafter also referred to as As the "downstream end 72b"), the direction of the flow is related to 154997.doc •15- 201239190 swim, downstream. Here, when the gas flows from the reed valve 74 to the second passage 72 and the connection portion 72a of the first passage 71 through the first passage 71, the amount of energy (energy loss) of the gas loss is set to L1. Further, when the gas flows through the second passage 72 from the downstream end 72b to the upstream end 72a of the second passage 72, the magnitude (energy loss) of the gas loss energy is set to L2. If these are compared, the first and second passages 71, 72 are designed so that the energy loss in the L1 &lt; L2 is synonymous with the pressure loss of the gas in the flow path. When the energy loss of the gas in the flow path from the connection portion 72a of the second passage 72 to the connection portion 71b of the exhaust passage 7 is set to L3, L1+L3&lt;L2+L3 can. When the energy loss from the reed valve 74 in the first passage 71 to the flow path 61 of the connecting portion 71b of the exhaust passage 7 is L11, L11 = L 1 + L3. On the other hand, if the energy loss from the downstream end 72b of the second passage 72 to the upstream end 72a and the flow path 62 passing through the first passage 71 to the downstream end 711 is L12', then L12 = L2 + L3. Therefore, the first and second passages 71 and 72 may be designed such that L11 &lt; L12. This relationship of energy loss can be verified, for example, in the following manner. That is, the second passage 72 is closed (for example, closed at the downstream end 72b), and the flow coefficient u of the air measured at the downstream end (connecting portion 71b) of the flow path 61 is flowed through the flow path 61. On the other hand, the first passage 71 is closed (for example, closed at the upstream end 71a), and the flow path "flows air", and the downstream end of the flow path 62 (the connection portion 71b) measures the flow coefficient to 2. In this case, if kl is satisfied. K2 satisfies L11 &lt; L12. It is sufficient to use the following method for flowing air in the flow paths 61 and 62. The i-th method is to connect the upstream ends of the flow paths 61 and 62 to the flow path 61, Air transport within 62 • 16· 154997.doc

201239190 方法。第2方法係將泵連接於流路61、62之下游端而自流 路61、62抽吸空氣之方法。 於可忽略空氣量控制閥75及/或空氣濾清器78之能量損 失時,亦可於流路61包含該些構件。該情形時,流路61係 自大氟開放位置至連接部71b之流路。又,於氣體自大氣 開放位置流動至第2通道72之與第丨通道”之連接部Ma為 述此里損失l 1設為上述氣體損失能量之大小。 1係數係私貫際流過之空氣流量相對於由實際開口面 積與壓差所決定之理論空氣量之比1,藉由實際之空氣 流量除以理論空氣流量而得。 氣體流過管路時之能量損失之例包含因與壁面之摩擦所 造成,損失、管路之入口或出口之損失、管路之弯曲所造 成之損失、流路剖面積之變化所引起之損失、及因閥所造 成之損失等。流路剖面積之變化所引起之損失係指剖面積 錢變大或變小時之損失、及剖面積緩慢變大或變小時之 壁面之表面粗糖度越粗縫、管路之長度越長、管路之叫 =二Γ壁面之摩擦所造成之損失越大。管徑除以 ,曲:曲率半徑之比越大、f曲之角度越大,則管路之彎 曲所造成之損失越大。因間 七叫电 Θ斤成之知失會根據閥之種類 或開度而不同,需要藉由f ▲ W 鞛由貫驗而求出。就簧片閥之損失而 吕,可藉由例如測定簧片閥 ^ μ 上/拜與下游之間之壓力差、 汽片閥之開度(流路之剖面 + %道山r丄V )夂貝量流量之關係,並基於 此而導出壓力差與損失係數之關係。 土於 154997.doc 201239190 圖2係普通之漸縮·漸擴噴嘴之模式圖。漸縮部“之上游 端之流路剖面⑽、喉部42之流路剖面積A2及漸擴和 之下游端之流路剖面積幻存在A1&gt;A2、A2&lt;A3之關係。喉 部42之流㈣_A2與漸料41之下游狀料剖面積及 渐擴部43之上游端之流路剖面積相同。本實施形態中,漸 ㈣Μ!與漸擴部4 3之流路剖面積分別沿著流動方向而以固 定之比例變化。然而,漸縮部41及漸擴部43亦可具有其他 ⑽m mm擎中所㈣之喷嘴般’採用流路剖 面積呈階段性(Step by Step)地變化之形狀。又,亦可使喷 嘴内表面形成為平滑之曲面。 漸縮-漸擴喷嘴40係以滿足下述數式〇)、(2)所示之條件 之方式形成。藉由流入至喉部42之廢氣之流速達到馬赫 1(即音速),而可於漸擴部43中使廢氣加速至超音速。 [數1] dM _ 八 ,. dx l~M2 ^ [數2] Λ Ξ Μ γ Μ2 ί4/) 1 dA ——---- L 2 J 2 [d) A dx ⑵ 數式(1)表示伴隨有黏性摩擦之一維流動中之排氣管來 狀與馬赫數之關係。數式(2)表不數式(1)中之八。今此 中’ Μ表示馬赫數,A表示排氣管之任意剖面之剖面積,〇 表示上述任意剖面之管相當直徑,γ表示比埶比, …m,X表不流 -18- 154997.doc201239190 Method. The second method is a method of connecting a pump to the downstream ends of the flow paths 61, 62 and sucking air from the flow paths 61, 62. These components may also be included in the flow path 61 when the energy loss of the air volume control valve 75 and/or the air cleaner 78 is negligible. In this case, the flow path 61 is a flow path from the large fluorine open position to the connection portion 71b. Further, in the connection portion Ma where the gas flows from the open position of the atmosphere to the second passage 72 and the second passage", the loss l 1 is the magnitude of the gas loss energy. The coefficient is the air flowing through the private passage. The ratio of the flow rate to the theoretical air amount determined by the actual opening area and the pressure difference is obtained by dividing the actual air flow rate by the theoretical air flow rate. Examples of energy loss when the gas flows through the pipeline include the wall surface The loss caused by friction, the loss of the inlet or outlet of the pipeline, the loss caused by the bending of the pipeline, the loss caused by the change of the cross-sectional area of the flow path, and the loss caused by the valve, etc. The loss caused by the loss of the cross-sectional area becomes larger or smaller, and the surface of the wall whose surface area is slowly becoming larger or smaller becomes thicker and coarser, the length of the pipeline is longer, and the pipeline is called The greater the loss caused by the friction of the wall surface. The diameter of the pipe is divided by the larger the ratio of the radius of curvature and the larger the angle of the f curve, the greater the loss caused by the bending of the pipe. Cheng Zhizhi will be based on the valve The class or degree of opening differs and needs to be determined by means of f ▲ W 。. In terms of the loss of the reed valve, for example, the pressure difference between the reed valve and the downstream and downstream can be determined. The relationship between the opening degree of the steam valve (the profile of the flow path + % Daoshan r丄V) and the flow rate of the scallop, and based on this, the relationship between the pressure difference and the loss coefficient is derived. Tu 154997.doc 201239190 Figure 2 is common Schematic diagram of the tapered and divergent nozzle. The flow path section (10) at the upstream end of the tapered portion, the cross-sectional area A2 of the flow path of the throat portion 42, and the cross-sectional area of the flow path at the downstream end of the divergence and the downstream end are illusory A1&gt;A2 , A2 &lt; A3 relationship. The flow of the throat portion 42 (4)_A2 is the same as the cross-sectional area of the downstream material of the tapered material 41 and the upstream end of the diverging portion 43. In the present embodiment, the flow path cross-sectional areas of the progressive (four) Μ and the dilating portion 43 are changed in a fixed ratio along the flow direction. However, the tapered portion 41 and the diverging portion 43 may have a shape in which the flow path sectional area is changed stepwise by the nozzle of the other (10) m mm. Further, the inner surface of the nozzle can be formed into a smooth curved surface. The tapered-swelling nozzle 40 is formed to satisfy the conditions shown in the following equations (2) and (2). The Mach 1 (i.e., the speed of sound) is reached by the flow rate of the exhaust gas flowing into the throat portion 42, and the exhaust gas can be accelerated to the supersonic speed in the dip portion 43. [Number 1] dM _ 八,. dx l~M2 ^ [Number 2] Λ Ξ Μ γ Μ2 ί4/) 1 dA ——---- L 2 J 2 [d) A dx (2) Equation (1) It is accompanied by the relationship between the shape of the exhaust pipe and the Mach number in one-dimensional flow of viscous friction. The equation (2) does not count eight of the equations (1). In this case, 'Μ denotes the Mach number, A denotes the sectional area of any section of the exhaust pipe, 〇 denotes the diameter of the tube of any of the above sections, γ denotes the specific ratio, ...m, X does not flow -18- 154997.doc

201239190 動方向上之距離,f表示摩擦係數。 如圖2所示,將喉部42上游之總壓力(Full Pressure)設為 P〇,將喉部42下游之靜壓力(Static Pressure)設為P。如圖3 所示’於該些壓力之比Ρ/Ρ0小於臨界壓力比=0.528(圖3之 點C)時’於喉部42之速度成為音速(馬赫1)以上,其結果, 於漸擴部43之速度成為超音速。因此,若以使p/p〇小於臨 界壓力比之方式提昇總壓力P〇,則可於漸縮-漸擴喷嘴4〇 形成超音速之流動。 若於漸縮-漸擴噴嘴40之流速成為超音速,則會產生朝 向漸擴部43下游傳播之衝擊波35b與朝向上游傳播之膨脹 波35c(參照圖6)。衝擊波35b與膨脹波35c之間之空間内之 流體急速膨脹,因此流過排氣通道7之廢氣之壓力降低。 其結果’藉由絕熱膨服(Adiabatic Expansion)所引起之絕 熱冷卻(Adiabatic cooling)之效果,可迅速降低廢氣之溫 度。而且’本發明者進行積極研究之結果發現,可藉由將 漸縮-漸擴喷嘴4 0與分支部3丨加以組合而實現該狀態。 下面,一面參照圖4A〜圖4C 一面說明廢氣於排氣通道7 中成為壓力較低之狀態、且溫度較低之狀態之原理。圖 4A〜圖4C模式性地表示包括排氣裝置5〇之引擎1。圖4八〜圖 4C中,對與圖1及圖2中所圖示者相同或同等之構件附上相 同符號。 如圖4A所示,若於引擎1之排氣衝程打開排氣口 9a,則 高壓之廢氣36自燃燒室1()通過排氣❿向排氣通道7之上 游4 7a喷出。於排氣σ 9a開始打開之時間點,燃燒室1〇與 154997.doc -19- 201239190 排氣通道7之上游部乃之間之壓力差較大,因此廢氣刊之 速度達到音速,從而於排氣通道7之上游部乃產生衝擊波 35。隨著排氣口 9a較大地打開,向排氣通道7之上游部、 流出之廢氣量增多,但廢氣之速度變慢。又,廢氣隨著於 排氣通道7之上游部7a前進而減速。如圖4A所示,衝擊波 35自排氣通道7之上游部7&amp;傳播至第丨排氣管51之内部,進 而朝向下游以尚速傳播。另一方面,廢氣36以較衝擊波35 低之速度於排氣通道7中滞後行進。 如圖4B所示,於第i排氣管51之内部前進之衝擊波”在 通過刀支部31之入口 31a時,分成在排氣通道7中傳播之衝 擊波與在分支部31中傳播之衝擊波,且分別獨立地於排氣 通道7與分支部31中行進。於排氣通道7中前進之衝擊波” 通過漸縮-漸擴噴嘴40後衰減、消失。另一方面,於分支 部31中前進之衝擊波35於分支部31之反射部3lb反射並於 分支部31逆行而返回至排氣通道7。 如圖4C所示,以使反射之衝擊波35自分支部31返回至排 氣通道7之時間與高壓之廢氣36到達分支部31之入口 3ia中 央之時間相同或遲於其的方式,設定分支部31之長度。因 此,於較漸擴部43更為上游且在分支部3丨之入口 31a或其 下游之排氣通道7中,衝擊波35與廢氣36衝撞。由此,可 提高漸縮-漸擴喷嘴40之喉部42之上游之總壓力。其結 果,可實現壓力比Ρ/Ρ0小於臨界壓力比之狀態’從而可於 漸縮-漸擴噴嘴40中形成超音速之流動。 圖5係表示衝擊波之行進路徑與廢氣之行進路徑之排氣 154997.doc -20· 201239190 通道7等之模式圖。將自排氣口 %之中心心至分支部入口 31a之流路剖面中心線χ之距離(流路長度)設為u,且將排 氣通道7之流路剖面中心線丫與反射部m之間之距離(流路 長度)設為Ls。進而,將廢氣36之速度設為%,將衝擊波 35之傳播速度設為Vs。自排氣口%打開起至廢氣刊到達入 口 3 la為止之時間T1以式(3)表示。又,自排氣口 %打開起 至衝擊波35於反射部31b反射並到達排氣通道7之中心線¥ 為止之時間T2以式(4)表示。 T1 .................. T2==(Le+2Ls)/V .......(4) 若T1ST2,則反射之衝擊波35與廢氣36衝撞。即,若201239190 The distance in the moving direction, f is the coefficient of friction. As shown in Fig. 2, the total pressure (Full Pressure) upstream of the throat portion 42 is set to P, and the static pressure (Static Pressure) downstream of the throat portion 42 is set to P. As shown in Fig. 3, when the ratio Ρ/Ρ0 of the pressures is less than the critical pressure ratio = 0.528 (point C in Fig. 3), the velocity at the throat 42 becomes the speed of sound (Mach 1) or more, and as a result, it is gradually expanded. The speed of the portion 43 becomes supersonic. Therefore, if the total pressure P 提升 is raised so that p / p 〇 is smaller than the critical pressure ratio, the supersonic flow can be formed in the tapered - diverging nozzle 4 。 . When the flow velocity of the tapered-smoothing nozzle 40 becomes supersonic, a shock wave 35b that propagates downstream of the diverging portion 43 and an expanding wave 35c that propagates upstream (see Fig. 6) are generated. The fluid in the space between the shock wave 35b and the expansion wave 35c rapidly expands, so that the pressure of the exhaust gas flowing through the exhaust passage 7 is lowered. As a result, the temperature of the exhaust gas can be rapidly reduced by the effect of Adiabatic cooling caused by Adiabatic Expansion. Further, as a result of active research by the inventors, it has been found that this state can be realized by combining the tapered-divergent nozzle 40 and the branch portion 3A. Next, the principle in which the exhaust gas is in a state where the pressure is low in the exhaust passage 7 and the temperature is low will be described with reference to FIGS. 4A to 4C. 4A to 4C schematically show the engine 1 including the exhaust unit 5〇. In Figs. 4 to 4C, the same or equivalent components as those shown in Figs. 1 and 2 are attached with the same reference numerals. As shown in Fig. 4A, if the exhaust port 9a is opened by the exhaust stroke of the engine 1, the high-pressure exhaust gas 36 is ejected from the combustion chamber 1 () through the exhaust port to the exhaust passage 7 above. At the time when the exhaust gas σ 9a starts to open, the pressure difference between the combustion chamber 1〇 and the upstream portion of the 154997.doc -19-201239190 exhaust passage 7 is large, so the speed of the exhaust gas reaches the speed of sound, thereby arranging The shock wave 35 is generated in the upstream portion of the gas passage 7. As the exhaust port 9a is opened largely, the amount of exhaust gas flowing out to the upstream portion of the exhaust passage 7 increases, but the speed of the exhaust gas becomes slow. Further, the exhaust gas is decelerated as it advances toward the upstream portion 7a of the exhaust passage 7. As shown in Fig. 4A, the shock wave 35 propagates from the upstream portion 7&amp; of the exhaust passage 7 to the inside of the third exhaust pipe 51, and then propagates toward the downstream at a constant speed. On the other hand, the exhaust gas 36 travels behind the exhaust passage 7 at a lower speed than the shock wave 35. As shown in FIG. 4B, the shock wave advancing inside the i-th exhaust pipe 51 is divided into a shock wave propagating in the exhaust passage 7 and a shock wave propagating in the branch portion 31 when passing through the inlet 31a of the knife branch portion 31, and Each of the exhaust waves 7 and the branch portion 31 travels independently. The shock wave that advances in the exhaust passage 7 is attenuated and disappears by the tapered-smoothing nozzle 40. On the other hand, the shock wave 35 that has advanced in the branch portion 31 is reflected by the reflection portion 31b of the branch portion 31 and is reversed to the branch portion 31 to return to the exhaust passage 7. As shown in FIG. 4C, the branch portion 31 is set such that the time during which the reflected shock wave 35 returns from the branch portion 31 to the exhaust passage 7 is the same as or later than the time at which the high-pressure exhaust gas 36 reaches the center of the inlet 3ia of the branch portion 31. The length. Therefore, the shock wave 35 collides with the exhaust gas 36 in the exhaust passage 7 which is further upstream than the gradually expanding portion 43 and at the inlet 31a of the branch portion 3A or downstream thereof. Thereby, the total pressure upstream of the throat 42 of the tapered-divergent nozzle 40 can be increased. As a result, a state in which the pressure ratio Ρ/Ρ0 is smaller than the critical pressure ratio can be achieved so that the supersonic flow can be formed in the tapered-smoothing nozzle 40. Fig. 5 is a schematic view showing the exhaust path of the shock wave and the exhaust path of the exhaust gas 154997.doc -20· 201239190 channel 7 and the like. The distance (flow path length) from the center of the exhaust port % to the center line 流 of the flow path section of the branch inlet 31a is u, and the center line 丫 of the flow path of the exhaust passage 7 and the reflection portion m The distance (flow path length) is set to Ls. Further, the speed of the exhaust gas 36 is set to %, and the propagation speed of the shock wave 35 is set to Vs. The time T1 from the time when the exhaust port is opened until the exhaust gas reaches the inlet 3 la is expressed by the formula (3). Further, the time T2 from when the exhaust port % is opened until the shock wave 35 is reflected by the reflecting portion 31b and reaches the center line ¥ of the exhaust passage 7 is expressed by the formula (4). T1 .................. T2==(Le+2Ls)/V .......(4) If T1ST2, the reflected shock wave 35 and exhaust gas 36 Crash. That is, if

Le/VeS(Le+2LS)/VS,則於較漸擴部43更為上游且在分支 部31之入口 31a或其下游之排氣通道7中,反射之衝擊波35 與廢氣36衝撞。再者,為方便起見,例如亦可將廢氣刊之 最大速度視為上述速度Ve,或將平均速度視為上述速度Le/VeS (Le+2LS)/VS, which is further upstream than the diverging portion 43 and in the inlet 31a of the branch portion 31 or the exhaust passage 7 downstream thereof, the reflected shock wave 35 collides with the exhaust gas 36. Furthermore, for convenience, for example, the maximum speed of the exhaust gas can be regarded as the above-mentioned speed Ve, or the average speed can be regarded as the above speed.

Ve。同樣地,例如亦可將反射之衝擊波35之最大傳播速度 視為上述傳播速度Vs,或將平均傳播速度視為上述傳播速 度Vs。 如圖5所示’將自分支部入口 3 1 a之流路剖面中心線X至 漸擴部43之上游端為止之距離(流路長度)設為Ld,將自排 氣口 9a打開至關閉為止之時間設為tv。自排氣口 9a打開至 廢氣36之末尾部到達漸擴部43之上游端為止之時間T3以式 (5)表示。又,自排氣口 9a打開至衝擊波35於反射部31b反 射並達到漸擴部43之上游端為止之時間T4以式(6)表示。 154997.doc -21 - 201239190 T3=tv+(Le+Ld)/Ve.....(5) T4=(Le+2Ls+Ld)/Vs ----(6) 右T4ST3 ’則於廢氣36全部通過喉部42之前,可使反射 之衝擊波35與廢氣36衝撞。即,若(Le+2Ls+Ld)/Vs$tv+ (Le+Ld)/Ve,則於廢氣刊全部通過喉部42之前,可使反射 之衝擊波35與廢氣36衝撞。 若排氣通道7之流路剖面中心線γ與反射部3丨b之間之距 離LS比較小’則可抑制分支部3 1中之衝擊波35之衰減。由 此’例如亦可將距離Ls設為小於距離Le。 廢氣之壓力藉由於漸縮部41之壓縮而提高。此外,藉由 衝擊波35與廢氣36之衝撞而使於漸縮部41之廢氣36之壓力 進而提高。如此一來’漸縮-漸擴喷嘴40之入口上游之總 壓力P0提尚’因此與此相對應’入口上游之總壓力p〇與喉 部之下游靜壓力p之比p/p〇小於臨界壓力比〇 528。其結 果’廢氣36之速度於喉部42達到音速。 圖6係使藉由紋影攝影法拍攝漸縮_漸擴喷嘴之内部而得 之照片模式化之模式圖。藉由廢氣36之速度達到音速,而 於漸縮·漸擴喷嘴40產生新的衝擊波。以下,方便起見將 新產生之衝擊波稱作行進衝擊波35b。該行進衝擊波351?於 通過漸縮-漸擴噴嘴40之漸擴部43時加速。於產生行進衝 擊波35b時’產生向與行進衝擊波35b相反之方向前進之膨 脹波35c。行進衝擊波3513於漸擴部43加速,與此同時,膨 脹波35(;向與行進衝擊波35b相反之方向行進。由此,存在 於行進衝擊波35b與膨脹波35c之間之廢氣36之壓力及溫度 154997.doc • 22- 201239190 大幅降低》如後述般,廢氣成為大氣壓以下,即成為負 壓。 圖7及圖8表示本案發明者所進行之模擬之結果。圖7表 示於漸縮-漸擴喷嘴40剛產生新的衝擊波35b後之排氣通道 7之各地點(Position)之廢氣速度(Exhaust Gas Velocity)及 廢氣壓力(Exhaust Gas Pressure)。圖8表示於漸縮-漸擴喷 嘴40更產生新的衝擊波35b後之排氣通道7之各地點 (Position)之廢氣速度(Exhaust Gas Velocity)及廢氣溫度 (Exhaust Gas Temperature) 〇 當於漸縮-漸擴喷嘴40產生衝擊波35b時,該衝擊波35b 於漸擴部43加速。如此一來,如圖7及圖8所示,廢氣之流 速迅速增大,廢氣之壓力及溫度迅速降低。再者,圖7及 圖8係表示廢氣流速之圖,並未表示衝擊波之傳播速度。 圖7及圖8表示將漸縮-漸擴喷嘴4〇之喉部42設定得較長之 情形之模擬結果。 當於分支部31反射之衝擊波35與廢氣%衝撞時,衝擊波 35較廢氣36而先行在喉部42傳播。此時,於廢_與衝擊 波35之間之空間中產生絕熱膨脹而導致壓力降低,因此, 如受到衝擊波35牽拉般廢氣36不降低速度地流過喉部❿ 由此,較佳為根據引擎而設定喉部42之以相同流路剖面積 連續之部分之長度。由此,可根據㈣擎而設^於漸擴部 43對衝擊波说進行加速之時機,換言之降低廢氣之壓力 及溫度之時機。 如此,根據本實施形態之引擎!, J权无刖而大幅降低 ]54997.doc •23· 201239190 排氣通道7中之廢氣之壓力及溫度。 其次,使用表示本案發明者進行模擬之結果之圖9A〜圖 9C對二次空氣供給裝置70之作用進行說明。二次空氣供給 裝置70藉由於較排氣通道7之漸擴部43更為上游之部分產 生之負壓,而向排氣通道7之較第1觸媒21更為下游之部分 有效率地供給二次空氣。 圖9A係表示於本實施形態之引擎丨中觀測到之曲柄轴 16(參照圖1)之旋轉角(曲柄角)與排氣通道7内之壓力之關 係之-例的圖。當於膨脹衝程之中途打開排氣_時,會 自燃燒室10向排氣通道7内排出高壓之廢氣。因此,如參 照符號91所示,排氣通道7内成為正壓。其後,藉由漸縮_ 漸擴喷嘴40之作用而如參照符號92所心於排氣通道7内 產生較大之負愿。其後,藉由排氣脈動而如參照符號Μ所 示’於排氣通道7内交替產生正壓與負壓。於藉由漸縮·漸 擴喷嘴40之作用而產生之較大的負塵之影響下,該排氣脈 動之振幅變得較通常大。 圖9B係表示於本實施形態之引擎1中所觀測到之曲柄轴 二6(參照圖υ之旋轉角(曲柄角)與第1通道71中之氣體(通過 簧片閥74之氣體)之質量流量之關係之-例的圖。其中, 就質量流量而言,以正值表示自第1通道71之上游端(菁片 間74側)朝向下游端(排氣通道7側)之方向之流量,而以負 丁向其相反方向之流量。當於排氣通道7内產生較 時(圖9Α之參照符號92),第1通道71内亦成為負 ,其結果’簧片閥74打開。由此,如圖9Β中參照符號94 154997.doc •24- 201239190 所不,氣體向第1通道71内流入。 自菁片閥74通過第1通道7 1並到達排氣通道7之流路 61(參照圖1) ’與通過第2通道72之下游端72b至上游端72a 並到達排氣通道7之流路62(參照圖1}之能量損失之大小關 係如上所述。即,氣體流過通過簧片閥74之流路61時所損 失之能量’小於氣體流過通過第2通道72之流路62時所損 失之能量。能量損失小之流路較能量損失大之流路而氣體 之流量增多’因此經由簧片閥74流過第1通道71之流量增 多。即,較之自第2通道72流至第1通道71之氣體量,自引 擎1外部流入至第1通道71之氣體量增多。從而,可將含有 大量氧之引擎1之外部空氣(二次空氣)導入至第丨通道71。 簧片閥74雖為僅容許向進入至第1通道71之一方向之氣 體之流動之構造,但於暫時打開後即將閉合之前之一瞬間 會產生向反方向之氣體之流動。圖9B中為呈現負質量流量 值之理由。 於空氣自引擎1外部導入至第i通道71之後,當於較漸擴 部43更為上游之排氣通道7内產生正壓時(例如,圖9A之參 照符號95),第1通道71内之空氣被擠出。簧片閥74使氣體 無法於自第丨通道7丨朝向引擎丨外部之方向流動,因此第1 通道71内之空氣被擠出至第2通道72。 圖9C係表示曲柄軸16之旋轉角(曲柄角)與排氣通道7及 -次空氣供給裝置7G之各部分中之氧量(氧濃度)之關係之 一例的圖。具體而言,曲線96a表示於第丨通道7ι中第2通 道72之連接部72a與排氣通道7之間(例如圖丨所示之測定點 154997.doc -25· 201239190 a)之氧濃度。又,曲線96b表示第2通道72之中間部附近(上 游端72a與下游端72b之間。例如圖1所示之測定點b)之氧 濃度。進而,曲線96c表示排氣通道7之較第i觸媒21更為 下游之部分(第i及第2觸媒21、22之間。例如圖⑽示之測 定點Ο之氧濃度。又,曲線96d表示第i通道連接部7比之 上游之排氣通道7内(例如圖1所示之測定點d)之氧濃度。 若對曲線96a、96c、96d加以比較,則得知第丨通道”内 之氧濃度高於排氣通道7内之氧濃度。此情況表示引擎”卜 之二次空氣導入至第1通道71。若對曲線96b、96c、96(1加 以比較’則得知第2通道72内之氧濃度高於排氣通道7内之 氧濃度。若對曲線96&amp;、鳴加以比車交,則得知第2通道72 内之氧濃度高於第1通道71内(靠近排氣通道7之位置)之氧 濃度。因此’得知引擎i外之二次空氣導人至第2通道72。 若二次空氣導入至第2通道72,則該二次空氣會供給至第! 及第2觸媒2卜22之間’因而實現二次空氣供給之目的。 根據對曲線96c、96d之比較而得知,較第i及第2觸媒 2卜22間之排氣通道7(例如圖i所示之測定點〇之氧濃度, 第】通道連接部71b之上游之排氣通道7内(例如⑸所示之 測定點d)之氧濃度較低4表示二次空氣導人至排氣通道 7之較第i觸媒21更為下游。通常’如第2通道㈣之氧濃 度(例如敎點b)高於第i通道連接部爪上游之排氣通道 7(例如測定點d)之氧濃度,則可認為實現向第2通道Μ導入 二次空氣之㈣。若能確認到該情況,則可實現向第工及 第2觸媒21、22間之排氣通道7供給二次空氣之目的。 J54997.doc -26· 201239190 如圖9C之曲線96c中參照符號97所示,氧濃度與圖9八之 參照符號95所示之產生正壓(於漸擴部43之上游產生正壓) 之時機大致同步地增加。此表示導入至第丨通道71之二次 空氣經由第2通道72送入第1及第2觸媒21、22間之排氣通 道7。 如以上所說明,根據本實施形態,不使用強制性地向排 氣通道7送入空氣之專用裝置即可向排氣通道7之較第丄觸 媒21更為下游之部分供給足量之二次空氣。即,使用利用 廢氣能量而產生之負壓自外部導入二次空氣,相同地使用 藉由廢氣能量而產生之正壓將導入之二次空氣送出至第i 觸媒2 1之下游。如此,使用廢氣能量實現泵作用,因而可 減低引擎輸出之損失。 而且’可於漸擴部43上游之排氣通道7產生較大之負 壓,因而可增大排氣脈動之振幅。因此,即便於引擎丄以 南轉速或而負載狀態運行時,亦可利用伴隨衝擊波產生之 較大之負壓與因排氣脈動所產生之充足之正壓而向第1觸 媒21下游^_排氣通道7供給二次空氣。 再者,亦可併用用以供給空氣之其他泵裝置。即便於該 情形時,亦可減輕對泵施加之負載,因而可減少引擎輸出 之損失。 該實施形態中,流過自第1通道71之上游端71a至下游端 7 lb之机路61之氣體之能量損失,小於流過自第2通道之 下游端72b至第1通道71之下游端71b之流路62之氣體之能 里扣失。即,封閉第2通道72而自第i通道上游端7ia流過 154997.doc -27· 201239190 空氣時之第1通道下游端71b之流量係數,大於在第2通道 72之連接部之上游封閉第1通道71而自第2通道下游端72b 流過空氣時之第1通道下游端71b之流量係數。由此,當於 較漸擴部43更為上游產生負壓時,第2通道72内之空氣不 逆流,而可通過第1通道71之簧片閥74將二次空氣確實地 導入至第1通道71 〇因此,其後,於漸擴部43上游之排氣 通道7成為正壓時,可將該導入之二次空氣送入至第2通道 72 ° 又,該實施形態中,排氣裝置5〇包括分别配置於第2通 道72之下游端72b之上游及下游之排氣通道7中之第i及第2 觸媒2丨、22。根據該構成,可提高向第2觸媒22供給之廢 氣之氧濃度。因此,可使第丨觸媒21主要作為還原觸媒發 揮作用,且使第2觸媒22主要作為氧化觸媒發揮作用。於 第1觸媒21及第2觸媒22應用三元觸媒之情形時,為進行還 原反應及氧化反應之雙方而必需將理論空燃比之廢氣導入 至該些觸媒。於使第丨觸媒21主要作為還原觸媒發揮功能 之情形時,亦可向第i觸媒21導入富含燃料之廢氣。又, 於使第2觸媒22作為氧化觸媒發揮功能之情形時,亦可向 第2觸媒22導入傾向於較低空燃比之廢氣。由此,第丨觸媒 21及第2觸媒22協作而可進行還原反應及氧化反應之雙 方,因而可有效率地除去廢氣中之有害成分。由此,不2 向第1觸媒21導入理論空燃比之廢氣,因而可擴大能夠除 去有害成分之空燃比之範圍。因此,不必嚴密控制空辦 比。 •28- 154997.docVe. Similarly, for example, the maximum propagation velocity of the reflected shock wave 35 may be regarded as the above-described propagation velocity Vs, or the average propagation velocity may be regarded as the above-described propagation velocity Vs. As shown in Fig. 5, the distance (flow path length) from the center line X of the flow path section of the branch inlet 3 1 a to the upstream end of the diverging portion 43 is Ld, and the self-venting port 9a is opened to be closed. The time is set to tv. The time T3 from when the exhaust port 9a is opened until the end of the exhaust gas 36 reaches the upstream end of the diverging portion 43 is expressed by the formula (5). Further, the time T4 from when the exhaust port 9a is opened until the shock wave 35 is reflected by the reflecting portion 31b and reaches the upstream end of the diverging portion 43 is expressed by the formula (6). 154997.doc -21 - 201239190 T3=tv+(Le+Ld)/Ve.....(5) T4=(Le+2Ls+Ld)/Vs ----(6) Right T4ST3 'is in exhaust gas 36 The reflected shock wave 35 can be collided with the exhaust gas 36 before passing through the throat 42 all. That is, if (Le + 2Ls + Ld) / Vs $ tv + (Le + Ld) / Ve, the reflected shock wave 35 can collide with the exhaust gas 36 before the exhaust gas passes through the throat portion 42. If the distance γ between the center line γ of the flow path of the exhaust passage 7 and the reflection portion 3丨b is small, the attenuation of the shock wave 35 in the branch portion 31 can be suppressed. Thus, for example, the distance Ls can also be set to be smaller than the distance Le. The pressure of the exhaust gas is increased by the compression of the tapered portion 41. Further, the pressure of the exhaust gas 36 of the tapered portion 41 is further increased by the collision of the shock wave 35 with the exhaust gas 36. In this way, the total pressure P0 upstream of the inlet of the tapered-divergent nozzle 40 is increased. Therefore, the ratio of the total pressure p〇 upstream of the inlet to the downstream static pressure p of the throat is less than the critical value. The pressure is 〇528. As a result, the speed of the exhaust gas 36 reaches the speed of sound at the throat 42. Fig. 6 is a schematic view showing the patterning of a photograph obtained by photographing the inside of a tapered_smoothing nozzle by a schlieren method. The speed of sound is reached by the velocity of the exhaust gas 36, and the tapered/divergent nozzle 40 generates a new shock wave. Hereinafter, the newly generated shock wave is referred to as a traveling shock wave 35b for convenience. The traveling shock wave 351 is accelerated when passing through the diverging portion 43 of the tapered-divergent nozzle 40. When the traveling shock wave 35b is generated, the expansion wave 35c that advances in the opposite direction to the traveling shock wave 35b is generated. The traveling shock wave 3513 is accelerated in the diverging portion 43 and, at the same time, the expanding wave 35 (which travels in the opposite direction to the traveling shock wave 35b. Thereby, the pressure and temperature of the exhaust gas 36 existing between the traveling shock wave 35b and the expanding wave 35c 154997.doc • 22-201239190 "Large reduction" As described later, the exhaust gas becomes below atmospheric pressure, that is, it becomes a negative pressure. Fig. 7 and Fig. 8 show the results of the simulation performed by the inventor of the present invention. Fig. 7 shows the tapered-smoothing nozzle. The exhaust gas velocity (Exhaust Gas Velocity) and the exhaust gas pressure (Exhaust Gas Pressure) of each of the exhaust passages 7 immediately after the new shock wave 35b is generated. Fig. 8 shows that the tapered-semi-expansion nozzle 40 is more new. Exhaust Gas Velocity and Exhaust Gas Temperature of each position of the exhaust passage 7 after the shock wave 35b. When the tapered-smoothing nozzle 40 generates the shock wave 35b, the shock wave 35b is The dilating portion 43 is accelerated. As a result, as shown in Fig. 7 and Fig. 8, the flow rate of the exhaust gas rapidly increases, and the pressure and temperature of the exhaust gas rapidly decrease. Further, Fig. 7 and Fig. 8 show the flow rate of the exhaust gas. The figure shows the propagation speed of the shock wave. Fig. 7 and Fig. 8 show the simulation results of the case where the throat portion 42 of the tapered-divergent nozzle 4 is set to be long. The shock wave 35 and the exhaust gas reflected at the branch portion 31 are shown. At the time of the collision, the shock wave 35 propagates first in the throat 42 than the exhaust gas 36. At this time, adiabatic expansion occurs in the space between the waste_and the shock wave 35, resulting in a pressure drop, and therefore, the exhaust gas 36 is pulled by the shock wave 35. It is preferable to set the length of the portion of the throat portion 42 that is continuous with the same flow path sectional area according to the engine, thereby setting the length of the portion of the throat portion 42 in accordance with the engine. The timing of accelerating the shock wave, in other words, the timing of reducing the pressure and temperature of the exhaust gas. Thus, according to the engine of the present embodiment, the J right is greatly reduced] 54997.doc •23· 201239190 Exhaust gas in the exhaust passage 7 Next, the operation of the secondary air supply device 70 will be described with reference to Figs. 9A to 9C showing the results of the simulation performed by the inventors of the present invention. The secondary air supply device 70 is provided by the exhaust passage 7 The expanded portion 43 is more negatively generated by the upstream portion, and the secondary air is efficiently supplied to the portion of the exhaust passage 7 that is further downstream than the first catalyst 21. Fig. 9A shows the engine of the present embodiment. A diagram showing the relationship between the rotation angle (crank angle) of the crankshaft 16 (refer to FIG. 1) and the pressure in the exhaust passage 7 in the medium. When the exhaust gas _ is opened midway through the expansion stroke, self-combustion occurs. The chamber 10 discharges high-pressure exhaust gas into the exhaust passage 7. Therefore, as indicated by reference numeral 91, the inside of the exhaust passage 7 becomes a positive pressure. Thereafter, by the action of the tapered_swelling nozzle 40, a large negative is generated as shown by reference numeral 92 in the exhaust passage 7. Thereafter, positive pressure and negative pressure are alternately generated in the exhaust passage 7 by exhaust pulsation as indicated by reference numeral ’. Under the influence of the large negative dust generated by the action of the tapered/diverging nozzle 40, the amplitude of the exhaust pulsation becomes larger than usual. Fig. 9B shows the mass of the crankshaft 2 (refer to the rotation angle (crank angle) of Fig. 与 and the gas in the first passage 71 (gas passing through the reed valve 74) observed in the engine 1 of the present embodiment. In the case of the flow rate, the flow rate in the direction from the upstream end of the first passage 71 (the side between the cyanites 74) toward the downstream end (the side of the exhaust passage 7) is represented by a positive value. And the flow rate of the negative direction to the opposite direction. When the time is generated in the exhaust passage 7 (refer to reference numeral 92 in Fig. 9A), the inside of the first passage 71 also becomes negative, and as a result, the reed valve 74 is opened. Therefore, as shown in Fig. 9A, reference numeral 94 154997.doc •24-201239190 does not, the gas flows into the first passage 71. The self-crystallization valve 74 passes through the first passage 71 and reaches the flow path 61 of the exhaust passage 7 ( Referring to Fig. 1), the magnitude of the energy loss with the flow path 62 (refer to Fig. 1) passing through the downstream end 72b of the second passage 72 to the upstream end 72a and reaching the exhaust passage 7 is as described above. That is, the gas flows through The energy lost by the flow path 61 of the reed valve 74 is less than the energy lost when the gas flows through the flow path 62 passing through the second passage 72. The flow path having a small amount of loss is larger than the flow path having a large energy loss and the flow rate of the gas is increased. Therefore, the flow rate through the first passage 71 through the reed valve 74 is increased. That is, the flow from the second passage 72 to the first passage 71 is increased. The amount of gas increases the amount of gas flowing from the outside of the engine 1 to the first passage 71. Therefore, the outside air (secondary air) of the engine 1 containing a large amount of oxygen can be introduced into the second passage 71. The reed valve 74 is Only the configuration of the flow of the gas into the direction of one of the first passages 71 is allowed, but the flow of the gas in the opposite direction is instantaneously generated immediately after the temporary opening is closed. The negative mass flow value is shown in FIG. 9B. The reason is that after the air is introduced from the outside of the engine 1 to the i-th channel 71, when a positive pressure is generated in the exhaust passage 7 which is further upstream than the diverging portion 43 (for example, reference numeral 95 in Fig. 9A), the first passage The air in the 71 is extruded. The reed valve 74 prevents the gas from flowing from the second passage 7 toward the outside of the engine casing, so that the air in the first passage 71 is extruded to the second passage 72. Fig. 9C Indicates the rotation angle (crank angle) of the crankshaft 16 and the exhaust passage 7 A diagram showing an example of the relationship between the amount of oxygen (oxygen concentration) in each portion of the secondary air supply device 7G. Specifically, the curve 96a indicates the connection portion 72a and the exhaust passage of the second passage 72 in the second passage 71. The oxygen concentration between 7 (for example, the measurement point 154997.doc -25·201239190 a shown in Fig. 又). Further, the curve 96b indicates the vicinity of the intermediate portion of the second passage 72 (between the upstream end 72a and the downstream end 72b. For example. The oxygen concentration at the measurement point b) shown in Fig. 1. Further, the curve 96c indicates a portion of the exhaust passage 7 which is further downstream than the i-th catalyst 21 (between the i-th and second catalysts 21, 22). For example, the oxygen concentration at the point of measurement is shown in Figure (10). Further, the curve 96d indicates the oxygen concentration in the exhaust passage 7 upstream of the i-th passage connecting portion 7 (for example, the measuring point d shown in Fig. 1). When the curves 96a, 96c, and 96d are compared, it is found that the oxygen concentration in the second channel is higher than the oxygen concentration in the exhaust passage 7. This indicates that the secondary air of the engine is introduced into the first passage 71. If the curves 96b, 96c, and 96 are compared, it is known that the oxygen concentration in the second channel 72 is higher than the oxygen concentration in the exhaust channel 7. If the curve 96 &amp; The oxygen concentration in the second passage 72 is higher than the oxygen concentration in the first passage 71 (close to the exhaust passage 7). Therefore, it is known that the secondary air outside the engine i is guided to the second passage 72. When air is introduced into the second passage 72, the secondary air is supplied between the second and second catalysts 2, and thus the secondary air supply is achieved. According to the comparison of the curves 96c and 96d, The exhaust passage 7 between the first and second catalysts 2b (for example, the oxygen concentration of the measurement point shown in FIG. i, the first passage connecting portion 71b is upstream of the exhaust passage 7 (for example, (5) The lower oxygen concentration of the measurement point d) indicates that the secondary air is directed to the exhaust passage 7 further downstream than the i-th catalyst 21. Generally, the oxygen concentration (e.g., the defect b) of the second passage (four) is high. The oxygen concentration of the exhaust passage 7 (for example, the measurement point d) upstream of the i-th channel connecting portion claw is considered to be (four) for introducing the secondary air into the second passage. When this is confirmed, the purpose of supplying secondary air to the exhaust passage 7 between the first worker and the second catalysts 21 and 22 can be achieved. J54997.doc -26· 201239190 Reference numeral 97 in the curve 96c of Fig. 9C It is shown that the oxygen concentration increases substantially synchronously with the timing at which a positive pressure (which generates a positive pressure upstream of the diverging portion 43) as indicated by reference numeral 95 in Fig. 9. This indicates that the secondary air introduced into the second channel 71 passes through The second passage 72 feeds the exhaust passage 7 between the first and second catalysts 21 and 22. As described above, according to the present embodiment, a dedicated device for forcibly feeding air to the exhaust passage 7 is not used. A sufficient amount of secondary air can be supplied to a portion of the exhaust passage 7 that is further downstream than the second catalyst 21. That is, secondary air is introduced from the outside using a negative pressure generated by utilizing exhaust gas energy, and the exhaust gas is used in the same manner. The positive pressure generated by the energy sends the introduced secondary air to the downstream of the ith catalyst 2. Thus, the pumping action is realized by using the exhaust gas energy, thereby reducing the loss of the engine output. Moreover, it can be upstream of the diverging portion 43. The exhaust passage 7 generates a large negative pressure, thus The amplitude of the exhaust pulsation can be increased. Therefore, even when the engine is operated at a south speed or a load state, a large negative pressure accompanying the shock wave and a sufficient positive pressure due to the exhaust pulsation can be utilized. The secondary air is supplied to the downstream exhaust passage 7 of the first catalyst 21. Further, other pump means for supplying air may be used in combination. Even in this case, the load applied to the pump can be reduced, thereby The loss of the engine output is reduced. In this embodiment, the energy loss of the gas flowing through the machine path 61 from the upstream end 71a to the downstream end 7 lb of the first passage 71 is smaller than the flow through the downstream end 72b of the second passage. The gas of the flow path 62 of the downstream end 71b of the channel 71 is deducted. That is, the flow coefficient of the first passage downstream end 71b when the second passage 72 is closed and flows from the upstream end 7ia of the i-th passage through the 154997.doc -27·201239190 air is larger than the upstream of the connection portion of the second passage 72. The flow coefficient of the first passage downstream end 71b of the first passage 71 while flowing air through the second passage downstream end 72b. Therefore, when a negative pressure is generated further upstream than the gradually expanding portion 43, the air in the second passage 72 does not flow backward, and the secondary air can be surely introduced to the first through the reed valve 74 of the first passage 71. Therefore, when the exhaust passage 7 upstream of the diverging portion 43 becomes a positive pressure, the introduced secondary air can be sent to the second passage 72°. In this embodiment, the exhaust device The fifth and second catalysts 2, 22 are disposed in the exhaust passages 7 upstream and downstream of the downstream end 72b of the second passage 72, respectively. According to this configuration, the oxygen concentration of the exhaust gas supplied to the second catalyst 22 can be increased. Therefore, the second catalyst 21 can be mainly used as a reduction catalyst, and the second catalyst 22 can mainly function as an oxidation catalyst. When the third catalyst 21 and the second catalyst 22 are applied to the three-way catalyst, it is necessary to introduce the theoretical air-fuel ratio exhaust gas to the catalysts in order to perform both the reduction reaction and the oxidation reaction. When the second catalyst 21 is mainly used as a reduction catalyst, the fuel-rich exhaust gas may be introduced into the i-th catalyst 21. Further, when the second catalyst 22 functions as an oxidation catalyst, the exhaust gas which tends to have a lower air-fuel ratio can be introduced into the second catalyst 22. Thereby, the second catalyst 21 and the second catalyst 22 cooperate to perform both the reduction reaction and the oxidation reaction, so that harmful components in the exhaust gas can be efficiently removed. Thereby, the exhaust gas of the stoichiometric air-fuel ratio is introduced into the first catalyst 21, so that the range of the air-fuel ratio at which the harmful components can be removed can be expanded. Therefore, it is not necessary to strictly control the empty ratio. •28- 154997.doc

201239190 另一方面’若將接近於理論空燃比之空燃比之混合氣供 給至燃燒室’則可抑制消耗燃料量。若應用理論空燃比左 右之空燃比’則廢氣成為高溫,從而存在該高溫廢氣引起 觸媒21、22嫁結之虞。但該實施形態中,於漸擴部μ生成 之新的衝擊波35b使其後方產生較大之負壓。因該負壓而 產生廢氣之絕熱膨脹’由此,可藉由絕熱冷卻效果而使廢 氣冷卻。即’廢氣於到達第1觸媒21之前被冷卻。因此, 可藉由使用接近於理論空燃比之空燃比之混合氣而抑制燃 料消耗量’並且可同時保護觸媒21、22,且實現有害成分 之無毒化。當然,即便於引擎1為高負載狀態或以高速度 運行之狀態下,亦可使廢氣為低壓及低溫,從而可保護觸 媒 21、22。 &lt;第2實施形態&gt; 圖10係表示本發明之第2實施形態之引擎之排氣通道等 之構成之剖面圖。圖10中,對上述圖丨所示之各部分之對 應部分附上相同參照符號。 與第1貫施形態相同’該第2實施形態之引擎1包括:氣 缸體3;設置於該氣缸體3之一端之氣缸蓋4;及於氣缸體3 内往返運動之活塞5 ;該些部分形成燃燒室1〇。於氣缸蓋4 設置有:對進氣口 8a進行開閉之進氣閥8 ;對排氣口 9&amp;進 行開閉之排氣閥9 ;以及用以驅動進氣閥8及排氣閥9之氣 門裝置。引擎1進而包括:排氣裝置5〇 ;及向排氣裝置5〇 之排氣通道7供給空氣之二次空氣供給裝置70。 排氣裝置50包括:連接於氣缸蓋4之第丨排氣管51 ;連接 J54997.doc -29- 201239190 於該第1排氣管51之第2排氣管52 ;及連接於該第2排氣管 52之第3排氣管53 ;且該些排氣管51、52、53形成排氣通 道7。於排氣通道7中隔開間隔而配置有第1觸媒21及第2觸 媒22。於第1排氣管51之上游部設置有分支管3〇β於分支 管30與第1觸媒21之間設置有漸縮-漸擴喷嘴4〇。 二次空氣供給裝置70包括:簧片閥74 ;第1二次空氣供 給管76;及連接於第1二次空氣供給管76之第2二次空氣供 給管77。第1二次空氣供給管76形成自簣片閥74至排氣通 道7之第1通道71。第2二次空氣供給管77形成自第1通道71 至第1及第2觸媒21、22之間之排氣通道7之第2通道72。 該實施形態中’進而於第2通道72設置有第2簧片閥 80(止回閥)。簧片閥80以使自第2通道71之上游端72a朝向 下游端72b之方向之氣流通過而阻止其相反方向之氣流的 方式構成。此以外之構成與第1實施形態相同。因此,第2 實施形態之詳細說明可由第1實施形態所相關之圖丨〜圖9及 其§羊細說明來代替。 當於較漸擴部43更為上游之排氣通道7内產生負壓時, 第1通道71之簧片閥74打開,外部空氣導入至第1通道71。 此時,第2通道72之簧片閥80成為閉合狀態,自第2通道72 之下游端72b向上游端72a之空氣流被阻止。另一方面,當 於較漸擴部43更為上游之排氣通道7内產生正壓時,第1通 道71之簧片閥74成為閉合狀態,第2通道72之簧片閥8〇打 開。由此’導入至第i通道71之二次空氣通過第2通道72而 送入至第1觸媒21下游之排氣通道7。從而,借助利用排氣 154997.doc -30- 201239190 通道7内產生之負壓及正壓之泵作用,而可將二次空氣供 給至第1觸媒21下游之排氣通道7。而且,可藉由配置於第 2通道72之簧片閥80而確實地抑制第2通道72中之空氣之逆 流,從而可有效率地供給二次空氣。 如此,根據該實施形態,第2通道72中之空氣之流動被 限制於自其上游端朝向下游端之方向◊即,可防止二次空 氣之逆流。由此,當於漸擴部43之上游產生負壓時,可自 第1通道71之上游端確實地導入二次空氣,且,當於漸擴 部43之上游產生正壓時,可將二次空氣確實地供給至第ι 及第2觸媒21、22 » &lt;第3實施形態&gt; 圖11係表示本發明之第3實施形態之引擎之排氣通道等 之構成之剖面圖。圖11中,對上述圖!所示之各部分之對 應部分附上相同參照符號。 與第1實施形態相同,該第3實施形態之引擎丨包括:氣 之氣缸蓋4;及於氣缸體3 缸體3 ;設置於該氣紅體3之一端 内往返運動之活塞5(參照圖1);且該些部分形成燃燒室 10。於氣缸蓋4設置有:對進氣口 8a進行開閉之進氣閥8 ; 對排氣口 9a進行開閉之排氣閥9;以及用以驅動進氣閥8及 排氣閥9之氣門裝置。引擎!進而包括:排氣裝置5〇;及向 排氣裝置50之排氣通道7供給空氣之二次空氣供給裝置 70 = 排氣裝置50包括··連接於氣紅蓋4之第i排氣管51 ;連接 於該第1排氣管51之第2排氣管52 ;及連接於該第2排氣管 I54997.doc •31 · 201239190 52之第3排氣管53,該些排氣管51 ' 52、53形成排氣通道 7。於排氣通道7隔開間隔而配置有第1觸媒21及第2觸媒 22。於第1排氣管5 1之上游部設置有分支管3〇。於分支管 3 0與第1觸媒21之間設置有漸縮-漸擴噴嘴4〇。 該第3實施形態中,分支管30兼作形成第1通道71之第1 二次空氣供給管76。即,廢棄專用之第1通道71而使分支 部31兼作第1通道71。亦可說成第1通道71兼作分支部31。 而且,第2二次空氣供給管77連接於兼作第丨二次空氣供給 官76之分支管30,而形成自分支部31(第i通道7丨)至第【及 第2觸媒21、22之間之排氣通道7的第2通道72。此以外之 構成與第1實施形態相同。因此,第3實施形態之詳細說明 可由第1實施形態所相關之圖丨〜圖9及其詳細說明來代替。 該第3實施形態中,簧片閥74結合於分支管3〇之與排氣 通道7為相反側之端部,進而,空氣量控制閥乃及空氣濾 清器78結合於其上游側。簧片閥74構成分支部31之反射部 31b。即,來自排氣通道7之衝擊波向分支部(第1通道7上) 为支,並於閉合狀態之簧片閥74(反射部31b)反射後再次通 過分支部3丨(第丨通道71)返回至排氣通道7。該衝擊波與在 排氣通道7内滯後行進之廢氣衝撞而提高廢氣之壓力。 於排氣閥9打開時簧片閥74閉合,可藉由簧片閥74而反 射衝擊波。當藉由漸縮_漸擴喷嘴4〇之作用而於排氣通道7 產生負壓時’簧片閥74打開,從而可向第1通道71供給來 自外邛之一-人空氣。其後’當藉由排氣脈動而於排氣通道 7產生正壓時,導入至第丨通道7ι之二次空氣經由第2通道 154997.doc •32- 201239190 72而供給至第1及第2觸媒21、22之間之排氣通道7。從 而,本實施形態中,亦可向第丨觸媒21下游之排氣通道7供 給足量之空氣。 ” 又,根據本實施形態,無需專門作為分支部31發揮功能 之通道或專門作為第1通道71發揮功能之通道。因此,與 使用專用之分支部3 1及專用之第丨通道7丨之構成(例如第j 實施形態)相比,可實現成本降低。 &lt;第4實施形態&gt; 圖12係用以說明本發明之第4實施形態之引擎之排氣裝 置等之構成之剖面圖。圖12中,對與上述圖u所示之各部 分之對應部分附上相同參照符號。 與第3實施形態相同’該第4實施形態之引擎1包括·氣 缸體3,設置於該氣缸體3之—端之氣缸蓋4;及於氣缸體3 内往返運動之活塞5(參照圖”;且該些部分形成燃燒室 10 °於吼紅蓋4設置有:對進氣口 8a進行開閉之進氣間8 ; 對排氣口 9a進行開閉之排氣閥9;以及用以驅動進氣閥8及 排氣閱9之氣門裝置。引擎1進而包括:排氣裝置5〇;及向 排氣裝置50之排氣通道7供給空氣之二次空氣供 70。 排氣裝置5 〇句括.·;鱼μ尸t # 括·連接於氧缸蓋4之第1排氣管51 ;連接 於該m氣管51之第2排氣管52;及連接於該第2排氣管 、首7。、K S 53,且該些排氣管51、52、53形成排氣通 ^於排乳通道7隔開間隔而設置有第1觸媒21及第2觸媒 °於第1排氣管51之上游部設置有分支管3〇。 154997.doc •33· 201239190 分支管30兼作形成第1通道71之第1二次空氣供給管76。 第2二次空氣供給管77連接於兼作第1二次空氣供給管76之 分支管30,而形成自分支部31(第1通道71)至第1及第2觸媒 21、22之間之排氣通道7之第2通道72。 該第4實施形態中,分支管30用作漸縮·漸擴喷嘴之一部 分。其他構成與第3實施形態(參照圖11)相同。因此,第4 實施形態之詳細說明可由第1實施形態之圖1〜圖9及第3實 施形態之圖11及該些之詳細說明來代替。 第1〜第3實施形態中,漸縮部41、喉部42及漸擴部43形 成於較分支部31更為下游之排氣通道7。然而,本案發明 者繼續進行積極研究之結果而想到更簡單構造且可獲得相 同效果之構造。 本實施形態中,為產生作為新的衝擊波之行進衝擊波 35b,而設置使排氣衝程初期產生之衝擊波35反射並再次 向排氣通道7傳播之分支部31。若以不同之視點看該分支 部,則排氣通道7於分支部31之位置其流路剖面積增 大。而且,於較該位置更為下游流路剖面積變小。換言 之’藉由分支部3 1而形成漸縮部4丨與喉部42。 ”” 心砰軋通道7之流路 相積Α5與較分支部人咖更為下游之排氣通道7之产路 剖面積Α7大致相等之情形時,/ 八士如 又见即’位於較 刀 人口 31&amp;更為上游之排氣通道7之部分之气 Α5、與分# + 刀之流路剖面積 、刀支口P 31之流路剖面積A4相加而得之产 積,大於位於輕入σ 2s * . 力&lt;·路口丨J面 於較入口川更為下游之排氣通道7之部分之流 154997.doc -34· 201239190 路剖面積A7。A4+A5&gt;A7。因此,可視作於入口 3ι&amp;下游 形成有漸縮部41與喉部42。由此,僅於入口 31&amp;下游設置 漸擴部43實質上便可形成漸縮_漸擴噴嘴4〇〇八6表示漸擴 部43之流路剖面積,且Α7&lt;Α6β入口 31&amp;與漸擴部u之間 之部分成為喉部42。如此,喉部42亦可沿著流路方向而較 長地延伸。漸縮部4丨及漸擴部43無需為朝向下游而使流路 剖面積平滑地(連續地)變化之構成’亦可以使流路剖:積 呈階段性(Step by Step)地變化之方式構成。 該第4實施形態之構成亦可應用於上述第丨及第2實施形 態之構成。該情形時,於第1通道71之連接部71b之下游設 置漸擴部43,藉此實質上可形成漸縮_漸擴喷嘴扣。於該 構成之情形時,不僅於分支部3〗,亦於向第丨通道Η之分201239190 On the other hand, if the mixture of air-fuel ratio close to the theoretical air-fuel ratio is supplied to the combustion chamber, the amount of fuel consumed can be suppressed. If the air-fuel ratio of the theoretical air-fuel ratio is applied, the exhaust gas becomes a high temperature, so that the high-temperature exhaust gas causes the catalysts 21, 22 to marry. However, in this embodiment, the new shock wave 35b generated in the diverging portion μ generates a large negative pressure behind it. The adiabatic expansion of the exhaust gas is caused by the negative pressure. Thus, the exhaust gas can be cooled by the adiabatic cooling effect. That is, the exhaust gas is cooled before reaching the first catalyst 21. Therefore, the fuel consumption amount can be suppressed by using the air-fuel ratio close to the air-fuel ratio of the stoichiometric air-fuel ratio, and the catalysts 21, 22 can be simultaneously protected, and the poisoning of the harmful components can be achieved. Of course, even when the engine 1 is in a high load state or at a high speed, the exhaust gas can be made low pressure and low temperature, thereby protecting the catalysts 21, 22. &lt;Second Embodiment&gt; Fig. 10 is a cross-sectional view showing the configuration of an exhaust passage or the like of an engine according to a second embodiment of the present invention. In Fig. 10, the same reference numerals are attached to the corresponding portions of the respective portions shown in the above drawings. The engine 1 of the second embodiment includes a cylinder block 3, a cylinder head 4 provided at one end of the cylinder block 3, and a piston 5 that reciprocates in the cylinder block 3; the portions A combustion chamber 1〇 is formed. The cylinder head 4 is provided with an intake valve 8 that opens and closes the intake port 8a, an exhaust valve 9 that opens and closes the exhaust port 9&amp; and a valve device for driving the intake valve 8 and the exhaust valve 9. . The engine 1 further includes: an exhaust device 5; and a secondary air supply device 70 that supplies air to the exhaust passage 7 of the exhaust device 5A. The exhaust device 50 includes: a second exhaust pipe 51 connected to the cylinder head 4; a second exhaust pipe 52 connected to the first exhaust pipe 51 by J54997.doc -29-201239190; and connected to the second row The third exhaust pipe 53 of the air pipe 52; and the exhaust pipes 51, 52, 53 form an exhaust passage 7. The first catalyst 21 and the second catalyst 22 are disposed at intervals in the exhaust passage 7. A branch pipe 3〇β is provided in the upstream portion of the first exhaust pipe 51, and a tapered-divergent nozzle 4〇 is provided between the branch pipe 30 and the first catalyst 21. The secondary air supply device 70 includes a reed valve 74, a first secondary air supply pipe 76, and a second secondary air supply pipe 77 connected to the first secondary air supply pipe 76. The first secondary air supply pipe 76 forms a first passage 71 from the raft valve 74 to the exhaust passage 7. The second secondary air supply pipe 77 forms a second passage 72 from the first passage 71 to the exhaust passage 7 between the first and second catalysts 21 and 22. In this embodiment, the second reed valve 80 (check valve) is further provided in the second passage 72. The reed valve 80 is constructed such that the airflow from the upstream end 72a of the second passage 71 toward the downstream end 72b passes through the airflow in the opposite direction. The configuration other than this is the same as that of the first embodiment. Therefore, the detailed description of the second embodiment can be replaced by the drawings of Fig. 9 and Fig. 9 relating to the first embodiment. When a negative pressure is generated in the exhaust passage 7 which is further upstream than the gradually expanding portion 43, the reed valve 74 of the first passage 71 is opened, and the outside air is introduced into the first passage 71. At this time, the reed valve 80 of the second passage 72 is closed, and the air flow from the downstream end 72b of the second passage 72 to the upstream end 72a is blocked. On the other hand, when a positive pressure is generated in the exhaust passage 7 which is further upstream than the gradually expanding portion 43, the reed valve 74 of the first passage 71 is closed, and the reed valve 8 of the second passage 72 is opened. Thus, the secondary air introduced into the i-th channel 71 passes through the second passage 72 and is sent to the exhaust passage 7 downstream of the first catalyst 21. Thus, the secondary air can be supplied to the exhaust passage 7 downstream of the first catalyst 21 by the action of the negative pressure and the positive pressure generated in the passage 7 of the exhaust gas 154997.doc -30- 201239190. Further, the reed valve 80 disposed in the second passage 72 can reliably suppress the reverse flow of the air in the second passage 72, so that the secondary air can be efficiently supplied. As described above, according to this embodiment, the flow of the air in the second passage 72 is restricted from the upstream end toward the downstream end, that is, the reverse flow of the secondary air can be prevented. Therefore, when a negative pressure is generated upstream of the diverging portion 43, secondary air can be surely introduced from the upstream end of the first passage 71, and when a positive pressure is generated upstream of the diverging portion 43, The second air is supplied to the first and second catalysts 21 and 22. &lt;Third Embodiment&gt; FIG. 11 is a cross-sectional view showing the configuration of an exhaust passage or the like of the engine according to the third embodiment of the present invention. In Figure 11, the above figure! Corresponding parts of the various parts shown are denoted by the same reference numerals. Similarly to the first embodiment, the engine casing according to the third embodiment includes a cylinder head 4 for gas, a cylinder 3 for the cylinder block 3, and a piston 5 provided to reciprocate in one end of the gas red body 3 (refer to the figure). 1); and the portions form the combustion chamber 10. The cylinder head 4 is provided with an intake valve 8 that opens and closes the intake port 8a, an exhaust valve 9 that opens and closes the exhaust port 9a, and a valve device that drives the intake valve 8 and the exhaust valve 9. The engine further includes: an exhaust device 5; and a secondary air supply device 70 that supplies air to the exhaust passage 7 of the exhaust device 50. The exhaust device 50 includes an i-th exhaust connected to the gas red cover 4. a tube 51; a second exhaust pipe 52 connected to the first exhaust pipe 51; and a third exhaust pipe 53 connected to the second exhaust pipe I54997.doc • 31 · 201239190 52, the exhaust pipes 51 '52, 53 form an exhaust passage 7. The first catalyst 21 and the second catalyst 22 are disposed at intervals in the exhaust passage 7. A branch pipe 3 is provided in an upstream portion of the first exhaust pipe 51. A tapered-divergent nozzle 4 is provided between the branch pipe 30 and the first catalyst 21. In the third embodiment, the branch pipe 30 also serves as the first secondary air supply pipe 76 that forms the first passage 71. In other words, the dedicated first passage 71 is discarded, and the branch portion 31 also serves as the first passage 71. It can also be said that the first passage 71 also serves as the branch portion 31. Further, the second secondary air supply pipe 77 is connected to the branch pipe 30 which also serves as the second secondary air supply officer 76, and is formed from the branching portion 31 (i-th passage 7A) to the second and second catalysts 21 and 22. The second passage 72 of the exhaust passage 7 between. The configuration other than this is the same as that of the first embodiment. Therefore, the detailed description of the third embodiment can be replaced by the drawings 9 to 9 and the detailed description thereof in the first embodiment. In the third embodiment, the reed valve 74 is coupled to the end portion of the branch pipe 3 opposite to the exhaust passage 7, and the air amount control valve and the air cleaner 78 are coupled to the upstream side. The reed valve 74 constitutes the reflecting portion 31b of the branch portion 31. That is, the shock wave from the exhaust passage 7 is branched toward the branch portion (on the first passage 7), and is reflected by the reed valve 74 (reflecting portion 31b) in the closed state, and then passes through the branch portion 3 (the second passage 71) again. Return to the exhaust passage 7. The shock wave collides with the exhaust gas traveling in the exhaust passage 7 to increase the pressure of the exhaust gas. When the exhaust valve 9 is opened, the reed valve 74 is closed, and the shock wave can be reflected by the reed valve 74. When the negative pressure is generated in the exhaust passage 7 by the action of the tapered_swelling nozzle 4, the reed valve 74 is opened, so that one of the outer ones and the human air can be supplied to the first passage 71. Thereafter, when a positive pressure is generated in the exhaust passage 7 by the exhaust pulsation, the secondary air introduced into the second passage 7 is supplied to the first and second via the second passage 154997.doc •32-201239190 72. The exhaust passage 7 between the catalysts 21, 22. Therefore, in the present embodiment, a sufficient amount of air can be supplied to the exhaust passage 7 downstream of the second catalyst 21. Further, according to the present embodiment, there is no need for a passage that functions exclusively as the branch portion 31 or a passage that functions exclusively as the first passage 71. Therefore, the use of the dedicated branch portion 31 and the dedicated third passage 7丨(Fourth Embodiment) The present invention is a cross-sectional view showing the configuration of an exhaust device and the like of the engine according to the fourth embodiment of the present invention. In the same manner as in the third embodiment, the engine 1 of the fourth embodiment includes the cylinder block 3 and is disposed in the cylinder block 3. a cylinder head 4 at the end; and a piston 5 (refer to the figure) that reciprocates in the cylinder block 3; and the portions form a combustion chamber 10°. The crimson cover 4 is provided with an air inlet for opening and closing the air inlet 8a. An exhaust valve 9 that opens and closes the exhaust port 9a; and a valve device for driving the intake valve 8 and the exhaust valve 9. The engine 1 further includes: an exhaust device 5; and an exhaust device 50 The exhaust passage 7 supplies air to the secondary air supply 70. 5 〇 括 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 The tube, the first block SB, and the KS 53, and the exhaust pipes 51, 52, and 53 form the exhaust gas passage, and the first catalyst 21 and the second catalyst are disposed at intervals along the drain passage 7 The branch pipe 3 is provided in the upstream portion of the exhaust pipe 51. 154997.doc • 33· 201239190 The branch pipe 30 also serves as the first secondary air supply pipe 76 forming the first passage 71. The second secondary air supply pipe 77 is connected to The branch pipe 30 of the first secondary air supply pipe 76 is also formed, and the second passage 72 of the exhaust passage 7 from the branch portion 31 (first passage 71) to between the first and second catalysts 21 and 22 is formed. In the fourth embodiment, the branch pipe 30 is used as one of the tapered and divergent nozzles. The other configuration is the same as that of the third embodiment (see Fig. 11). Therefore, the detailed description of the fourth embodiment can be made by the first embodiment. 1 to 9 and FIG. 11 of the third embodiment and the detailed descriptions thereof are used instead. In the first to third embodiments, the tapered portion 41, the throat portion 42, and the diverging portion 43 are formed in the branch portion 31. for The inventor of the present invention continues to carry out the results of active research and conceives a structure that is simpler in construction and can obtain the same effect. In the present embodiment, in order to generate the traveling shock wave 35b as a new shock wave, the inventor is provided. The branching portion 31 which is reflected by the shock wave 35 generated at the beginning of the exhaust stroke and propagates again to the exhaust passage 7. When the branch portion is viewed from a different viewpoint, the flow passage sectional area of the exhaust passage 7 at the position of the branch portion 31 is increased. Further, the cross-sectional area of the downstream flow path becomes smaller at this position. In other words, the tapered portion 4 and the throat portion 42 are formed by the branch portion 31. ” ” 砰 砰 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰 砰The population 31 & more upstream of the exhaust passage 7 part of the gas 5, and the subsection # + knife flow path sectional area, the knife branch P 31 flow path sectional area A4 added to the production, greater than the light Into the σ 2s * . Force &lt; · intersection 丨 J face in the downstream of the inlet channel downstream of the exhaust channel 7 part of the flow 154997.doc -34 · 201239190 road sectional area A7. A4+A5&gt;A7. Therefore, it is considered that the tapered portion 41 and the throat portion 42 are formed downstream of the inlet 3i & Thus, the diverging portion 43 can be formed only in the downstream of the inlet 31 & the tapered progressively expanding nozzle 4 〇〇 8 6 represents the cross-sectional area of the flow path of the diverging portion 43, and Α 7 &lt; Α 6β inlet 31 &amp; The portion between the expanded portions u becomes the throat portion 42. Thus, the throat 42 can also extend longer along the flow path direction. The tapered portion 4 and the diverging portion 43 need not have a configuration in which the cross-sectional area of the flow path is changed smoothly (continuously) toward the downstream, and the flow path can be formed in a stepwise manner. Composition. The configuration of the fourth embodiment can also be applied to the configurations of the above-described second and second embodiments. In this case, the diverging portion 43 is provided downstream of the connecting portion 71b of the first passage 71, whereby the tapered-swelling nozzle clasp can be substantially formed. In the case of this configuration, not only the branch portion 3 but also the third channel

支部產生流路剖面積之變化’因此亦可考慮於第〗通道I 接部71b下游之排氣通道7形成漸縮部41及喉部42。該情形 時,連接部71b與漸擴部43之間之排氣通道7之部分成為喉 部 42 » 、 &lt;第5實施形態&gt; 圖13係用以說明本發明之第5實施形態之引擎之排氣裝 置等之構成之剖面圖。該圖13中,對與上述圖㈣示之各 部分對應之部分附上相同參照符號並省略說明。 該貫施形態申,於排氣通道7申在漸縮_漸擴喷嘴4〇之下 游设.置有一觸媒23 ^第2通道72之下游端72b結合於觸媒23 之側面。即,於第2通道72之下游端72b形成有使觸媒幻之 大致整個側面敞開之筒狀之空氣導入空間8丨。另一方面, I54997.doc -35- 201239190 於觸媒23之側面形成有多個向内部導入空氣之空氣導入孔 82 ° 自第1通道71供給至第2通道72之二次空氣,自空氣導入 空間81進入至觸媒23内部。進入至觸媒23内部之二次空氣 一面與自觸媒23之上游端23a導入之廢氣混合,一面流向 觸媒23之下游端。由此’於觸媒23内部,自觸媒23之上游 端23a朝向下游變得尖細之錐形狀的區域24A成為來自燃燒 室1 0之排氣佔支配地位之低氧濃度區域。而且,除區域24 以外之剩餘之區域24B成為充足地供給有二次空氣之高氧 濃度區域。觸媒23於低氧濃度區域24A中作為還原觸媒發 揮功能,而於高氧濃度區域24B中作為氧化觸媒發揮功 能。從而,可使一種觸媒23兼作還原觸媒及氧化觸媒,因 而可充分地使來自燃燒室10之排氣無毒化。因此,可提高 廢棄之淨化效率。又,因一種觸媒23便足夠,故而可減小 排氣裝置50整體之熱容。由此,當引擎丨啟動時,可使觸 媒23迅速活化,從而可於引擎剛啟動後便充分淨化廢氣。 6玄實施形態之又一特徵在於,於自第1通道71與第2通道 72之連接部至第丨通道”之下游端7ib之範圍之中途配置有 (節机孔)83 »由此’可阻止來自燃燒室i 〇之廢氣進入 至第1通道71而又不會對二次空氣之供給產生影響。由 此’可提高供給至第2通道72之线之氧濃度。孔口仏亦 可為例如中央具有開口之板狀體。 於上述或後述之其他實施形態中,相同之孔口亦可設置 154997.doc -36· 201239190 圖14係用以說明觸媒23之構成例之圖解性之立體圖。觸 媒23具有蜂寫狀之金屬載體85。金屬載體85係將開孔之平 坦泊片(羯材)86與開孔之波形箔片(箔材)87交替積層而形 成蜂窩構造。更具體而言,使帶狀之平坦箔片86與帶狀之 皮片87重疊並捲成輥狀’由此形成包含圓柱狀之蜂窩 構造之金屬載體85。平坦箔片86係使多個空氣孔86a均等 分散形成於平坦的金屬箔上製作而成。波形箔片87係使例 如多個空氣孔87a均等分散形成於形成為條狀波形之金屬 羯上製作而成。於觸媒23之最外周面配置有平坦箔片86, 於最外周面露出之空氣孔86a相當於上述空氣導入孔82。 &lt;第6實施形態&gt; 圖15係用以說明本發明之第6實施形態之引擎之排氣裝 置等之構成之剖面圖。該圖15中,對與上述圊13所示之各 部分對應之部分附上相同參照符號並省略說明。 該實施形態中,第2通道72之下游端72b連接於觸媒23之 側面與觸媒23之上游端23a之外周區域》即,於第2通道72 之下游端72b形成有使觸媒23之大致整個側面敞開並且使 觸媒23之上游端23a之外周部敞開之筒狀的空氣導入空間 88。觸媒23之構成為如上所述。 自第1通道71供給至第2通道72之二次空氣,自空氣導入 空間88例如至觸媒23内部。即,自觸媒23之側面與觸媒23 之上游端23a之外周區域進入至觸媒23内部。進入至觸媒 23内部之二次空氣,一面與自觸媒23之上游端23a之中央 區域導入之廢氣混合,一面流向觸媒23之下游端。由此, 154997.doc •37- 201239190 於觸媒23内部,自觸媒23之上游端23a之中央區域朝向下 游變得尖細之錐形狀的區域24A成為來自燃燒室1〇之廢氣 佔支配地位之低氧濃度區域。而且,除區域24以外之剩餘 之區域24B成為充足供給有二次空氣之高氧濃度區域。觸 媒23於低氧濃度區域24A中作為還原觸媒發揮功能,而於 高氧濃度區域24B中作為氧化觸媒發揮功能。從而,可使 一種觸媒23兼作還原觸媒及氧化觸媒。亦自觸媒23之上游 端23a之外周區域導入二次空氣,因此與第$實施形態之情 形相比’低氧濃度區域24變小》即,與第5實施形態之情 形相比,尚氧濃度區域2 5變大。因此,可對觸媒2 3供給足 量之二次空氣,因此可充分地使來自燃燒室1〇之廢氣無毒 化。 &lt;第7實施形態&gt; 圖16係表示本發明之第7實施形態之引擎之排氣裝置之 構成之模式圖。圖16中,對上述圖1所示之各部分之對應 部分附上相同參照符號。第5實施形態係將本發明之一實 施形態應用於多氣缸引擎之例。 該第7實施形態之引擎1包括複數個氣缸#八、#Ββ各氣 缸#八、#B包括:氣缸體3(參照圖丨);設置於該氣缸體^之 一端之氣缸蓋4 ;及於氣缸體3内往返運動之活塞5(參照圖 1) ’且該些部分形成燃燒室1〇。於氣缸蓋4設置有:對進 氣口 8a進行開閉(參照圖1}之進氣閥8(參照圖1};對排氣口 %進行開閉之排氣閥9 ;以及用以驅動進氣閥8(參照圖丨)及 排氣閥9之氣門裝置。引擎1進而包括:排氣裝置5 〇 ;及向 154997.docThe branch portion produces a change in the cross-sectional area of the flow path. Therefore, it is also possible to form the tapered portion 41 and the throat portion 42 in consideration of the exhaust passage 7 downstream of the first passage I-joining portion 71b. In this case, the portion of the exhaust passage 7 between the connecting portion 71b and the diverging portion 43 is the throat portion 42 » &lt;Fifth Embodiment&gt; FIG. 13 is an engine for explaining the fifth embodiment of the present invention. A cross-sectional view of the structure of the exhaust device or the like. In the drawings, the same reference numerals will be given to the portions corresponding to the respective portions shown in the above (4), and the description thereof will be omitted. The embodiment is applied to the exhaust passage 7 under the tapered _ diverging nozzle 4 游. The catalyst 23 is disposed. The downstream end 72b of the second passage 72 is coupled to the side of the catalyst 23. In other words, a cylindrical air introduction space 8 is formed in the downstream end 72b of the second passage 72 so as to open substantially the entire side surface of the catalyst. On the other hand, I54997.doc -35-201239190 is formed on the side surface of the catalyst 23, and a plurality of air introduction holes 82 are introduced into the air, and the secondary air supplied from the first passage 71 to the second passage 72 is introduced from the air. The space 81 enters the inside of the catalyst 23. The secondary air that has entered the inside of the catalyst 23 is mixed with the exhaust gas introduced from the upstream end 23a of the catalyst 23, and flows to the downstream end of the catalyst 23. Thus, in the inside of the catalyst 23, the tapered region 24A which is tapered toward the downstream from the upstream end 23a of the catalyst 23 becomes a low oxygen concentration region which is dominated by the exhaust gas from the combustion chamber 10. Further, the remaining region 24B other than the region 24 is a region of high oxygen concentration in which secondary air is sufficiently supplied. The catalyst 23 functions as a reduction catalyst in the low oxygen concentration region 24A, and functions as an oxidation catalyst in the high oxygen concentration region 24B. Therefore, one type of catalyst 23 can also serve as a reduction catalyst and an oxidation catalyst, so that the exhaust gas from the combustion chamber 10 can be sufficiently poisoned. Therefore, the purification efficiency of waste can be improved. Further, since one type of catalyst 23 is sufficient, the heat capacity of the entire exhaust unit 50 can be reduced. Thereby, when the engine is started, the catalyst 23 can be quickly activated, so that the exhaust gas can be sufficiently purified immediately after the engine is started. According to still another aspect of the present invention, in the range from the connection portion of the first passage 71 and the second passage 72 to the downstream end 7ib of the second passage 72, (the orifice) 83 is provided. The exhaust gas from the combustion chamber i is prevented from entering the first passage 71 without affecting the supply of the secondary air. Thus, the oxygen concentration of the line supplied to the second passage 72 can be increased. For example, in the other embodiments described above or described later, the same orifices may be provided with 154997.doc -36·201239190. FIG. 14 is a schematic perspective view for explaining a configuration example of the catalyst 23. The catalyst 23 has a bee-shaped metal carrier 85. The metal carrier 85 is formed by alternately laminating a flat plate (cavity) 86 having an opening and a corrugated foil (foil) 87 having an opening to form a honeycomb structure. In other words, the strip-shaped flat foil 86 is overlapped with the strip-shaped leather sheet 87 and wound into a roll shape. Thus, a metal carrier 85 having a cylindrical honeycomb structure is formed. The flat foil 86 is a plurality of air holes 86a. Equally dispersed and formed on a flat metal foil. The foil 87 is formed by, for example, uniformly dispersing a plurality of air holes 87a in a metal crucible formed in a stripe shape. A flat foil 86 is disposed on the outermost peripheral surface of the catalyst 23, and air is exposed on the outermost peripheral surface. The hole 86a corresponds to the air introduction hole 82. Fig. 15 is a cross-sectional view showing the configuration of an exhaust device and the like of the engine according to the sixth embodiment of the present invention. The portions corresponding to those in the above-mentioned 圊13 are denoted by the same reference numerals, and the description thereof will be omitted. In this embodiment, the downstream end 72b of the second passage 72 is connected to the side of the catalyst 23 and the upstream end 23a of the catalyst 23. In the outer peripheral region, a cylindrical air introduction space 88 in which the substantially entire side surface of the catalyst 23 is opened and the outer peripheral end 23a of the catalyst 23 is opened is formed in the downstream end 72b of the second passage 72. The catalyst 23 is formed. The secondary air supplied from the first passage 71 to the second passage 72 is supplied from the air introduction space 88 to the inside of the catalyst 23, for example, the side of the catalyst 23 and the upstream end of the catalyst 23. The outer peripheral area of 23a enters into the interior of the catalyst 23. The secondary air to the inside of the catalyst 23 is mixed with the exhaust gas introduced from the central portion of the upstream end 23a of the catalyst 23, and flows to the downstream end of the catalyst 23. Thus, 154997.doc •37-201239190 In the inside of the portion 23, the region 24A in which the central portion of the upstream end 23a of the catalyst 23 is tapered toward the downstream becomes a low oxygen concentration region in which the exhaust gas from the combustion chamber 1 is dominant. The remaining region 24B is a region of high oxygen concentration in which secondary air is sufficiently supplied. The catalyst 23 functions as a reduction catalyst in the low oxygen concentration region 24A and functions as an oxidation catalyst in the high oxygen concentration region 24B. Therefore, one catalyst 23 can be used as both a reduction catalyst and an oxidation catalyst. Since the secondary air is introduced from the outer peripheral region of the upstream end 23a of the catalyst 23, the "low oxygen concentration region 24 becomes smaller" than in the case of the fifth embodiment, that is, the oxygen is compared with the case of the fifth embodiment. The concentration region 25 becomes larger. Therefore, a sufficient amount of secondary air can be supplied to the catalyst 2, so that the exhaust gas from the combustion chamber 1 can be sufficiently detoxified. &lt;Fourth Embodiment&gt; Fig. 16 is a schematic view showing the configuration of an exhaust device of an engine according to a seventh embodiment of the present invention. In Fig. 16, the same reference numerals are attached to the corresponding portions of the respective portions shown in Fig. 1 described above. The fifth embodiment is an example in which an embodiment of the present invention is applied to a multi-cylinder engine. The engine 1 of the seventh embodiment includes a plurality of cylinders #8, #Ββ, each cylinder #8, #B includes: a cylinder block 3 (refer to FIG. ;); a cylinder head 4 disposed at one end of the cylinder block; The piston 5 (refer to FIG. 1) of the reciprocating motion in the cylinder block 3 and the portions form the combustion chamber 1〇. The cylinder head 4 is provided with an intake valve 8 that opens and closes the intake port 8a (refer to FIG. 1) (refer to FIG. 1); an exhaust valve 9 that opens and closes the exhaust port %; and is used to drive the intake valve 8 (refer to the figure 丨) and the valve device of the exhaust valve 9. The engine 1 further comprises: an exhaust device 5; and a 154997.doc

S -38· 201239190 排氣裝置50之排氣通道7供給空氣之二次空氣供給裝置 70 〇 排氣裝置50包括:連接於氣缸蓋4之第1排氣管51 ;連接 於該第1排氣管51之第2排氣管52 ;及連接於該第2排氣管 52之第3排氣管53。該些排氣管51、52、53形成排氣通道 7(7A ' 7B &gt; 7C) 〇 5亥實施形態中,第1排氣管51形成分別連接於複數個燃 燒室10之排氣口 9a之個別之排氣通道7A、7B。該些個別 排氣通道7A、7B於集合部25集合而連接於集合排氣通道 7C。於該集合排氣通道7C設置有漸縮_漸擴喷嘴仂。於漸 縮-漸擴喷嘴40下游側之集合排氣通㈣,隔開間隔而設 置有第1及第2觸媒21、22。又,形成第丨通道71之第丨二次 空氣供給管76連接於集合部25與漸縮_漸擴喷嘴4〇之間之 集合排氣通道7C。形成第2通道72之第2二次空氣供給管77 ^上游端連接於第1二次空氣供給管76。第2二次空氣供給 管77之下游端連接於第1及第2觸媒21、22之間,即連接於 第1觸媒21下游之集合排氣通道7C。其他構成與上述第^實 施形態相同。 圖17A〜圖17C係表示該第7實施形態之引擎之動作之模 式圖田一氣缸#]8之排氣口 9a打開時,排氣口9a閉合之另 轧缸#A之個別排氣通道7A作為分支部31發揮功能。 即’當氣㈣B之排氣口%打開時,自該排氣口%排出廢氣 广、且產生衝擊波35,該些廢氣36及衝擊波35通過個別排 風通道7B傳播(參照圖17A)。衝擊波35於集合部25分支並 154997.doc -39- 201239190 進入至另一氣缸#八之個別排氣通道7A ^該分支之衝擊波 35向上游側傳播過個別排氣通道7A(參照圖丨7B),並於氣 缸#八之排氣閥9(閉合狀態)反射。即,閉合狀態之排氣閥9 作為反射部31b發揮功能。反射之衝擊波35向下游側傳播 過個別排氣通道7 A,並再次到達集合部25(參照圖丨7C)而 與廢氣36衝撞。由此,於漸縮-漸擴喷嘴4〇之入口之壓力 提尚’從而於漸擴部43產生新的衝擊波。 藉由伴隨該新的衝擊波之產生而產生之負壓,使外部之 二次空氣被導入第1通道71。繼而,當藉由其後之排氣脈 動而使較漸擴部43更為上游之集合排氣通道7(:成為正壓 時’被導入至第1通道71之二次空氣會被送入至第2通道 72。由此,使二次空氣被送入至第丨觸媒2丨下游之集合排 氣通道7C。 如此,使排氣口 9a閉合之氣缸之個別排氣通道7A、7B 兼作分支部3 1,藉此可實現與參照上述圖4A〜圖4C所說明 之動作相同之動作而實現。各氣缸之個別排氣通道7a、 7B之管路長度係以使反射之衝擊波35與廢氣36於集合部25 衝撞之方式進行設計。 經排氣集合之氣缸#A、#B係處於當一方之氣缸之排氣 口 9a為打開狀態時、另一方之氣缸之排氣口 %為閉合狀態 之關係之一對氣缸組。更具體而言,於具有氣缸#1、#2、 #3、#4之4氣缸引擎中,點火順序設為氣缸#1_氣缸#3_氣缸 #4-氣缸#2。該情形時,點火時間相差36〇度之氣缸#1與氣 缸#4之組相當於上述兩個氣缸#A、#b之組。又,同樣地 154997.doc -40- 201239190 點火時間相差360度之氣缸#2與氣缸#3之組相當於上述兩 個氣缸#A、#B之組。即,4氣缸引擎中,相當於兩個氣缸 #A、#B之氣缸對存在有2對。 &lt;其他實施形態&gt; 圖18係表示搭載有本發明之一實施形態之引擎之船舶之 一例之立體圖。具體而言,船舶1 〇〇包括船體102,及具有 本發明之一實施形態之引擎1之舷外機1 〇 1。該例中,2台 舷外機101搭載於船體102 ^舷外機ιοί包括例如:引擎1 ; 作為推進力產生構件之螺旋槳(未圖示);及將引擎1之驅動 力傳遞至螺旋槳之傳遞機構(未圖示)。傳遞機構包括例 如.藉由引擎1之驅動力而旋轉之驅動軸;結合於螺旋槳 之螺旋槳轴;及設置於驅動軸與螺旋槳軸之間之離合器。 作為裝備於船舶100之推進力產生單元,除舷外機1〇1之 外,亦可例示舷内機、般内外機。此外,亦可使用例如將 藉由引擎而旋轉之葉輪置於水流路之喷射泵單元作為用 於船舶100之推進力產生單元。 圖19係表不搭載有本發明之一實施形態之引擎之車輛之 立體圖。具體而s ’作為車輛之一例之電動二輪車包 括·車身201 ;安裝於直盛 、單身201别後之前輪2〇2及後輪 2〇3(車輪);及本發明之—實施形態之引擎卜引擎丄配置於 車身加之中央。引擎1產生之驅動力藉由傳遞機構2〇4而 傳遞至後輪203。 此外’作為發電機或鍵链望 X嗎4之引擎,亦可應用本發明之 引擎。當然,本發明之引聲 奋 之適用對象並無任何限定。 154997.doc 201239190 圖20係表示實施形態之變形例之排氣通道等之剖面圖。 第1實施形態t ’如圖2G中再次所示般,第!二次空氣供略 管76’即第mit71於較分支部31更為下游連接於排氣^ 道7。然而,第丨通道71之連接位置既可為較分支部3ι更為 上游(參照符號71A),亦可為與分支部31相同之位置(參照 符號71Βρ μ 又,上述實施形態中,表示有相對於丨個燃燒室而設置 有1個排氣π之引擎,但亦可相對於—個燃燒室而具有複 數個排氣σ。又’表不有相對於i個燃燒室而設置有上個漸 縮-漸擴喷嘴之例’但亦可相對於一個燃燒室而設置有2個 =上喷嘴。該些變形當然亦可應用於具有複數個燃燒室之 多氣缸引擎。此外,本發明可應用於各種各樣之引擎。 進而,上述實施形態中,表示有相對於丨個排氣通道而 2置有1個分支部之構成,但亦可相對於一個排氣通道而 叹置有複數個分支部。例如,第丨實施形態(參照圖1)之構 成中,若以第1通道71滿足分支部31之條件(參照圖5)之方 式進行設計,則該構成實質上具有複數個分支部。又,亦 可設置將自排氣通道7之相同位置分支之複數個分支部之 端部加以連接而具有環狀通道之分支部。該情形時,於各 分支部傳播而來之衝擊波相互衝撞並反射。該情形時,複 ^個分支部連接之部分(衝擊波相互衝撞之部位)成為反射 部。反射部即便不存在如壁般之構件亦成立。 又’上述實施形態中,包括第【及第2觸媒21、22,但亦 可如圖21所示之第1實施形態之變形例般省去第2觸媒。 154997.doc • 42· 201239190 該情形時,藉由南笛!艇μ ㈣向第1觸媒21之下游供給 用’另一 使第1觸媒21之上游側部分作為還原觸媒發揮Γ 方面可使其下游側部分作為氧化觸媒發揮作用。即 由排氣脈動而將自第2通道 錯 子八心一-人空氣導入至筮 媒21時’廢氣中之空氣比率 丰挺间。由此,第1觸媒21之下 游側部分作為氧化觸媒發揮功能。從而,可利用二次空氣 有效率地淨化廢氣。第2〜第4及第6實施形態中亦可進行相 同之變形。 又’上述實施形態中,於第i通道71之簧片閥74之上游 具有空氧量控制閥75及空氣濾清器,但亦可省去該些中之 一者或兩者。 又’上述實施形態中’表示有於第丨通道Η之上游端配 置有簧片閥74之構成’但簧片閥74亦可配置於第i通道71 之上游端與下游端之間。該情形時,第2通道72之上游端 72a亦可於第1通道71中配置於簧片閥74與排氣通道7之 間。 又,圖14所示之觸媒亦可用作第5及第6實施形態以外之 實施形態中之第1及/或第2觸媒21、22。但第1及/或第2觸 媒21、22無需具有於側面具有空氣導入口之觸媒載體,以 可自上游端導入廢氣之方式構成即可。 進而,上述實施形態中’說明了經由第2通道72向排氣 通道供給二次空氣之構成’但二次空氣之供給目的地亦可 為排氣通道以外之部分。例如’圖22所示之一實施形態 中,第2通道72之下游端結合於蓄壓箱63之導入口 65°蓄 154997.doc • 43- 201239190 壓箱63劃分可收納氣壓高於大氣壓之高壓空氣之收納空間 64 °蓄壓箱63包括:導入空氣之導入口 65 ;開閉導入口 65 之單向閥66 ;及排出收納空間64内之高壓空氣之排出口 67。單向閥66以如下方式構成,即於第2通道72内之空氣 壓高於收納空間64内之空氣壓時打開,使空氣自第2通道 72流入至收納空間64 »單向閥66以如下方式構成,即於收 納空間64内之空氣壓為第2通道72内之空氣壓以上時保持 為閉合狀態’由此’可阻止空氣自收納空間64向第2通道 72流出》 根據該構成,收納空間64内之空氣受到加壓(壓縮),因 而可蓄積壓力。即,可將廢氣之能量轉換為壓力能量並加 以蓄積。高壓空氣供給路68之上游端連接於排出口 66。於 高壓空氣供給路68之中途配置有輸出控制閥69。藉由對輸 出控制閥69進行開閉而可控制蓄壓箱64中蓄積之高壓空氣 (壓縮空氣)之輸出。高壓空氣供給路68之下游端連接於利 用高壓空氣而作動之裝置210。作為該裝置210之一例而為 由煞車助力器及離合器助力器所代表之操作輔助裝置。 又,作為裝置210之其他例,可列舉空氣懸架裝置及警笛 裝置。 對本發明之實施形態進行了詳細說明,但該些只不過為 用以明確本發明之技術性内容之具體例,本發明不應限定 於該些具體例進行解釋,本發明之範圍僅藉由隨附之申請 專利範圍限定。 β 【圖式簡單說明】 154997.doc • 44- 201239190 圖1係表示本發明之第1實施形態之引擎構成之剖面圖。 圖2係表示漸縮-漸擴喷嘴之構成之模式圖。 圖3係表示漸縮-漸擴喷嘴之壓力比與馬赫數之關係之圖 表。 圖4係用以說明衝擊波與廢氣之行進狀態之剖面圖。圖 4A表示排氣衝程之初始狀態,圖4B表示衝擊波於分支路 内傳播時之狀態,圖4C表示於分支路反射之衝擊波與廢氣 衝撞時之狀態。 圖5係表示衝擊波之行進路徑與廢氣之行進路徑之排氣 通道等之模式圖。 圖6係使藉由紋影攝影法而拍攝漸縮·漸擴噴嘴内部而得 之照片模式化之模式圖。 圖7係表示衝擊波加速時之廢氣流速與廢氣壓力之關係 之圖表。 圖8係表示衝擊波加速時之廢氣流速與廢氣溫度之關係 之圖表。 圖9係用以說明二次空氣供給裝置之作用之圖。圖9A係 表示曲柄角與排氣通道内之壓力之關係之一例之圖。圖9B 係表示曲柄角與第丨通道中之氣體之質量流量之關係之一 例之圖。圖9C係表示曲柄角與排氣通道及二次空氣供給裝 置之各部分中之氧濃度之關係之一例之圖。 圖10係表示本發明之第2實施形態之引擎之排氣通道等 之構成之剖面圖。 圖11係本發明之第3實施形態之引擎之排氣通道等之構 154997.doc -45· 201239190 成之剖面圖。 圖12係用以說明本發明之第彳實施形態之 置等之構成之剖面圖。 $之排孔裝 用以說明本發明之第5實施形態之?丨擎之排氣裝 置等之構成之剖面圖。 圖14係用以說明觸媒之構成例之圖解性之立體圖。 用以說明本發明之第6實施形態…之排氣裝 置荨之構成之剖面圖。 圖16係表示本發明之第7實施形態之引擎之排氣裝置之 構成之模式圖。 圖⑽表示第7實施形態之引擎之動作之模式圖。圖Μ 表不排氣衝程之初始狀態’圖17B表示衝擊波於其他氣缸 之個別排氣通道(分支路)内傳播時之狀態,圖I%表示於 分支路反射之衝擊波與廢氣衝揸時之狀態。 、 圖18係例示包括搭載有引擎之舷外機之船舶之圖。 圖19係例示搭載有引擎之電動二輪車之圓。 圖20係表示變形例之排氣通道等之剖面圖。 圖21係表示第1實施形態之變形例之構成之剖面圖。 圖22係表示本發明之第8實施形態之構成之模式圖。 【主要元件符號說明】 1 引擎 2 喷射器 3 氣缸體 4 氣缸蓋 I54997.doc .46-S -38· 201239190 Exhaust passage 7 of exhaust device 50 Secondary air supply device 70 for supplying air 〇Exhaust device 50 includes: first exhaust pipe 51 connected to cylinder head 4; connected to the first exhaust gas The second exhaust pipe 52 of the pipe 51; and the third exhaust pipe 53 connected to the second exhaust pipe 52. The exhaust pipes 51, 52, and 53 form an exhaust passage 7 (7A '7B &gt; 7C). In the embodiment, the first exhaust pipe 51 is formed with exhaust ports 9a connected to the plurality of combustion chambers 10, respectively. Individual exhaust passages 7A, 7B. The individual exhaust passages 7A, 7B are collected in the collecting portion 25 and connected to the collecting exhaust passage 7C. A tapered_riverging nozzle 仂 is provided in the collective exhaust passage 7C. The first and second catalysts 21 and 22 are disposed at intervals along the collective exhaust gas passage (four) on the downstream side of the tapered-divergent nozzle 40. Further, the second secondary air supply pipe 76 forming the second passage 71 is connected to the collective exhaust passage 7C between the collecting portion 25 and the tapered_riverging nozzle 4A. The second secondary air supply pipe 77 that forms the second passage 72 is connected to the first secondary air supply pipe 76 at the upstream end. The downstream end of the second secondary air supply pipe 77 is connected between the first and second catalysts 21 and 22, that is, connected to the collective exhaust passage 7C downstream of the first catalyst 21. The other configuration is the same as that of the above embodiment. 17A to 17C are diagrams showing the operation of the engine according to the seventh embodiment. When the exhaust port 9a of the first cylinder #8 is opened, the exhaust passage 9a is closed, and the individual exhaust passages 7A of the additional cylinder #A are closed. The branch unit 31 functions. That is, when the exhaust port % of the gas (four) B is turned on, the exhaust gas is exhausted from the exhaust port %, and the shock wave 35 is generated, and the exhaust gas 36 and the shock wave 35 are propagated through the individual exhaust passages 7B (refer to Fig. 17A). The shock wave 35 branches at the collecting portion 25 and 154997.doc -39 - 201239190 enters the individual exhaust passage 7A of the other cylinder #8. The shock wave 35 of the branch propagates to the upstream side through the individual exhaust passage 7A (refer to Fig. 7B). And reflected in the cylinder #8's exhaust valve 9 (closed state). That is, the exhaust valve 9 in the closed state functions as the reflecting portion 31b. The reflected shock wave 35 propagates to the downstream side through the individual exhaust passages 7 A, and reaches the collecting portion 25 again (see Fig. 7C) to collide with the exhaust gas 36. Thereby, the pressure at the entrance of the tapered-divergent nozzle 4 is raised to generate a new shock wave in the dilating portion 43. The external secondary air is introduced into the first passage 71 by the negative pressure generated by the generation of the new shock wave. Then, when the exhaust gas pulsation is followed by the exhausting passage 7 which is further upstream than the diverging portion 43 (when the positive pressure is applied, the secondary air introduced into the first passage 71 is sent to The second passage 72. Thereby, the secondary air is sent to the collective exhaust passage 7C downstream of the second catalyst 2丨. Thus, the individual exhaust passages 7A, 7B of the cylinders for closing the exhaust port 9a serve as points. The branch portion 3 1 can be realized by the same operation as that described with reference to the above-described Figs. 4A to 4C. The lengths of the individual exhaust passages 7a, 7B of the respective cylinders are such that the shock wave 35 and the exhaust gas 36 are reflected. The design is performed in such a manner that the collecting portion 25 collides. The cylinders #A and #B of the exhaust gas collection are in a closed state when the exhaust port 9a of one of the cylinders is in an open state, and the exhaust port % of the other cylinder is in a closed state. One of the relationships is for the cylinder group. More specifically, in the four-cylinder engine with cylinders #1, #2, #3, #4, the ignition sequence is set to cylinder #1_cylinder#3_cylinder#4-cylinder# 2. In this case, the group of cylinder #1 and cylinder #4 whose ignition timing differs by 36 相当于 is equivalent to the above two cylinders #A, #b Also, similarly, 154997.doc -40- 201239190 The group of cylinder #2 and cylinder #3 whose ignition timing differs by 360 degrees corresponds to the group of the above two cylinders #A, #B. That is, in the 4-cylinder engine, There are two pairs of cylinder pairs of the two cylinders #A and #B. <Other Embodiments> Fig. 18 is a perspective view showing an example of a ship on which an engine according to an embodiment of the present invention is mounted. 1 〇〇 includes a hull 102 and an outboard motor 1 〇1 having an engine 1 according to an embodiment of the present invention. In this example, two outboard motors 101 are mounted on the hull 102. The outboard machine ιοί includes, for example: An engine 1; a propeller (not shown) as a propulsion generating member; and a transmitting mechanism (not shown) for transmitting the driving force of the engine 1 to the propeller. The transmitting mechanism includes, for example, a rotating force by the driving force of the engine 1. a drive shaft; a propeller shaft coupled to the propeller; and a clutch disposed between the drive shaft and the propeller shaft. As a propulsion generating unit equipped with the ship 100, an inboard machine may be exemplified in addition to the outboard motor 1〇1 , inside and outside the machine. In addition, you can also use the example A jet pump unit that is placed in a water flow path by an impeller that is rotated by an engine is used as a propulsive force generating unit for the ship 100. Fig. 19 is a perspective view showing a vehicle in which an engine according to an embodiment of the present invention is not mounted. 'The electric two-wheeled vehicle as an example of the vehicle includes the body 201; the front wheel 2〇2 and the rear wheel 2〇3 (wheel) attached to the straight body, the single body 201, and the engine engine 丄 of the embodiment of the present invention The vehicle body is centered. The driving force generated by the engine 1 is transmitted to the rear wheel 203 by the transmission mechanism 2〇4. Further, the engine of the present invention can also be applied as an engine of a generator or a key chain. Of course, there is no limitation on the application of the present invention. 154997.doc 201239190 Fig. 20 is a cross-sectional view showing an exhaust passage or the like according to a modification of the embodiment. The first embodiment t' is as shown again in Fig. 2G, the first! The secondary air supply pipe 76', i.e., the mit 71, is connected downstream of the branch portion 31 to the exhaust gas passage 7. However, the connection position of the second channel 71 may be further upstream than the branch portion 3 (refer to reference numeral 71A) or may be the same position as the branch portion 31 (reference numeral 71Βρ μ, in the above embodiment, the relative position is indicated. An engine with one exhaust gas π is provided in one combustion chamber, but a plurality of exhaust gases σ may be provided with respect to one combustion chamber. Further, there is no upper chamber with respect to i combustion chambers. The example of the contraction-swelling nozzle is 'but it is also possible to provide two = upper nozzles with respect to one combustion chamber. These deformations can of course also be applied to a multi-cylinder engine having a plurality of combustion chambers. Further, the present invention can be applied to Further, in the above embodiment, the configuration is such that one branch portion is provided for each of the exhaust passages 2, but a plurality of branch portions may be slanted with respect to one exhaust passage. For example, in the configuration of the third embodiment (see FIG. 1), when the first channel 71 satisfies the condition of the branch portion 31 (see FIG. 5), the configuration has substantially a plurality of branch portions. Can also be set to self-exhaust The ends of the plurality of branch portions of the same position of the track 7 are connected to each other to have a branch portion of the annular passage. In this case, the shock waves propagating from the respective branch portions collide with each other and are reflected. In this case, The portion where the branch portions are connected (the portion where the shock waves collide with each other) serves as a reflecting portion. The reflecting portion is formed even if there is no member such as a wall. In the above embodiment, the first and second catalysts 21 and 22 are included. The second catalyst can be omitted as in the modification of the first embodiment shown in Fig. 21. 154997.doc • 42· 201239190 In this case, the downstream of the first catalyst 21 is supplied by the south flute! In the case where the other side of the first catalyst 21 is used as a reduction catalyst, the downstream side portion can function as an oxidation catalyst. That is, the exhaust gas pulsates and the second channel is misplaced. When the air is introduced into the sputum 21, the ratio of the air in the exhaust gas is rich. Thus, the downstream side portion of the first catalyst 21 functions as an oxidation catalyst. Therefore, the exhaust gas can be efficiently purified by the secondary air. 2nd to 4th and 6th The same deformation can be performed in the form. In the above embodiment, the air oxygen amount control valve 75 and the air cleaner are provided upstream of the reed valve 74 of the i-th channel 71, but the above may be omitted. In the above-described embodiment, 'the configuration of the reed valve 74 is disposed at the upstream end of the second channel '', but the reed valve 74 may be disposed at the upstream and downstream of the i-th channel 71. In this case, the upstream end 72a of the second passage 72 may be disposed between the reed valve 74 and the exhaust passage 7 in the first passage 71. Further, the catalyst shown in Fig. 14 may also be used. The first and/or second catalysts 21 and 22 in the embodiment other than the fifth and sixth embodiments. However, the first and/or second catalysts 21 and 22 do not need to have the air introduction port on the side surface. The medium carrier may be configured to be capable of introducing exhaust gas from the upstream end. Further, in the above-described embodiment, 'the configuration of supplying the secondary air to the exhaust passage via the second passage 72' has been described, but the supply destination of the secondary air may be a portion other than the exhaust passage. For example, in one embodiment shown in Fig. 22, the downstream end of the second passage 72 is coupled to the inlet 65 of the accumulator tank 63. 154997.doc • 43- 201239190 The pressure box 63 divides the high pressure at which the air pressure is higher than the atmospheric pressure. The air storage space 64° pressure storage tank 63 includes an inlet port 65 for introducing air, a check valve 66 for opening and closing the inlet port 65, and a discharge port 67 for discharging high-pressure air in the storage space 64. The check valve 66 is configured to open when the air pressure in the second passage 72 is higher than the air pressure in the storage space 64, and to allow air to flow from the second passage 72 to the accommodation space 64 » the check valve 66 as follows In a configuration, when the air pressure in the storage space 64 is equal to or higher than the air pressure in the second passage 72, the air is kept in a closed state. This prevents air from flowing out of the storage space 64 to the second passage 72. According to this configuration, the air is stored. The air in the space 64 is pressurized (compressed) so that pressure can be accumulated. That is, the energy of the exhaust gas can be converted into pressure energy and accumulated. The upstream end of the high pressure air supply path 68 is connected to the discharge port 66. An output control valve 69 is disposed in the middle of the high-pressure air supply path 68. The output of the high-pressure air (compressed air) accumulated in the accumulator tank 64 can be controlled by opening and closing the output control valve 69. The downstream end of the high pressure air supply path 68 is connected to a device 210 that operates with high pressure air. As an example of the device 210, it is an operation assisting device represented by a brake booster and a clutch booster. Further, as another example of the device 210, an air suspension device and a siren device can be cited. The embodiments of the present invention have been described in detail, but these are merely specific examples for clarifying the technical contents of the present invention. The present invention is not limited to the specific examples, and the scope of the present invention is only The scope of the patent application is limited. 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 Fig. 2 is a schematic view showing the configuration of a tapered-semi-expansion nozzle. Fig. 3 is a graph showing the relationship between the pressure ratio of the tapered-swelling nozzle and the Mach number. Fig. 4 is a cross-sectional view for explaining a traveling state of a shock wave and an exhaust gas. Fig. 4A shows the initial state of the exhaust stroke, Fig. 4B shows the state when the shock wave propagates in the branch path, and Fig. 4C shows the state when the shock wave reflected by the branch path collides with the exhaust gas. Fig. 5 is a schematic view showing an exhaust passage of a traveling path of a shock wave and a traveling path of an exhaust gas. Fig. 6 is a schematic view showing a pattern of photographs obtained by photographing the inside of a tapered and divergent nozzle by a schlieren method. Fig. 7 is a graph showing the relationship between the exhaust gas flow rate and the exhaust gas pressure at the time of shock wave acceleration. Fig. 8 is a graph showing the relationship between the flow rate of the exhaust gas at the time of shock wave acceleration and the temperature of the exhaust gas. Fig. 9 is a view for explaining the action of the secondary air supply device. Fig. 9A is a view showing an example of the relationship between the crank angle and the pressure in the exhaust passage. Fig. 9B is a view showing an example of the relationship between the crank angle and the mass flow rate of the gas in the third channel. Fig. 9C is a view showing an example of the relationship between the crank angle and the oxygen concentration in each portion of the exhaust passage and the secondary air supply means. Fig. 10 is a cross-sectional view showing the configuration of an exhaust passage or the like of an engine according to a second embodiment of the present invention. Fig. 11 is a cross-sectional view showing the structure of an exhaust passage of an engine according to a third embodiment of the present invention, 154997.doc-45·201239190. Fig. 12 is a cross-sectional view showing the configuration of the third embodiment of the present invention. 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 Fig. 14 is a schematic perspective view for explaining a configuration example of a catalyst. A cross-sectional view showing the configuration of an exhaust device 第 according to a sixth embodiment of the present invention. Fig. 16 is a schematic view showing the configuration of an exhaust device of an engine according to a seventh embodiment of the present invention. Fig. 10 is a schematic view showing the operation of the engine of the seventh embodiment. Figure Μ shows the initial state of the exhaust stroke. Figure 17B shows the state of the shock wave propagating in the individual exhaust passages (branch paths) of other cylinders. Figure I% shows the state of the shock wave reflected by the branch road and the exhaust gas. . Fig. 18 is a view showing a ship including an outboard motor equipped with an engine. Fig. 19 is a view showing a circle of an electric two-wheeled vehicle equipped with an engine. Fig. 20 is a cross-sectional view showing an exhaust passage or the like of a modification. Fig. 21 is a cross-sectional view showing the configuration of a modification of the first embodiment. Fig. 22 is a schematic view showing the configuration of an eighth embodiment of the present invention. [Main component symbol description] 1 Engine 2 Injector 3 Cylinder block 4 Cylinder head I54997.doc .46-

201239190 5 6 6a 7、7C、7B、7C 7a 8 8a 9 9a 9ac 10 11 12 15 16 17 19201239190 5 6 6a 7, 7C, 7B, 7C 7a 8 8a 9 9a 9ac 10 11 12 15 16 17 19

20 21 22 23 23a 24A 24B 活塞 進氣通道 進氣通道之下游部 排氣通道 排氣通道之上游部 進氣閥 進氣口 排氣閥 排氣口 排氣口之中心 燃燒室 節氣門閥 螺栓 連桿 曲柄軸 曲柄箱 氧濃度感測器 ECU 第1觸媒 第2觸媒 觸媒 觸媒之上游端 低氧濃度區域 向氧濃度區域 • 47· 154997.doc 201239190 25 集合部 30 分支管 31 分支部 31a 入口 31b 反射部 35 衝擊波 35b 新衝擊波(行進衝擊波) 35c 膨脹波 36 廢氣 40 漸縮-漸擴喷嘴 41 漸縮部 42 喉部 43 漸擴部 50 排氣裝置 51 第1排氣管 52 第2排氣管 53 第3排氣管 55 排氣室 61 流路 62 流路 63 蓄壓箱 64 收納空間 65 導入口 66 單向閥 154997.doc ·48· 201239190 67 排出口 68 高壓空氣供給路 69 輸出控制閥 70 二次空氣供給裝置 71 第1通道 71A、71B、91、 參照符號 92 、 93 、 94 、 95 、 99 71a 第1通道之上游端 71b 與排氣通道之連接部 72 第2通道 72a 與第1通道之連接部 72b 與排氣通道之連接部 74 簧片閥 75 空氣量控制閥 76 第1二次空氣供給管 77 第2二次空氣供給管 78 空氣濾清器 80 (第2)簧片閥 81 筒狀之空氣導入空間 82 空氣導入孔 83 孔口 85 金屬載體 86 平坦箔片 、下游端 上游端 、下游端 154997.doc • 49- 201239190 86a、87a 空氣孔 87 波形箔片 88 空氣導入空間 96a ' 96b ' 96c ' 曲線 96d 100 船舶 101 舷外機 102 船體 200 電動二輪車 201 車身 202 前輪 203 後輪 204 傳遞機構 210 利用高壓空氣作動之聚置 A、B 氣紅 A1 漸縮部之上游端之流路剖面積 A2 喉部之流路剖面積 A3 漸擴部之下游端之流路剖面積 A4 分支部之流路剖面積 A5 較分支部入口更為上游之排氣通道之 部分之流路剖面積 A6 漸擴部之流路剖面積 A7 較入口更為下游之排氣通道之部分之 流路剖面積 I54997.doc -5〇· 20123919020 21 22 23 23a 24A 24B Piston Intake Channel Intake Channel Downstream Exhaust Channel Exhaust Channel Upstream Intake Valve Inlet Exhaust Valve Exhaust Port Vent Center Combustion Chamber Throttle Valve Bolt Link Crankshaft crankcase oxygen concentration sensor ECU First catalyst second catalyst contact catalyst upstream end low oxygen concentration region to oxygen concentration region • 47· 154997.doc 201239190 25 assembly portion 30 branch pipe 31 branch portion 31a Entrance 31b Reflection portion 35 Shock wave 35b New shock wave (traveling shock wave) 35c Expansion wave 36 Exhaust gas 40 Tapered-swelling nozzle 41 Tapering portion 42 Throat portion 43 Scaling portion 50 Exhaust device 51 First exhaust pipe 52 Row 2 Air pipe 53 Third exhaust pipe 55 Exhaust chamber 61 Flow path 62 Flow path 63 Accumulator tank 64 Storage space 65 Guide port 66 Check valve 154997.doc ·48· 201239190 67 Discharge port 68 High-pressure air supply path 69 Output control Valve 70 Secondary air supply device 71 First passages 71A, 71B, 91, reference numerals 92, 93, 94, 95, 99 71a Connection portion 72 of the upstream end 71b of the first passage and the exhaust passage 72 Connection portion 74 of the second passage 72a and the first passage and the connection portion of the exhaust passage 74 Reed valve 75 Air amount control valve 76 First secondary air supply pipe 77 Second secondary air supply pipe 78 Air cleaner 80 (2nd) Reed valve 81 Cylindrical air introduction space 82 Air introduction hole 83 Hole 85 Metal carrier 86 Flat foil, downstream end upstream end, downstream end 154997.doc • 49- 201239190 86a, 87a Air hole 87 Waveform Foil 88 Air introduction space 96a ' 96b ' 96c ' Curve 96d 100 Ship 101 Outboard motor 102 Hull 200 Electric two-wheeler 201 Body 202 Front wheel 203 Rear wheel 204 Transmission mechanism 210 Using high-pressure air to actuate A, B Gas red A1 The cross-sectional area of the flow path at the upstream end of the tapered portion A2 The cross-sectional area of the flow path of the throat A3 The cross-sectional area of the flow path at the downstream end of the diverging portion A4 The cross-sectional area of the flow path of the branch portion A5 The exhaust gas upstream of the branch inlet The cross-sectional area of the flow path of the part of the passage A6 The cross-sectional area of the flow path of the gradually expanding part A7 The cross-sectional area of the part of the exhaust passage which is further downstream than the inlet I54997.doc -5〇· 201239190

P PO Le Ls Ld a、b、c、 X Y 漸擴部之壓力 漸縮部之壓力 自排氣口之中心至分支部入口之流路 剖面中心線為止之距離(流路長度) 排氣通道之流路剖面中心線與反射部 之間之距離(流路長度) 自分支部入口之流路剖面中心線至漸 擴部之上游端為止之距離(流路長度) 測定點 分支部入口之流路剖面中心線 排氣通道之流路剖面中心線 154997.doc •51 ·P PO Le Ls Ld a, b, c, XY The pressure taper of the taper is the distance from the center of the exhaust port to the center line of the flow path of the branch inlet (flow path length) Distance between the center line of the flow path section and the reflecting portion (flow path length) Distance from the center line of the flow path section of the branch inlet to the upstream end of the diverging portion (flow path length) Measurement of the flow path section of the branch branch inlet Center line of the center line exhaust passage 154997.doc •51 ·

Claims (1)

201239190 七、申請專利範圍: L 一種引擎,其包括: 燃燒室’其形成有排氣口 ; 排氣閥,其開閉上述排氣口; . 排氣裝置,其具有導引自上述燃燒室通過上述排氣口 排出之廢氣之排氣通道;及 空氣供給裝置,其供給空氣; 上述排氣裝置包括: 漸縮。卩,其设置於上述排氣通道,且下游端之流路剖 面積小於上游端之流路剖面積; 漸擴部’其於上述排氣通道中設置於較上述漸縮部更 為下游’且下游端之流路剖面積大於上游端之流路剖面 積;及 分支部,其將以較上述排氣口打開時自上述燃燒室流 入至上述排氣通道之廢氣更高之速度在上述排氣通道中 朝向下游傳播之衝擊波,於較上述漸擴部更為上游處自 上述排氣通道分支,且將該衝擊波再次向上述排氣通道 傳播; 上述空氣供給裝置包括: 第1通道,其具有使自上游端朝向下游端之氣流通過 之第1簣片閥’且下游端連接於上述排氣通道之較上述 漸擴部更為上游處;及 第2通道,其上游端連接於上述第】通道之較上述第1 簧片閥更為下游處;且 154997.doc 201239190 上述排氣裝置構成為:使自上述燃燒室流入至上述排 氣通道之廢氣通過上述漸縮部,且於上述分支部與上述 漸擴邛之間與在上述分支部中傳播之衝擊波發生衝撞, 藉此於上述漸縮部提高廢氣之Μ力,並藉由使此,壓力經 提尚之廢氣通過上述漸擴部而產生新的衝擊波; 上述空氣供給裝置構成為:利用藉由上述新產生之衝 擊波而於較上述漸擴部更為上游之上述排氣通道内產生 2. 3. 4. 負壓通過上述第1簧片閥而將空氣導入上述第1通 道’並利用純上述漸擴部更為上游之上述排氣通道内 產生之正壓而將上述導入之空氣供給至上述第2通道。 如°月求項1之引擎’其中以使流過自上述第1通道之上游 端至下游端之流路之氣體之能量損失,小於流過自上述 、I之下游端至上述第1通道之下游端之流路之氣體 之旎量損失的方式構成上述第〗通道及第2通道。 如呀长項1之引擎,其中以如下方式構成上述第!通道及 第2通道·當封閉上述第2通道而使空氣自上述第1通道 之上游端向下游端流動時之上述&amp;通道之下游端的流 '、 大於田使上述第1通道在較其與上述第2通道之 連,部更為上游側處封閉而使空氣自上述第2通道之下 游^向上述第1通道之下游端流動時之上述第1通道之下 游端的流量係數。 =項1之引擎,其中上述空氣供給裝置進而包括第2 '4,其設置於上述第2通道’且使自上述第2通道之 上游端朝向下游端之空氣通過。 I54997.doc 201239190 5.如請求項!之引擎,其中 道。 支。卩兼作為上述第!通 6·如請求項1之引擎,其中進而包括孔口,装 道與上述第2通道連接之連接部與上其於上述第1通 之間,配置於上” _之0。第1通道之下游端 7.如明求項1之弓丨擎,其中上述第 述排氣通道。 、&lt;下游端連接於上 用长項7之引擎’其中進而包括第1觸媒龙 氣通道中設置於較上述漸擴部更為下游處,’、於上述排 上述第2通道之下游端連接於上 第1觸媒更為下游處。 札通道之較上述 9» 其中上述排氣 媒,其遇而包括第2觸 再配置於較上述第2通道之下 ^ 氣通道。 更為下游側之排 10·如凊求項7之引擎,其中進而包括第i 氣通道中钟¥於t t 觸媒’其於上述排 、甲叹置於較上述漸擴部更為下游處, 上述第2通道之下游端於上述第 述排氣通道。 媒之側方連接於上 11·如請求項1〇之引擎,其中上述第Μ 導入孔。 則面具有空氣 之下游端連接於 之空氣亦可自上 12·如請求項10之引擎,其中上述第2通道 上述排氣通道,以使來自上述第2通道 述第1觸媒之上游端導入至該第丨觸媒。 13.如請求項11之引擎 其中上述第2通道 &lt;下游端連接於 154997.doc 201239190 上述排氣通道,以使來自上述第2通道之空氣亦可自上 述第1觸媒之上游端導入至該第丨觸媒。 M.如請求項⑴丨擎’其中上述第2通道中之氧漢度高於較 上述第1觸媒更為上游之上述排氣通道内之氧濃度。 15. -種車輛,其具備如請求項ljli4中任—項之引擎。 16· 一種船舶’其具備如請求項1至14中任一項之引擎。 154997.doc201239190 VII. Patent application scope: L An engine comprising: a combustion chamber formed with an exhaust port; an exhaust valve opening and closing the exhaust port; and an exhaust device having a guide from the combustion chamber through An exhaust passage of the exhaust gas discharged from the exhaust port; and an air supply device that supplies air; the exhaust device includes: a taper. The crucible is disposed in the exhaust passage, and the cross-sectional area of the flow path at the downstream end is smaller than the cross-sectional area of the flow path at the upstream end; the diverging portion is disposed downstream of the tapered portion in the exhaust passage and a cross-sectional area of the flow path at the downstream end is larger than a cross-sectional area of the flow path at the upstream end; and a branch portion that is at a higher speed than the exhaust gas flowing from the combustion chamber to the exhaust passage when the exhaust port is opened a shock wave propagating downstream in the passage branches from the exhaust passage further upstream than the diverging portion, and the shock wave is again transmitted to the exhaust passage; the air supply device includes: a first passage having a a flow from the upstream end toward the downstream end through the first flap valve 'and a downstream end connected to the exhaust passage further upstream than the diverging portion; and a second passage having an upstream end connected to the first passage The exhaust device is further downstream than the first reed valve; and 154997.doc 201239190 is configured to: exhaust the exhaust gas flowing from the combustion chamber to the exhaust passage through the above-mentioned a contraction portion that collides with a shock wave propagating in the branch portion between the branch portion and the diverging enthalpy, thereby increasing the force of the exhaust gas at the tapered portion, and by which the pressure is improved The exhaust gas is generated by the diverging portion to generate a new shock wave; and the air supply device is configured to generate the exhaust passage in the exhaust passage further upstream than the diverging portion by the newly generated shock wave. The negative pressure is introduced into the first passage ′ through the first reed valve, and the introduced air is supplied to the second passage by a positive pressure generated in the exhaust passage upstream of the purely expanding portion. . For example, the engine of the item 1 of the month 1 is such that the energy loss of the gas flowing through the flow path from the upstream end to the downstream end of the first passage is smaller than the flow from the downstream end of the I, to the first passage. The manner in which the amount of gas in the flow path at the downstream end is lost constitutes the first passage and the second passage. The engine of the long item 1, wherein the first channel and the second channel are configured to block the second channel to allow air to flow from the upstream end to the downstream end of the first channel The flow at the downstream end is larger than the field, so that the first passage is closed at the upstream side of the portion connected to the second passage, and the air flows from the downstream of the second passage to the downstream end of the first passage. The flow coefficient of the downstream end of the first passage at the time. The engine of item 1, wherein the air supply device further includes a second '4' disposed in the second passage' and passing air from the upstream end of the second passage toward the downstream end. I54997.doc 201239190 5. The engine of the request item! support.卩 Also as the above! The engine of claim 1, further comprising an orifice, wherein the connecting portion connected to the second passage and the first passage are disposed between the first passage and the first passage. The downstream end 7. The bowing engine of the present invention, wherein the first exhaust passage is connected to the engine of the upper end 7 of the engine, wherein the first catalyst is disposed in the first air passage. Further downstream of the diverging portion, 'the downstream end of the second passage in the row is connected to the downstream of the upper first catalyst. The passage of the passage is higher than the above 9», wherein the exhaust medium meets Including the second touch is disposed in the gas channel below the second channel. The row on the downstream side is the engine of the item 7, which further includes the clock in the i-th gas channel. The downstream end of the second passage is located further downstream than the diverging portion, and the downstream end of the second passage is in the first exhaust passage. The side of the medium is connected to the upper 11 · the engine of claim 1 Wherein the third inlet hole is introduced, and the air having the downstream end of the air is connected to the air The engine of claim 10, wherein the exhaust passage of the second passage is such that an upstream end of the first catalyst from the second passage is introduced into the third catalyst. In the engine, the second passage &lt; downstream end is connected to the exhaust passage of 154997.doc 201239190 such that air from the second passage can be introduced into the second catalyst from the upstream end of the first catalyst. M. The request item (1) 丨 ' 'where the oxygen level in the second channel is higher than the oxygen concentration in the exhaust channel upstream of the first catalyst. 15. - a vehicle having the request The engine of any item in item ljli4. 16· A ship having an engine as claimed in any one of claims 1 to 14. 154997.doc
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TWI659149B (en) * 2017-06-06 2019-05-11 三陽工業股份有限公司 Exhaust pipe structure for motorcycle

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EP3239505B1 (en) * 2014-12-22 2020-04-08 Yamaha Hatsudoki Kabushiki Kaisha Air-cooled engine unit

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI659149B (en) * 2017-06-06 2019-05-11 三陽工業股份有限公司 Exhaust pipe structure for motorcycle

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