JPH0115860Y2 - - Google Patents

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Publication number
JPH0115860Y2
JPH0115860Y2 JP10231284U JP10231284U JPH0115860Y2 JP H0115860 Y2 JPH0115860 Y2 JP H0115860Y2 JP 10231284 U JP10231284 U JP 10231284U JP 10231284 U JP10231284 U JP 10231284U JP H0115860 Y2 JPH0115860 Y2 JP H0115860Y2
Authority
JP
Japan
Prior art keywords
diffusion
flame
piston
outer periphery
swirl chamber
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP10231284U
Other languages
Japanese (ja)
Other versions
JPS6117419U (en
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed filed Critical
Priority to JP10231284U priority Critical patent/JPS6117419U/en
Priority to DE19853520775 priority patent/DE3520775A1/en
Priority to GB08514801A priority patent/GB2160262B/en
Priority to US06/743,673 priority patent/US4662330A/en
Publication of JPS6117419U publication Critical patent/JPS6117419U/en
Application granted granted Critical
Publication of JPH0115860Y2 publication Critical patent/JPH0115860Y2/ja
Granted legal-status Critical Current

Links

Description

【考案の詳細な説明】 (産業上の利用分野) 本考案は、渦流室式デイーゼルエンジンの燃焼
室の改良に関し、詳しくはピストン頂上部に形成
する主室キヤビテイの改良に関する。
[Detailed Description of the Invention] (Industrial Application Field) The present invention relates to an improvement in the combustion chamber of a swirl chamber type diesel engine, and more particularly to an improvement in a main chamber cavity formed at the top of a piston.

(従来の技術) 高速デイーゼルエンンジンに適した燃焼室とし
て渦流室式が知られているが、その燃焼性状をさ
らに改善する目的で第3図、第4図に示すような
ものが提案されている(実開昭57−78724号参
照)。
(Prior Art) The swirl chamber type is known as a combustion chamber suitable for high-speed diesel engines, but the ones shown in Figures 3 and 4 have been proposed to further improve its combustion properties. (Refer to Utility Model Publication No. 57-78724).

これを説明すると、エンジンの圧縮上死点付近
で渦流室20内で着火された燃料は火炎(燃焼ガ
ス)となつて噴口21から主室キヤビテイ6内に
噴出流入する。
To explain this, fuel ignited in the swirl chamber 20 near the compression top dead center of the engine becomes a flame (combustion gas) and ejects into the main chamber cavity 6 from the injection port 21.

主室キヤビテイ6内では火炎(流れをBで示
す)はトレンチ部10に沿つて流れ、一対の拡散
部7,8の連結部9に衝突し二手に分かれる。分
かれた火炎は拡散部7,8の円弧に沿つて拡散
し、新気を取り入れながら燃焼が進行する。な
お、トレンチ部10は溝状に、一対の拡散部7,
8は円形状凹部に形成されている。また、1はシ
リンダブロツク、2はシリンダヘツド、23は燃
料噴射弁、24はグロープラグである。
Inside the main chamber cavity 6, the flame (flow is indicated by B) flows along the trench portion 10, collides with the connecting portion 9 of the pair of diffusion portions 7 and 8, and splits into two. The separated flames spread along the arcs of the diffusion parts 7 and 8, and combustion progresses while taking in fresh air. Incidentally, the trench portion 10 has a groove shape and a pair of diffusion portions 7,
8 is formed into a circular recess. Further, 1 is a cylinder block, 2 is a cylinder head, 23 is a fuel injection valve, and 24 is a glow plug.

ところで、一般に、渦流室式デイーゼルエンジ
ンにおいてHCやスモークの排出量を低減するに
は、渦流室容積をできるだけ大きくして噴射燃料
に対する渦流室内の空気利用率を高めることが有
効である。
By the way, in general, in order to reduce the amount of HC and smoke emitted in a swirl chamber type diesel engine, it is effective to increase the volume of the swirl chamber as much as possible to increase the air utilization rate in the swirl chamber for the injected fuel.

しかし、渦流室容積を増大すると、エンジンの
圧縮比が低下し、この圧縮比の低下により圧縮空
気温度が下がり、HC排出量が増大する。このた
め、渦硫室容積を増大する場合には、主室キヤビ
テイ容積を小さく抑えて全体としての燃焼室容積
を考慮する必要がある。
However, increasing the swirl chamber volume lowers the compression ratio of the engine, which lowers the compressed air temperature and increases HC emissions. Therefore, when increasing the swirl chamber volume, it is necessary to keep the main chamber cavity volume small and take into account the combustion chamber volume as a whole.

一方、渦流室から主室に噴出した火炎内の未燃
成分を主室内で良好に燃焼させるためには、火炎
と主室内空気との混合を良好にすればよく、この
ためには前述の主室キヤビテイの拡散部容積を確
保する必要がある。
On the other hand, in order to properly burn the unburned components in the flame ejected from the swirl chamber into the main chamber, it is sufficient to improve the mixing of the flame and the air in the main chamber. It is necessary to secure the volume of the diffusion section of the chamber cavity.

こうした3つの要求から主室キヤビテイ容積が
設定され、第3図に示されるクローバリーフ状の
主室キヤビテイ6がピストン3の頂上部4の図中
右半分の部分に形成されている。
The volume of the main chamber cavity is determined based on these three requirements, and the cloverleaf-shaped main chamber cavity 6 shown in FIG. 3 is formed in the right half of the top portion 4 of the piston 3 in the figure.

ところが、拡散部容積は小さく主室内の空気利
用率はなお十分とはいえない。
However, the volume of the diffusion section is small and the air utilization rate in the main room is still not sufficient.

そこで、主室内の空気利用率の向上を図り、か
つ圧縮比の上昇をめざして、拡散部がバルブリセ
スとしても利用されるバルブリセス共用型の主室
キヤビテイをピストン頂上部に形成したものが提
案されている。(実願昭57−189037号参照)。
Therefore, in order to improve the air utilization rate in the main chamber and to increase the compression ratio, it has been proposed to form a main chamber cavity at the top of the piston, in which the diffusion section is also used as a valve recess. There is. (See Utility Application No. 189037, 1983).

この主室キヤビテイでは、円形状凹部からなる
一対の拡散部がピストン頂上部に大きく形成さ
れ、拡散部容積が拡大されている。
In this main chamber cavity, a pair of large diffusion portions consisting of circular recesses are formed at the top of the piston, and the volume of the diffusion portion is expanded.

(考案が解決しようとする問題点) 拡散部での良好な燃焼は拡散部内空気の取り入
れを行う火炎の勢いに左右され、勢いが弱められ
ると、初期燃焼を悪化させることになる。ところ
が、逆スキツシユの利用により火炎流れの大部分
はトレンチ部の下流側末端から拡散部外周の円弧
に案内されて流れる主流(旋回流)として流れる
が、その一部はトレンチ部の上流側始端からすぐ
に拡散部外周に案内されて流れる傍流となる。こ
の傍流は同じ拡散部外周に方向づけられた火炎主
流に反対方向から衝突する対向流となるので、そ
の勢いを相殺する傾向にある。このため、火炎と
空気との混合が鈍つて燃焼が悪化し、燃焼初期に
発生しやすいスモーク排出量の増加を招くことが
考えられる。
(Problems to be solved by the invention) Good combustion in the diffusion section depends on the momentum of the flame that takes in air within the diffusion section, and if the momentum is weakened, the initial combustion will be worsened. However, due to the use of reverse skidding, most of the flame flow flows from the downstream end of the trench section as the main flow (swirling flow) guided by the circular arc around the diffusion section, but part of it flows from the upstream starting end of the trench section. It immediately becomes a side stream that flows as it is guided around the outer periphery of the diffusion section. This side flow becomes a counter flow that collides from the opposite direction with the main flame directed toward the outer periphery of the same diffusion section, and thus tends to offset its momentum. For this reason, it is thought that the mixing of the flame and air becomes sluggish and combustion deteriorates, leading to an increase in the amount of smoke emissions that tend to occur in the early stages of combustion.

本考案は、こうした傍流をシリンダ壁に衝突さ
せて減衰消滅させることにより火炎主流への干渉
を回避し、火炎主流の勢いを確保する渦流室式デ
イーゼルエンジンを提供することを目的とする。
An object of the present invention is to provide a swirl chamber type diesel engine that avoids interference with the mainstream flame and secures the momentum of the mainstream flame by colliding the side flow with the cylinder wall and attenuating it.

(問題点を解決するための手段) 本考案は、吸排気バルブの下方に位置して両バ
ルブの径よりも大きな径を有する円形状凹部から
なる一対の拡散部と、両拡散部に連なるとともに
一端が渦流室に連絡される噴口の下面に延びる溝
状のトレンチ部とからなる主室キヤビテイをピス
トン頂上部に形成した渦流室式デイーゼルエンジ
ンを前提とする。
(Means for Solving the Problems) The present invention consists of a pair of diffusion parts that are located below the intake and exhaust valves and have a diameter larger than the diameter of both the valves, and a pair of diffusion parts that are connected to both the diffusion parts. The present invention is based on a swirl chamber type diesel engine in which a main chamber cavity is formed at the top of the piston and includes a groove-shaped trench portion extending on the lower surface of the nozzle port, one end of which is connected to the swirl chamber.

本考案は、トレンチ部の中心軸に直交し拡散部
外周に接する2つの接線間の範囲にあり、かつピ
ストン外周に近接する部分を拡散部底面と同一の
深さに形成する。
In the present invention, a portion located in a range between two tangent lines perpendicular to the central axis of the trench portion and touching the outer periphery of the diffusion portion and close to the outer periphery of the piston is formed to have the same depth as the bottom surface of the diffusion portion.

(作用) このように構成すると、傍流は拡散部外周に接
する接線方向に案内されてシリンダ壁に向かい衝
突して消滅するため、火炎主流に干渉することが
なく、一方、火炎主流は拡散部形状の変更により
旋回性が弱められることからその分広がつた旋回
流として流れるものの、拡散部容積の拡大と相ま
つて拡散部内空気との混合が積極的に促進され良
好な火炎燃焼が確保されることになる。
(Function) With this configuration, the side flow is guided in the tangential direction touching the outer periphery of the diffusion part, collides with the cylinder wall, and disappears, so it does not interfere with the mainstream flame. Although the swirling property is weakened by changing the , the flow becomes a wider swirling flow, but the expansion of the volume of the diffusion section and the active promotion of mixing with the air inside the diffusion section ensure good flame combustion. become.

(実施例) 第1図Aは本考案の一実施例のピストン頂上部
の平面図、第1図Bは第1図AのA−A線断面図
である。
(Embodiment) FIG. 1A is a plan view of the top of a piston according to an embodiment of the present invention, and FIG. 1B is a sectional view taken along line A--A in FIG. 1A.

図中ピストン頂上部4には吸排気バルブ(図示
せず)の下方に位置して両バルブの径よりも大き
な径を有する円形状凹部からなる一対の拡散部7
A,8Aと、拡散部7A,8Aに連なるとともに
一端が渦流室に連絡される噴口(図示せず)の下
面に延びる溝状のトレンチ部10Aが形成され
る。なお、このトレンチ部10Aの溝底面31
は、噴口の下面に延びる側(図中下方)が最も深
く最深部から連結部9Aに向けて浅くなり、連結
部9Aで連結部段差と同一の深さになる傾斜面に
て形成している。
In the figure, on the piston top 4, there is a pair of diffusion parts 7 located below the intake and exhaust valves (not shown) and consisting of a circular concave part having a diameter larger than the diameter of both valves.
A, 8A, a groove-shaped trench portion 10A is formed which extends to the lower surface of a nozzle (not shown) that is connected to the diffusion portions 7A, 8A and has one end connected to the swirl chamber. Note that the groove bottom surface 31 of this trench portion 10A
is formed by an inclined surface that is deepest on the side extending to the lower surface of the nozzle (bottom in the figure) and becomes shallower from the deepest part toward the connecting part 9A, and reaches the same depth as the connecting part step at the connecting part 9A. .

こうして一対の拡散部7A,8Aとトレンチ部
10Aからる主室キヤビテイ6Aが形成される
が、本考案では、トレンチ部10Aの中心軸に直
交し拡散部外周32,33に接する2つの接線
E,E間の範囲にあり、かつピストン外周40に
近接する部分(図中斜線にて示す)を拡散部底面
34,35と同一の深さに形成する。すなわち、
斜線部分は拡大された拡散部36,37として形
成される。なお、バルブリセスとしても利用され
る拡散部7A,8Aの最小深さはバルブリフト、
圧縮比等から設定される。
In this way, the main chamber cavity 6A is formed by the pair of diffusion parts 7A, 8A and the trench part 10A, but in the present invention, two tangents E, A portion located in the range between E and close to the piston outer periphery 40 (indicated by diagonal lines in the figure) is formed to have the same depth as the bottom surfaces 34 and 35 of the diffusion portion. That is,
The shaded portions are formed as enlarged diffusion portions 36 and 37. Note that the minimum depth of the diffusion portions 7A and 8A, which are also used as valve recesses, is the valve lift,
It is set based on the compression ratio, etc.

以上の構成による作用を説明すると、膨張行程
初期に噴口からトレンチ部10Aに噴出する火炎
は逆スキツシユの作用により主としてトレンチ部
10Aの下流側末端(図中上方)から一対の拡散
部外周32,33に案内されて旋回する火炎主流
Cを形成するが、トレンチ部の上流側始端(図中
下方)からすぐに拡散部外周32,33に案内さ
れて流れる傍流Dを形成するものがある。こうし
た傍流Dは拡散部外周32,33からそのまま接
線方向へと案内され、対面するシリンダ壁に衝突
し減衰消滅する。このため、火炎主流はその勢い
が傍流の干渉を受けて鈍るということはない。な
お、比較のため従来例を2点鎖線にて同図に重ね
て示すと、傍流と火炎主流とは同じ拡散部外周に
より反対方向から案内されピストン外周40に近
いほぼ中間点で衝突し、傍流が火炎主流の勢いを
相殺する。しかし、本考案では傍流が火炎主流の
流れ方向には向かうことがないのである。なお、
火炎流れは一方の拡散部についてのみ示している
が、他方についても同様である。
To explain the effect of the above configuration, the flame ejected from the nozzle to the trench portion 10A at the beginning of the expansion stroke mainly flows from the downstream end (upper part in the figure) of the trench portion 10A to the outer periphery of the pair of diffusion portions 32, 33 due to the reverse squishing action. There is a flame main stream C that is guided by the flame main stream C and swirls, but there is also a side stream D that is guided to the outer periphery of the diffusion part 32, 33 and flows immediately from the upstream starting end of the trench part (lower part in the figure). This side flow D is directly guided in the tangential direction from the outer circumferences 32 and 33 of the diffusion portions, collides with the facing cylinder wall, and attenuates and disappears. Therefore, the momentum of the mainstream flame is not slowed down by interference from side streams. For comparison, the conventional example is shown superimposed on the same figure using a two-dot chain line. The side flow and the main flame are guided from opposite directions by the same diffusion section outer periphery and collide at an approximately midpoint near the piston outer periphery 40. offsets the momentum of the mainstream flame. However, in the present invention, the side flow does not flow in the flow direction of the main flame stream. In addition,
Although flame flow is shown for only one diffusion section, the same is true for the other.

一方、火炎主流は拡散部外周の形状が変更にな
つた分だけ旋回性が緩むが、拡大拡散部36,3
7の付加により拡散部容積が拡大するので、火炎
主流の利用空気が多くなり、火炎と空気の混合が
活発に行なわれ燃焼が良好に促進される。このた
め、所定回転数(1200rpm)でのスモーク濃度を
示すと第2図のようになり、広い負荷範囲にわた
つてスモーク発生量を低減するのである。
On the other hand, the swirling property of the main stream of the flame is loosened due to the change in the shape of the outer periphery of the diffusion section, but
Since the volume of the diffusion section is expanded by adding 7, the amount of air used in the mainstream of the flame increases, and the flame and air are actively mixed to promote combustion. For this reason, the smoke density at a predetermined rotation speed (1200 rpm) is shown in Figure 2, and the amount of smoke generated is reduced over a wide load range.

(考案の効果) 本考案によれば、トレンチ部の中心軸に直交し
拡散部外周に接する2つの接線間の範囲にあり、
かつピストン外周に近接する部分を拡散部底面と
同一の深さに形成したので、火炎主流の勢いが傍
流により相殺されることがなく、火炎主流は拡散
部内空気との混合を促進し燃焼初期に発生しやす
いスモーク排出量を低減することができる。
(Effect of the invention) According to the invention, in the range between two tangents that are perpendicular to the central axis of the trench part and in contact with the outer periphery of the diffusion part,
In addition, since the portion close to the outer circumference of the piston is formed at the same depth as the bottom surface of the diffusion section, the momentum of the mainstream flame is not offset by the side flow, and the mainstream flame promotes mixing with the air inside the diffusion section and is heated at the beginning of combustion. It is possible to reduce the amount of smoke emissions that are likely to occur.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図Aは本考案の一実施例のピストン頂上部
の平面図、第1図Bは第1図AのA−A線断面
図、第2図はスモーク濃度の特性図である。第3
図は従来例の燃焼室の縦断面図、第4図は同じく
ピストン頂上部の平面図である。 3……ピストン、4……ピストン頂上部、6A
……主室キヤビテイ、7A,8A……拡散部、7
B,8B……拡散部段差、10A……トレンチ
部、31……溝底面、32,33……拡散部外
周、34,35……拡散部底面、36,37……
拡大拡散部、40……ピストン外周。
FIG. 1A is a plan view of the top of a piston according to an embodiment of the present invention, FIG. 1B is a sectional view taken along line A--A in FIG. 1A, and FIG. 2 is a characteristic diagram of smoke density. Third
The figure is a longitudinal sectional view of a conventional combustion chamber, and FIG. 4 is a plan view of the top of the piston. 3...Piston, 4...Piston top, 6A
...Main room cavity, 7A, 8A...Diffusion section, 7
B, 8B... Diffusion part step, 10A... Trench part, 31... Groove bottom surface, 32, 33... Diffusion part outer periphery, 34, 35... Diffusion part bottom surface, 36, 37...
Enlarged diffusion section, 40...Piston outer periphery.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 吸排気バルブの下方に位置して両バルブの径よ
りも大きな径を有する円形状凹部からなる一対の
拡散部と、両拡散部に連なるとともに一端が渦流
室に連絡される噴口の下面に延びる溝状のトレン
チ部とからなる主室キヤビテイをピストン頂上部
に形成した渦流室式デイーゼルエンジンにおい
て、トレンチ部の中心軸に直交し拡散部外周に接
する2つの接線間の範囲にあり、かつピストン外
周に近接する部分を拡散部底面と同一の深さに形
成したことを特徴とする渦流室式デイーゼルエン
ジン。
A pair of diffusion parts located below the intake and exhaust valves and consisting of circular recesses having a diameter larger than the diameter of both valves, and a groove extending on the lower surface of the nozzle that is connected to both diffusion parts and has one end connected to the swirl chamber. In a swirl chamber type diesel engine in which a main chamber cavity consisting of a shaped trench portion is formed at the top of the piston, the main chamber cavity is located in the range between two tangents perpendicular to the central axis of the trench portion and in contact with the outer periphery of the diffusion portion, and is located on the outer periphery of the piston. A swirl chamber type diesel engine characterized in that the adjacent portion is formed at the same depth as the bottom surface of the diffusion section.
JP10231284U 1984-06-12 1984-07-06 Swirl chamber diesel engine Granted JPS6117419U (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP10231284U JPS6117419U (en) 1984-07-06 1984-07-06 Swirl chamber diesel engine
DE19853520775 DE3520775A1 (en) 1984-06-12 1985-06-10 Diesel engine with a swirl chamber and a flame distribution recess molded into the piston crown
GB08514801A GB2160262B (en) 1984-06-12 1985-06-11 Diesel engine having a swirl pre-combustion chamber and a shaped flame dispersing recess in piston crown
US06/743,673 US4662330A (en) 1984-06-12 1985-06-11 Diesel engine having swirl chamber and shaped flame dispersing recess in piston crown

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10231284U JPS6117419U (en) 1984-07-06 1984-07-06 Swirl chamber diesel engine

Publications (2)

Publication Number Publication Date
JPS6117419U JPS6117419U (en) 1986-01-31
JPH0115860Y2 true JPH0115860Y2 (en) 1989-05-11

Family

ID=30661712

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10231284U Granted JPS6117419U (en) 1984-06-12 1984-07-06 Swirl chamber diesel engine

Country Status (1)

Country Link
JP (1) JPS6117419U (en)

Also Published As

Publication number Publication date
JPS6117419U (en) 1986-01-31

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